| 1. |  A Century on Diameter Measurement Techniques in Cylindrical Structures..
[País não identificado] |
| 2. | A laboratory infrared model of astrophysical pyrimidines.
[Não foi possível obter dados do DOI] |
| 3. | A novel 3D fibre-reinforcement architecture for high performance natural fibre reinforced composite adhesively bonded joints.
[Não foi possível obter dados do DOI] |
| 4. | A study on the effect of nanoclay addition on the erosion wear characteristics of S-glass/sisal reinforced hybrid polymer composites.
[País não identificado] |
| 5. | Acoustic impedance measurement method using spherical waves.
[País não identificado] |
| 6. | Analyzing the LMS Weight Error Covariance Matrix: An Exact Expectation Approach.
[País não identificado] |
| 7. | ARCog-NET: An Aerial Robot Cognitive Network Architecture for Swarm Applications Development.
[País não identificado] |
| 8. | Assessment of Shear Fracture Energy in Hybrid Composites with Natural and Synthetic Fibers.
[País não identificado] |
| 9. | Autonomous UAV Exploration and Mapping in Uncharted Terrain through Boundary-Driven Strategy.
[País não identificado] |
| 10. | CMS iRPC FEB development and validation.
[País não identificado] |
| 11. | Conjugate gradient-based active noise cancellation.
[Não foi possível obter dados do DOI] |
| 12. | Dimensional Evaluation of Additively Manufactured Parts for Autonomous Vehicles.
Portugal, Brazil. |
| 13. | Effect of hybridization and composite architecture symmetry in the bonded joint performance of jute/carbon fibre-reinforced composites.
[País não identificado] |
| 14. | Enhanced photovoltaic efficiency in dye-sensitized solar cells with natural co-sensitizers from Annona squamosa, Malus domestica and Musa fruits.
[País não identificado] |
| 15. | Enhancing the Efficiency of Solar Cells Based on TiO2 and ZnO Photoanodes Through Copper Oxide: A Comparative Study Using Vitis labrusca Extract and N3 Ruthenium Dye.
[País não identificado] |
| 16. | Evaluation of durability of 3D-printed multi-material parts for potential applications in structures exposed to marine environments.
[País não identificado] |
| 17. | F.
[País não identificado] |
| 18. | Flexible supercapacitors based on carbon fiber cloth coated copper hexacyanoferrate nanoparticles as positive electrode material.
[País não identificado] |
| 19. | Generation and practical controlling of adaptative structured photorefractive moiré patterns for optical metrology applications.
[Não foi possível obter dados do DOI] |
| 20. | Heat and mass transfer with chemical kinetics in alcoholic fermentation of multiple sugars: Lumped formulation and dimensional analysis.
[País não identificado] |
| 21. | Heavy ion radiolysis of the chiral terpene α-pinene.
[Não foi possível obter dados do DOI] |
| 22. | Heterogeneous Multi-Robot Collaboration for Coverage Path Planning in Partially Known Dynamic Environments.
[País não identificado] |
| 23. | Higher-order moments of the elliptic flow distribution in PbPb collisions at $$ sqrt{s_{ extrm{NN}}} $$ = 5.02 TeV.
[País não identificado] |
| 24. | Impact of carbon dioxide-assisted activation on Millettia pinnata shell-derived porous activated carbon for enhanced performance in symmetric supercapacitors.
[País não identificado] |
| 25. | Improved resistive plate chambers for HL-LHC upgrade of CMS.
[País não identificado] |
| 26. | Influence of Biomass-derived Porous Activated Carbon on Polyaniline as Electrode Material for Supercapacitor Applications.
[País não identificado] |
| 27. | Influence of sintering temperature on graphitic carbon nitride nanosheets grafted binary metal oxide for high performance asymmetric supercapacitors.
[País não identificado] |
| 28. | Influence of various solvents in extraction of natural pigments from Annona Atemoya and Physalis Peruviana as photosensitizers for dye-sensitized solar cells.
[País não identificado] |
| 29. | LoRaCELL-Driven IoT Smart Lighting Systems: Sustainability in Urban Infrastructure.
[País não identificado] |
| 30. | Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 31. | Measurement of the production cross section for a W boson in association with a charm quark in proton-proton collisions at $$sqrt{s} = 13,hbox {TeV}$$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Chile, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 32. | Measurement of the τ lepton polarization in Z boson decays in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 33. | Mechanical characterization of jute/carbon hybrid epoxy composites.
[Não foi possível obter dados do DOI] |
| 34. | Mechanical characterization of short Curauá/glass fiber-reinforced interlaminar hybrid composite adhesive joints.
[Não foi possível obter dados do DOI] |
| 35. | Modifications of astrophysical ices induced by cosmic rays. I. Water, carbon monoxide, and methanol mixtures.
Brazil. |
| 36. | Optoelectronic oscillator using visible LEDs and plastic optical fibers.
[País não identificado] |
| 37. | Physical activation assisted porous activated carbon from Strychnos Potatorum shells for high-performance symmetric supercapacitors.
[País não identificado] |
| 38. | Plastic optical fibers as optical illuminators for digital holography and structured fringe patterns generation.
[País não identificado] |
| 39. | Preparation of Acetylenediol (HOCCOH) and Glyoxal (HCOCHO) in Interstellar Analog Ices of Carbon Monoxide and Water.
[País não identificado] |
| 40. | Pressure correction study for the CMS iRPC detector.
[País não identificado] |
| 41. | Processing a new diamond composite by high pressure and high temperature with improved thermostability using Mo as a binder.
[País não identificado] |
| 42. | Pyrolysis-assisted synthesis of two-dimensional graphitic carbon nitride nanosheets embedded with transition metal oxide (Ni or Fe) for high-performance asymmetric supercapacitors.
[País não identificado] |
| 43. | Research and development of time resolution and time reference adjustment for CMS improved resistive plate chambers (iRPCs).
[País não identificado] |
| 44. | Review of Uncertainty Sources in Optical Current Sensors Used in Power Systems.
[País não identificado] |
| 45. | Search for dark matter particles in W+W− events with transverse momentum imbalance in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 46. | Search for long-lived heavy neutral leptons with lepton flavour conserving or violating decays to a jet and a charged lepton.
[País não identificado] |
| 47. | Sparsity-aware distributed adaptive filtering with robustness against impulsive noise and low SNR.
[País não identificado] |
| 48. | Stability Analysis of the Bias Compensated LMS Algorithm.
[País não identificado] |
| 49. | Stochastic Modelling of the Set-Membership-sign-NLMS Algorithm.
[País não identificado] |
| 50. | Study of charm hadronization with prompt $$ {Lambda}_{ extrm{c}}^{+} $$ baryons in proton-proton and lead-lead collisions at $$ sqrt{s_{ extrm{NN}}} $$ = 5.02 TeV.
[País não identificado] |
| 51. | The Impact of Fe²+ and Fe³+ Segregation on the Structural and Magnetic Properties of ZnO/Fe Multilayers Deposited via Sputtering: A Study Using EELS and EDS.
[País não identificado] |
| 52. | Tracking Analysis of the $$ell _0$$-LMS Algorithm.
[País não identificado] |
| 53. | Transient Analysis of a Selective Partial-Update LMS Algorithm.
[País não identificado] |
| 54. | Two-particle Bose-Einstein correlations and their Lévy parameters in PbPb collisions at s N N = 5.02 TeV.
[Não foi possível obter dados do DOI] |
| 55. | Upwelling-driven variation of sound speed profile in a Brazilian bay monitored by a coastal acquisition system.
Brazil. |
| 56. | Use of BODIPY and BORANIL Dyes to Improve Solar Conversion in the Fabrication of Organic Photovoltaic Cells Through the Co-Sensitization Method.
[País não identificado] |
| 1. | A Multi-Plasmonic Approach for Simultaneous Measurements based on a D-Shaped Photonic Crystal Fiber Sensor: from Temperature to Optical Dispersion.
[País não identificado] |
| 2. | A novel heuristic for the analysis of block sign LMS algorithm.
[Não foi possível obter dados do DOI] |
| 3. | A search for decays of the Higgs boson to invisible particles in events with a top-antitop quark pair or a vector boson in proton-proton collisions at $$sqrt{s} = 13, ext {Te}hspace{-.08em} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Chile, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 4. | A search for new physics in central exclusive production using the missing mass technique with the CMS detector and the CMS-TOTEM precision proton spectrometer. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Chile, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 5. | Adaptive Path Planning for Fusing Rapidly Exploring Random Trees and Deep Reinforcement Learning in an Agriculture Dynamic Environment UAVs.
[País não identificado] |
| 6. | Aging studies for the CMS improved Resistive Plate Chambers.
[País não identificado] |
| 7. | Analysis of single-channel SPR-SMS refractive index and temperature sensor.
[País não identificado] |
| 8. | Attitude Control of Ornithopter Wing by Using a MIMO Active Disturbance Rejection Strategy.
[País não identificado] |
| 9. | Azimuthal anisotropy of dijet events in PbPb collisions at $$ sqrt{s_{ extrm{NN}}} $$ = 5.02 TeV.
[País não identificado] |
| 10. | Azimuthal correlations in Z +jets events in proton-proton collisions at $$sqrt{s} = 13, ext {Te}hspace{-.08em} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 11. | CMS pythia 8 colour reconnection tunes based on underlying-event data. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 12. | Combination of inclusive top-quark pair production cross-section measurements using ATLAS and CMS data at $$ sqrt{s} $$ = 7 and 8 TeV.
[País não identificado] |
| 13. | Conjunto de Boas Práticas Baseadas na Avaliação de Risco para a Padronização Nacional em Ambientes Computacionais.
[Não foi possível obter dados do DOI] |
| 14. | Construction and characterization of organic photovoltaic cells sensitized by Chrysanthemum based natural dye.
[País não identificado] |
| 15. | Cooperative Heterogeneous Robots for Autonomous Insects Trap Monitoring System in a Precision Agriculture Scenario.
[País não identificado] |
| 16. | Determination of carbohydrates in brewer's wort by capillary electrophoresis with indirect UV detection.
[País não identificado] |
| 17. | Development of MOF Based Recyclable Photocatalyst for the Removal of Different Organic Dye Pollutants.
[País não identificado] |
| 18. | Diesel Engine Fault Prediction Using Artificial Intelligence Regression Methods.
[País não identificado] |
| 19. | Effect of Multi-Walled Carbon Nanotubes on the Mechanical and Thermal Properties of Curauá Natural-Fiber-Reinforced Composites.
[País não identificado] |
| 20. | Effect of water on the mechanical and thermal properties of natural fibre reinforced hybrid composites.
[Não foi possível obter dados do DOI] |
| 21. | Evaluation of Solar Conversion Efficiency in Dye-sensitized Solar Cells Using Natural Dyes Extracted from Alpinia purpurata and Alstroemeria Flower Petals as Novel Photosensitizers.
[País não identificado] |
| 22. | Evolutionary Intelligent System for Proactive Management of Smart Oil Fields.
[País não identificado] |
| 23. | Fiber Bragg grating thermometry application to measure flow: laminar and turbulent regimes.
[País não identificado] |
| 24. | First measurement of the forward rapidity gap distribution in p Pb collisions at s NN l.
[Não foi possível obter dados do DOI] |
| 25. | First measurement of the top quark pair production cross section in proton-proton collisions at $$ sqrt{s} $$ = 13.6 TeV.
[País não identificado] |
| 26. | Formation of N-O-H bearing species in HNO 3 and H 2 O icy samples by heavy-ion irradiation: an infrared spectroscopic study.
[País não identificado] |
| 27. | Graphite oxide synthetized by pulsed laser ablation technique used as an antifouling coating to inhibit CaCO3 scale on stainless steel surfaces.
[Não foi possível obter dados do DOI] |
| 28. | High-performance asymmetric supercapacitors utilizing manganese oxide nanoparticles grafted graphitic carbon nitride nanosheets as the cathode and hypercross-linked polymer derived activated carbon as the anode.
[País não identificado] |
| 29. | High-performance flexible supercapacitors based on potassium nickel( ) hexacyanoferrates( ) nanoparticles on carbon cloth as an electrode material.
India, Brazil. |
| 30. | Improved Proportionate Constrained Normalized Least Mean Square for Adaptive Beamforming.
[País não identificado] |
| 31. | Improved variational mode decomposition for combined imbalance-and-misalignment fault recognition and severity quantification.
[País não identificado] |
| 32. | Infrared Spectral Signatures of Nucleobases in Interstellar Ices I: Purines.
[País não identificado] |
| 33. | Latest results of Longevity studies on the present CMS RPC system for HL-LHC phase.
[País não identificado] |
| 34. | Machine Learning based tool for CMS RPC currents quality monitoring.
[País não identificado] |
| 35. | Measurement of inclusive and differential cross sections for single top quark production in association with a W boson in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 36. | Measurement of the differential $$hbox {t}overline{hbox {t}}$$ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Chile, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 37. | Measurement of the Higgs boson inclusive and differential fiducial production cross sections in the diphoton decay channel with pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 38. | Measurement of the mass dependence of the transverse momentum of lepton pairs in Drell-Yan production in proton-proton collisions at $$sqrt{s} = 13, ext {Tehspace{-.08em}V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Qatar, Austria, Brazil, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 39. | Measurement of the top quark mass using a profile likelihood approach with the lepton+jets final states in proton-proton collisions at $$sqrt{s}=13, ext {Te}hspace{-.08em} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Chile, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 40. | Measurement of the top quark pole mass using $$ extrm{t}overline{ extrm{t}} $$+jet events in the dilepton final state in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 41. | Measurements of jet multiplicity and jet transverse momentum in multijet events in proton-proton collisions at $${sqrt{s}=13, ext {TeV}}$$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Qatar, Austria, Brazil, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 42. | Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $$ sqrt{s_{ extrm{NN}}} $$ = 5.02 TeV.
[País não identificado] |
| 43. | Natural Fibre Composites and Their Mechanical Behaviour.
[País não identificado] |
| 44. | Neglected frequencies analysis on switching operations in extra-high voltage electrical power substations.
[País não identificado] |
| 45. | New slow control emulator for the CMS phase-2 upgrade RPC link system.
[País não identificado] |
| 46. | Nickel Nanoparticles Supported on Carbon Cloth via Pulsed Laser Deposition as an Effective Catalyst for Urea Electro-oxidation Reaction.
[País não identificado] |
| 47. | Numerical analysis of repaired wall loss defect pipelines for optimum composite wrap thickness.
France, Italy, India, Brazil. |
| 48. | Observation of triple J/ψ meson production in proton-proton collisions.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 49. | On the design of KLT-based maximally incoherent deterministic sensing matrices for compressive sensing applied to wireless sensor networks data.
[País não identificado] |
| 50. | Performance enhancement of adhesive joints of additive manufactured parts by using different types of fibre reinforcements.
[País não identificado] |
| 51. | Recent Advances in Adhesive Bonding of 3D-Printed Parts and Methods to Increase their Mechanical Performance.
Portugal, Brazil. |
| 52. | Recent Advances in MXenes Based Composites as Photocatalysts: Synthesis, Properties, and Photocatalytic Removal of Organic Contaminants from Wastewater.
[Não foi possível obter dados do DOI] |
| 53. | RPC background studies at CMS experiment.
[País não identificado] |
| 54. | RPC based tracking system at CERN GIF++ facility.
[País não identificado] |
| 55. | Search for a charged Higgs boson decaying into a heavy neutral Higgs boson and a W boson in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 56. | Search for a high-mass dimuon resonance produced in association with b quark jets at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 57. | Search for a vector-like quark T- → tH via the diphoton decay mode of the Higgs boson in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 58. | Search for CP violating top quark couplings in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 59. | Search for CP violation in t$$ overline{ extrm{t}} $$H and tH production in multilepton channels in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 60. | Search for heavy resonances and quantum black holes in eμ, eτ, and μτ final states in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 61. | Search for Higgs boson decays to a Z boson and a photon in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 62. | Search for high-mass exclusive γγ → WW and γγ → ZZ production in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 63. | Search for light Higgs bosons from supersymmetric cascade decays in $$ ext {pp}$$ collisions at $$sqrt{s}=13, extrm{TeV}$$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 64. | Search for long-lived particles decaying to a pair of muons in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 65. | Search for long-lived particles using out-of-time trackless jets in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 66. | Search for new physics in multijet events with at least one photon and large missing transverse momentum in proton-proton collisions at 13 TeV.
[País não identificado] |
| 67. | Search for nonresonant Higgs boson pair production in the four leptons plus twob jets final state in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 68. | Search for pair production of vector-like quarks in leptonic final states in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 69. | Search for physics beyond the standard model in top quark production with additional leptons in the context of effective field theory.
[País não identificado] |
| 70. | Search for resonant and nonresonant production of pairs of dijet resonances in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 71. | Search for supersymmetry in final states with a single electron or muon using angular correlations and heavy-object identification in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 72. | Search for top squarks in the four-body decay mode with single lepton final states in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 73. | Searches for additional Higgs bosons and for vector leptoquarks in ττ final states in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 74. | Sliding Mode Controller Applied to Autonomous UAV Operation in Marine Small Cargo Transport.
[País não identificado] |
| 75. | Statistical modeling of atmospheric turbulence based on a low-cost experimental setup for measuring 𝐶2𝑛 over water.
[País não identificado] |
| 76. | Strange hadron collectivity in pPb and PbPb collisions.
[País não identificado] |
| 77. | The CMS RPC system readiness for LHC Run-3 data taking.
[País não identificado] |
| 78. | UAV Power Line Tracking Control Based on a Type-2 Fuzzy-PID Approach.
[País não identificado] |
| 79. | Variant ADRC Design Paradigm for Controlling Uncertain Dynamical Systems.
[País não identificado] |
| 1. | A fuzzy approach to LPFG-based optical sensor processing and interrogation.
[País não identificado] |
| 2. | A new calibration method for charm jet identification validated with proton-proton collision events at √s = 13 TeV.
[País não identificado] |
| 3. | A novel sEMG data augmentation based on WGAN-GP.
[Não foi possível obter dados do DOI] |
| 4. | A portrait of the Higgs boson by the CMS experiment ten years after the discovery.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Bulgaria, Romania, Qatar, Austria, Brazil, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 5. | A Review of Recent Advances in Hybrid Natural Fiber Reinforced Polymer Composites.
Brazil. |
| 6. | A simple optical sensor based on Multimodal Interference superimposed on additive manufacturing for diameter measurement.
[País não identificado] |
| 7. | An edge-fog architecture for distributed 3D reconstruction.
[País não identificado] |
| 8. | An Edge-Fog Architecture for Distributed 3D Reconstruction and Remote Monitoring of a Power Plant Site in the Context of 5G.
[País não identificado] |
| 9. | Analysis of tennis games using TrackNet-based neural network and applying morphological operations to the match videos.
[País não identificado] |
| 10. | Analysis of the CP structure of the Yukawa coupling between the Higgs boson and τ leptons in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 11. | Analysis of the Least Mean Squares Algorithm with Reusing Coefficient Vector.
[País não identificado] |
| 12. | Automatic detection of Aedes aegypti breeding grounds based on deep networks with spatio-temporal consistency.
[País não identificado] |
| 13. | Bimetallic MOF derived ZnCo2O4 nanocages as a novel class of high performance photocatalyst for the removal of organic pollutants.
[País não identificado] |
| 14. | Chemical reactions in H2O:CO interstellar ice analogs promoted by energetic heavy ion irradiation.
[Não foi possível obter dados do DOI] |
| 15. | Comprehensive Direct Georeferencing of Aerial Images for Unmanned Aerial Systems Applications.
[País não identificado] |
| 16. | Computer Vision Based Path Following for Autonomous Unammed Aerial Systems in Unburied Pipeline Onshore Inspection.
[País não identificado] |
| 17. | Development and Mechanical Characterization of Short Curauá Fiber-Reinforced PLA Composites Made via Fused Deposition Modeling.
[País não identificado] |
| 18. | Dynamic Path Planning Based on Neural Networks for Aerial Inspection.
[País não identificado] |
| 19. | earch for a W- boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $$ sqrt{mathrm{s}} $$ = 13 TeV.
[País não identificado] |
| 20. | Effect of bandgap energies by various color petals of Gerbera jamesonii flower dyes as a photosensitizer on enhancing the efficiency of dye-sensitized solar cells.
[País não identificado] |
| 21. | Effect of ultraviolet radiation and water spraying on the mechanical properties of multi-walled carbon nanotubes reinforced natural fiber and hybrid composites.
[Não foi possível obter dados do DOI] |
| 22. | EKF-Based Vision Assisted Target Tracking and Approaching for Autonomous UAV in Offshore Mooring Tasks.
[País não identificado] |
| 23. | Entropy loading for capacity maximization of RGB-based visible light communications.
[País não identificado] |
| 24. | Erratum to: Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 25. | Evidence for X(3872) in Pb-Pb Collisions and Studies of its Prompt Production at s N N = 5.02 - - TeV.
[Não foi possível obter dados do DOI] |
| 26. | Experimentation and Simulation with Autonomous Coverage Path Planning for UAVs.
[País não identificado] |
| 27. | Fabrication of High-Performance Asymmetric Supercapacitor Consists of Nickel Oxide and Activated Carbon (NiO//AC).
[País não identificado] |
| 28. | Facile synthesis of transition metal (M=Cu, Co) oxide grafted graphitic carbon nitride nanosheets for high performance asymmetric supercapacitors.
[País não identificado] |
| 29. | First Search for Exclusive Diphoton Production at High Mass with Tagged Protons in Proton-Proton Collisions at.
[Não foi possível obter dados do DOI] |
| 30. | Fragmentation of jets containing a prompt J/ψ meson in PbPb and pp collisions at s NN.
[País não identificado] |
| 31. | Fuzzy Gain-Scheduling PID for UAV Position and Altitude Controllers.
[País não identificado] |
| 32. | Hybrid data augmentation method for combined failure recognition in rotating machines. JOURNAL OF INTELLIGENT MANUFACTURING (DORDRECHT.
[País não identificado] |
| 33. | Hybrid methodology based on computational vision and sensor fusion for assisting autonomous UAV on offshore messenger cable transfer operation.
Brazil. |
| 34. | IMPROVEMENTS in the thermal, mechanical and electrical conductivity properties of a structural adhesive: A preliminary study.
[País não identificado] |
| 35. | Inclusive and differential cross section measurements of single top quark production in association with a Z boson in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 36. | Inclusive nonresonant multilepton probes of new phenomena at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 37. | Infrared Spectroscopic Study on Swift-Ion Irradiation of Solid N 2 O-H 2 O Samples: Synthesis of N-O Bearing Species in Astrophysical Ices.
[Não foi possível obter dados do DOI] |
| 38. | Intelligent Detection of Arrhythmia Episodes in Dialysis Patients.
[País não identificado] |
| 39. | Joint Optical Wireless Communication and Localization using OFDM.
[País não identificado] |
| 40. | Measurement and QCD analysis of double-differential inclusive jet cross sections in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 41. | Measurement of differential cross sections in proton-proton collisions at and effective field theory constraints.
[Não foi possível obter dados do DOI] |
| 42. | Measurement of double-parton scattering in inclusive production of four jets with low transverse momentum in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 43. | Measurement of the Drell-Yan forward-backward asymmetry at high dilepton masses in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 44. | Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Romania, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 45. | Measurement of the inclusive $$ mathrm{t}overline{mathrm{t}} $$ production cross section in proton-proton collisions at $$ sqrt{s} $$ = 5.02 TeV.
[País não identificado] |
| 46. | Measurement of the Inclusive and Differential Higgs Boson Production Cross Sections in the Decay Mode to a Pair of τ Leptons in p p Collisions at s.
[Não foi possível obter dados do DOI] |
| 47. | Measurement of the inclusive and differential t$$ overline{t} $$γ cross sections in the dilepton channel and effective field theory interpretation in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 48. | Measurement of the inclusive and differential WZ production cross sections, polarization angles, and triple gauge couplings in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 49. | Measurement of the production cross section for Z + b jets in proton-proton collisions at s = 1.
[Não foi possível obter dados do DOI] |
| 50. | Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $$sqrt{s}=8, ext {TeV} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 51. | Memetic algorithm applied to topology control optimization of a wireless sensor network.
[País não identificado] |
| 52. | Methods to increase the mechanical performance of composite adhesive joints: An overview with focus on joints with natural fibre composite adherends.
[Não foi possível obter dados do DOI] |
| 53. | Observation of B s 0 mesons and measurement of the B.
[País não identificado] |
| 54. | Observation of the B c + Meson in Pb-Pb and p p.
[Não foi possível obter dados do DOI] |
| 55. | On the synthesis of N-O bearing species in astrophysical ices - an infrared spectroscopic study using heavy-ion irradiation of solid N2:CO samples.
[Não foi possível obter dados do DOI] |
| 56. | Optical Strain Gauge Prototype Based on a High Sensitivity Balloon-like Interferometer and Additive Manufacturing.
[País não identificado] |
| 57. | Performance analysis of humidity high-sensitivity tapered optical fiber sensor.
[País não identificado] |
| 58. | Performance evaluation of DSSCs using naturally extracted dyes from petals of Lantana repens and Solidago canadensis flowers as light-harvesting units.
[País não identificado] |
| 59. | Precision measurement of the W boson decay branching fractions in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 60. | Probing Charm Quark Dynamics via Multiparticle Correlations in Pb-Pb Collisions at s NN = 5.02 - l.
[Não foi possível obter dados do DOI] |
| 61. | R D of back-end electronics for improved resistive plate chambers for the phase 2 upgrade of the CMS end-cap muon system.
[País não identificado] |
| 62. | Recent Advancements of Polyaniline/Metal Organic Framework (PANI/MOF) Composite Electrodes for Supercapacitor Applications: A Critical Review.
[País não identificado] |
| 63. | RFBG Thermal Aging Evaluation Above Regeneration Temperature.
[País não identificado] |
| 64. | Search for a heavy resonance decaying into a top quark and a W boson in the lepton+jets final state at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 65. | Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 66. | Search for charged-lepton flavor violation in top quark production and decay in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 67. | Search for electroweak production of charginos and neutralinos in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 68. | Search for flavor-changing neutral current interactions of the top quark and the Higgs boson decaying to a bottom quark-antiquark pair at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 69. | Search for heavy resonances decaying to a pair of Lorentz-boosted Higgs bosons in final states with leptons and a bottom quark pair at $$ sqrt{s} $$= 13 TeV.
[País não identificado] |
| 70. | Search for heavy resonances decaying to in proton-proton collisions at.
[Não foi possível obter dados do DOI] |
| 71. | Search for heavy resonances decaying to W W , W Z , or.
[Não foi possível obter dados do DOI] |
| 72. | Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 73. | Search for higgsinos decaying to two Higgs bosons and missing transverse momentum in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 74. | Search for high-mass resonances decaying to a jet and a Lorentz-boosted resonance in proton-proton collisions at.
[País não identificado] |
| 75. | Search for invisible decays of the Higgs boson produced via vector boson fusion in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 76. | Search for long-lived heavy neutral leptons with displaced vertices in proton-proton collisions at $$ sqrt{mathrm{s}} $$ =13 TeV.
[País não identificado] |
| 77. | Search for long-lived particles decaying into muon pairs in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV collected with a dedicated high-rate data stream.
[País não identificado] |
| 78. | Search for long-lived particles decaying to leptons with large impact parameter in proton-proton collisions at $$sqrt{s} = 13, ext {Te} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 79. | Search for long-lived particles produced in association with a Z boson in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 80. | Search for low-mass dilepton resonances in Higgs boson decays to four-lepton final states in proton-proton collisions at $$sqrt{s}=13, ext {TeV} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 81. | Search for new physics in the lepton plus missing transverse momentum final state in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 82. | Search for Resonances Decaying to Three Bosons in Proton-Proton Collisions at.
[Não foi possível obter dados do DOI] |
| 83. | Search for resonances decaying to three bosons in the hadronic final state in proton-proton collisions at.
[Não foi possível obter dados do DOI] |
| 84. | Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV.
[País não identificado] |
| 85. | Search for single production of a vector-like T quark decaying to a top quark and a Z boson in the final state with jets and missing transverse momentum at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 86. | Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 87. | Search for Wγ resonances in proton-proton collisions at s = 13 TeV using hadronic decays of Lorentz-boosted W bosons.
[País não identificado] |
| 88. | Semantic Segmentation for Automatic Extraction of Linear Geological Structures from Uav Imagery - Saelgs.
[País não identificado] |
| 89. | SHI irradiation of water ice at different temperatures: H2O2 and O3 synthesis and sputtering yield.
[Não foi possível obter dados do DOI] |
| 90. | Simulation Analysis of Signal Conditioning Circuits for Plants’ Electrical Signals.
[País não identificado] |
| 91. | sp-hybridized carbon atoms formed by low-energy collisions in carbon nanofoams produced by pulsed laser deposition.
[País não identificado] |
| 92. | Strengthening of additive manufactured parts by using different type of fibre reinforcements.
[País não identificado] |
| 93. | Study of dijet events with large rapidity separation in proton-proton collisions at $$ sqrt{s} $$ = 2.76 TeV.
[País não identificado] |
| 94. | Study of quark and gluon jet substructure in Z+jet and dijet events from pp collisions.
[País não identificado] |
| 95. | Tunable plasmonic resonance sensor using a metamaterial film in a D-shaped photonic crystal fiber for refractive index measurements.
[País não identificado] |
| 96. | Unmanned Aerial Vehicles Motion Control with Fuzzy Tuning of Cascaded-PID Gains.
[País não identificado] |
| 97. | Upgrade of the CMS resistive plate chambers for the high luminosity LHC.
[País não identificado] |
| 98. | Using Z Boson Events to Study Parton-Medium Interactions in Pb-Pb Collisions.
[Não foi possível obter dados do DOI] |
| 99. | Visual-based Assistive Method for UAV Power Line Inspection and Landing.
[País não identificado] |
| 1. | A Family of Adaptive Volterra Filters Based on Maximum Correntropy Criterion for Improved Active Control of Impulsive Noise.
[País não identificado] |
| 2. | A Framework for Coverage Path Planning Optimization Based on Point Cloud for Structural Inspection.
[País não identificado] |
| 3. | A Gait Energy Image-Based System for Brazilian Sign Language Recognition.
[País não identificado] |
| 4. | A new cohesive element to model environmental degradation of adhesive joints in the rail industry.
[Não foi possível obter dados do DOI] |
| 5. | A non-uniform NSAF-SF adaptive algorithm.
[Não foi possível obter dados do DOI] |
| 6. | A Photoionization Mass Spectrometry Investigation into Complex Organic Molecules Formed in Interstellar Analog Ices of Carbon Monoxide and Water Exposed to Ionizing Radiation.
[País não identificado] |
| 7. | A Point-to-Multi-Point Tracking System for FSO Communication.
[País não identificado] |
| 8. | A probabilistic approach to assess the impact of wind power generation in transmission network expansion planning.
[País não identificado] |
| 9. | A Review of Structural Adhesive Joints in Hybrid Joining Processes.
[País não identificado] |
| 10. | A Review on the Thermal Characterisation of Natural and Hybrid Fiber Composites.
Brazil. |
| 11. | A Rhythmic Activation Mechanism for Soft Multi-legged Robots.
[País não identificado] |
| 12. | A Simple Optical Sensor Based on an In-line Mach-Zehnder Interferometer for Monitoring Single- and Two-phase Flows in Pipelines.
[País não identificado] |
| 13. | Adhesively bonded joints of jute, glass and hybrid jute/glass fibre-reinforced polymer composites for automotive industry.
[País não identificado] |
| 14. | All-fiber sensors for salinity and temperature simultaneous measurement.
[País não identificado] |
| 15. | An analytical model for permittivity measurement of liquid dielectrics with a tubular sample holder.
[Não foi possível obter dados do DOI] |
| 16. | An opto-electronic oscillator based on Fabry-Perot stabilized dual-wavelength fiber ring laser.
[Não foi possível obter dados do DOI] |
| 17. | Analysis of a tunable CMOS-compatible multilayer waveguide structure for dual polarizer-modulator operation.
[País não identificado] |
| 18. | Angular analysis of the decay B+ → K∗(892)+μ+μ− in proton-proton collisions at $$ sqrt{mathrm{s}} $$ = 8 TeV.
[País não identificado] |
| 19. | ARCog: An Aerial Robotics Cognitive Architecture.
Canada, Spain, Brazil. |
| 20. | Assessment of the Presence of PAHs and Hydrogenated PAHs in the Young Stellar Object Mon R2 and the Taurus Dense Cloud Toward Elias 16.
[País não identificado] |
| 21. | Biomass-derived porous activated carbon nanofibers from Sapindus trifoliatus nut shells for high-performance symmetric supercapacitor applications.
[País não identificado] |
| 22. | Blind and Semi-blind Anechoic Mixing System Identification Using Multichannel Matching Pursuit.
[País não identificado] |
| 23. | CMS phase-II upgrade of the RPC Link System.
[País não identificado] |
| 24. | CMS RPC background - studies and measurements.
[País não identificado] |
| 25. | Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $$sqrt{s} = 13, ext {Te} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 26. | Comparative analysis of the mechanical and thermal properties of polyester and epoxy natural fibre-reinforced hybrid composites.
[Não foi possível obter dados do DOI] |
| 27. | Constrained Least Mean Square Algorithm with Coefficient Reusing.
[País não identificado] |
| 28. | Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state.
[Não foi possível obter dados do DOI] |
| 29. | Constraints on the Initial State of Pb-Pb Collisions via Measurements of Z -Boson Yields and Azimuthal Anisotropy at s N N.
[Não foi possível obter dados do DOI] |
| 30. | Correlations of azimuthal anisotropy Fourier harmonics with subevent cumulants in collisions at.
[Não foi possível obter dados do DOI] |
| 31. | Decomposition of the CO stretching vibration band of laboratory H2O-CO ices irradiated by heavy ions.
[Não foi possível obter dados do DOI] |
| 32. | Development and validation of HERWIG7 tunes from CMS underlying-event measurements. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 33. | Development of a Solar Panel Control Strategy for Tracking Maximum Power Generation.
[Não foi possível obter dados do DOI] |
| 34. | Diagnostic and severity analysis of combined failures composed by imbalance and misalignment in rotating machines.
[País não identificado] |
| 35. | Dynamic Optimization and Heuristics Based Online Coverage Path Planning in 3D Environment for UAVs.
[País não identificado] |
| 36. | Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC.
[País não identificado] |
| 37. | Enhancement of Cu Nanoparticles Dispersion in Nanolubricants by Magnetron Sputtering Deposition and Its Influence on the Tribological Behavior.
Brazil. |
| 38. | Erratum to: Measurement of single-diffractive dijet production in proton-proton collisions at $$sqrt{s} = 8, ext {Te} ext {V} $$ with the CMS and TOTEM experiments.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 39. | Erratum to: Search for dark matter produced in association with a leptonically decaying $${mathrm{Z}} $$ boson in proton-proton collisions at $$sqrt{s}=13, ext {TeV} $$.
South Korea, Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 40. | Etched Fiber Bragg Grating Probe using a Regular CNC Machine and a 3D Printer.
[País não identificado] |
| 41. | Evidence for electroweak production of four charged leptons and two jets in proton-proton collisions at s = 13 TeV.
[País não identificado] |
| 42. | Evidence for Higgs boson decay to a pair of muons.
[País não identificado] |
| 43. | Experimental investigation of a strain gauge sensor based on Fiber Bragg Grating for diameter measurement.
[País não identificado] |
| 44. | Facile synthesis of transition metal (M = Cu, Co) oxide grafted graphitic carbon nitride nanosheets for high performance asymmetric supercapacitors.
[País não identificado] |
| 45. | FBG-Assisted Micro-Channel for Refractive Index Measurements.
[País não identificado] |
| 46. | First measurement of large area jet transverse momentum spectra in heavy-ion collisions.
[País não identificado] |
| 47. | First measurement of the cross section for top quark pair production with additional charm jets using dileptonic final states in pp collisions at s = 13.
[País não identificado] |
| 48. | Flattening the curves: on-off lock-down strategies for COVID-19 with an application to Brazil.
[País não identificado] |
| 49. | Formation of phosphine imide (HN-PH ) and its phosphinous amide (H N-PH ) isomer.
United States, Taiwan, Germany, Brazil. |
| 50. | Front-end electronics for CMS iRPC detectors.
[País não identificado] |
| 51. | Hard color-singlet exchange in dijet events in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 52. | In-medium modification of dijets in PbPb collisions at $$ sqrt{s_{mathrm{NN}}} $$ = 5.02 TeV.
[País não identificado] |
| 53. | Interocclusal Device Instrumented by Fiber Bragg Gratings: Case Study of Bruxism Treatment With Botulinum Toxin.
[País não identificado] |
| 54. | Kinetics of polymerization shrinkage of self-adhesive and conventional dual-polymerized resin luting agents inside the root canal.
[País não identificado] |
| 55. | Loading Condition Estimation Using Long-Period Fiber Grating Array.
[País não identificado] |
| 56. | Low-cost Trajectory-Based Ball Detection for Impact Indication and Recording.
[País não identificado] |
| 57. | Measurement of b jet shapes in proton-proton collisions at $$ sqrt{s} $$ = 5.02 TeV.
[País não identificado] |
| 58. | Measurement of differential cross sections for Z bosons produced in association with charm jets in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 59. | Measurement of differential t t ¯ production cross sections in the full kinematic range using.
[Não foi possível obter dados do DOI] |
| 60. | Measurement of differential t t ¯ production cross sections using top quarks at large transverse momenta in p p.
[Não foi possível obter dados do DOI] |
| 61. | Measurement of prompt D0 and D - 0 meson azimuthal anisotropy and search for strong electri.
[País não identificado] |
| 62. | Measurement of prompt open-charm production cross sections in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 63. | Measurement of the azimuthal anisotropy of and mesons in PbPb collisions at s NN.
[País não identificado] |
| 64. | Measurement of the CP-violating phase -s in the B s 0 →.
[País não identificado] |
| 65. | Measurement of the electroweak production of Z γ and two jets in proton-proton collisions at s = 13 - -.
[Não foi possível obter dados do DOI] |
| 66. | Measurement of the Higgs boson production rate in association with top quarks in final states with electrons, muons, and hadronically decaying tau leptons at $$sqrt{s} = 13, ext {Te} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 67. | Measurement of the inclusive and differential Higgs boson production cross sections in the leptonic WW decay mode at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 68. | Measurement of the inclusive and differential t$$ overline{t} $$γ cross sections in the single-lepton channel and EFT interpretation at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 69. | Measurement of the top quark mass using events with a single reconstructed top quark in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 70. | Measurement of the W γ Production Cross Section in Proton-Proton Collisions at s = 13 - -.
[Não foi possível obter dados do DOI] |
| 71. | Measurement of the Z boson differential production cross section using its invisible decay mode (Z → $$ u overline{ u} $$) in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 72. | Measurements of $${mathrm{p}} {mathrm{p}} ightarrow {mathrm{Z}} {mathrm{Z}} $$ production cross sections and constraints on anomalous triple gauge couplings at $$sqrt{s} = 13, ext {TeV} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 73. | Measurements of angular distance and momentum ratio distributions in three-jet and $${ ext {Z}}$$ + two-jet final states in $${ ext {p}}{ ext {p}}$$ collisions.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 74. | Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at $$ sqrt{mathrm{s}} $$ = 13 TeV.
[País não identificado] |
| 75. | Measurements of production cross sections of polarized same-sign W boson pairs in association with two jets in proton-proton collisions at s = 13 TeV.
[País não identificado] |
| 76. | Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 77. | Measurements of the differential cross sections of the production of Z + jets and γ + jets and of Z boson emission collinear with a jet in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 78. | Measurements of the Electroweak Diboson Production Cross Sections in Proton-Proton Collisions at s = 5.02 - - TeV Using Lepto.
[Não foi possível obter dados do DOI] |
| 79. | Measurements of the pp → W±γγ and pp → Zγγ cross sections at $$ sqrt{mathrm{s}} $$ = 13 TeV and limits on anomalous quartic gauge couplings.
[País não identificado] |
| 80. | Modelling of an Optical Access Network Platform for Radio-Frequency Transmission in the S Band / Modelação de uma Plataforma de Rede de Acesso Óptico para Transmissão de Radiofrequências na Banda S.
[Não foi possível obter dados do DOI] |
| 81. | Multi-Armed Bandits for Minesweeper: Profiting from Exploration-Exploitation Synergy.
[País não identificado] |
| 82. | Multi-plasmonic resonance based sensor for the characterization of optical dispersion using a D-shaped photonic crystal fiber.
[País não identificado] |
| 83. | MUSiC: a model-unspecific search for new physics in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 84. | New efficient subband structures for blind source separation.
[País não identificado] |
| 85. | Observation of a New Excited Beauty Strange Baryon Decaying to - b − π + π −.
[Não foi possível obter dados do DOI] |
| 86. | Observation of Forward Neutron Multiplicity Dependence of Dimuon Acoplanarity in Ultraperipheral Pb-Pb Collisions at s N N =.
[Não foi possível obter dados do DOI] |
| 87. | Observation of tW production in the single-lepton channel in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 88. | On the Skewness of the LMS Adaptive Weights.
[País não identificado] |
| 89. | On the synthesis of N-O bearing species in astrophysical ices - an infrared spectroscopic study using heavy-ion irradiation of solid N2: CO samples.
[Não foi possível obter dados do DOI] |
| 90. | On the Use of UTD-Based Models for RF Path Loss Prediction Due to Diffraction on a Forest-Covered Ridge.
[País não identificado] |
| 91. | One-step electropolymerization of methylene blue films on highly flexible carbon fiber electrode as supercapacitors.
[País não identificado] |
| 92. | Optical Inclinometer Based on a LPG-Taper Series Configuration.
[País não identificado] |
| 93. | Optical Properties of Iron to 30 eV.
Brazil. |
| 94. | Origin of ammoniated phyllosilicates on dwarf planet Ceres and asteroids.
United States, Italy, Brazil. |
| 95. | Performance of the CMS muon trigger system in proton-proton collisions at √(s) = 13.
[País não identificado] |
| 96. | Photogrammetric Process to Monitor Stress Fields Inside Structural Systems.
[País não identificado] |
| 97. | Positioning Analysis of HF Monopole Antennas on a Frigate.
[País não identificado] |
| 98. | Precision luminosity measurement in proton-proton collisions at $$sqrt{s} = 13,hbox {TeV}$$ in 2015 and 2016 at CMS.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 99. | Probing effective field theory operators in the associated production of top quarks with a Z boson in multilepton final states at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 100. | Rapid Radical-Radical Induced Explosive Desorption of Ice-coated Interstellar Nanoparticles.
[País não identificado] |
| 101. | Real-Time Fermentation Monitoring of Synthetic Beer Wort using Etched Fiber Bragg Grating..
[País não identificado] |
| 102. | Research and development of the back-end electronics for the two-dimensional improved resistive plate chambers in CMS upgrade.
[País não identificado] |
| 103. | Search for a heavy Higgs boson decaying into two lighter Higgs bosons in the ττbb final state at 13 TeV.
[País não identificado] |
| 104. | Search for a heavy resonance decaying to a top quark and a W boson at $$ sqrt{s} $$ = 13 TeV in the fully hadronic final state.
[País não identificado] |
| 105. | Search for a heavy vector resonance decaying to a $${mathrm{Z}}_{mathrm{}}^{mathrm{}}$$ boson and a Higgs boson in proton-proton collisions at $$sqrt{s} = 13, ext {Te} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 106. | Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton-proton collisions at $$sqrt{s} = 13,{ ext {TeV}} $$.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Uzbekistan, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Kuwait, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 107. | Search for chargino-neutralino production in events with Higgs and W bosons using 137 fb−1 of proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 108. | Search for dark matter produced in association with a leptonically decaying $${mathrm{Z}} $$ boson in proton-proton collisions at $$sqrt{s}=13, ext {Te} ext {V} $$. EUROPEAN PHYSICAL JOURNAL C.
South Korea, Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Australia, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 109. | Search for dark photons in Higgs boson production via vector boson fusion in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 110. | Search for lepton-flavor violating decays of the Higgs boson in the μ τ and e τ final states in proton-proton collisions at.
[Não foi possível obter dados do DOI] |
| 111. | Search for Long-Lived Particles Decaying in the CMS End Cap Muon Detectors in Proton-Proton Collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 112. | Search for long-lived particles decaying to jets with displaced vertices in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 113. | Search for long-lived particles using displaced jets in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 114. | Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 115. | Search for new physics in top quark production with additional leptons in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV using effective field theory.
[País não identificado] |
| 116. | Search for nonresonant Higgs boson pair production in final states with two bottom quarks and two photons in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 117. | Search for resonant and nonresonant new phenomena in high-mass dilepton final states at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 118. | Search for singly and pair-produced leptoquarks coupling to third-generation fermions in proton-proton collisions at s = 13 TeV.
[País não identificado] |
| 119. | Search for supersymmetry in final states with two oppositely charged same-flavor leptons and missing transverse momentum in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 120. | Search for the lepton flavor violating decay τ → 3μ in proton-proton collisions at $$ sqrt{mathrm{s}} $$ = 13 TeV.
[País não identificado] |
| 121. | Search for the rare decay of the W boson into a pion and a photon in proton-proton collisions at s = 13 TeV.
[País não identificado] |
| 122. | Search for top squark pair production using dilepton final states in $${ ext {p}}{ ext {p}}$$ collision data collected at $$sqrt{s}=13, ext {TeV} $$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 123. | Search for top squark production in fully hadronic final states in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 124. | Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 125. | Search for W- bosons decaying to a top and a bottom quark at s = 13 TeV in the hadronic final.
[País não identificado] |
| 126. | Second-Order Dispersion Sensor Based on Multi-Plasmonic Surface Resonances in D-Shaped Photonic Crystal Fibers.
[País não identificado] |
| 127. | Shared control methodology based on head positioning and vector fields for people with quadriplegia.
Brazil. |
| 128. | Studies of charm and beauty hadron long-range correlations in pp and pPb collisions at LHC energies.
[País não identificado] |
| 129. | Study of Drell-Yan dimuon production in proton-lead collisions at $$ sqrt{s_{mathrm{NN}}} $$ = 8.16 TeV.
[País não identificado] |
| 130. | Study of Z boson plus jets events using variables sensitive to double-parton scattering in pp collisions at 13 TeV.
[País não identificado] |
| 131. | Subsampled digital holographic image reconstruction by a compressive sensing approach.
[País não identificado] |
| 132. | Technical and Economic Feasibility Study for Implementing a Novel Mooring-Assisting Methodology in Offloading Operations Using Autonomous Unmanned Aerial Vehicles.
[Não foi possível obter dados do DOI] |
| 133. | The effect of multiscale hybridization on the mechanical properties of natural fiber¿reinforced composites.
[Não foi possível obter dados do DOI] |
| 134. | The effects of scaling and bends in a modalmetric acoustic detector.
[Não foi possível obter dados do DOI] |
| 135. | Towards a two-dimensional readout of the improved CMS Resistive Plate Chamber with a new front-end electronics.
[País não identificado] |
| 136. | Transient Analysis of the Bias-Compensated LMS Algorithm.
[País não identificado] |
| 137. | Transient Analysis of the Set-Membership LMS Algorithm.
[País não identificado] |
| 138. | Weight classifier using optical time domain reflectometry and a long period grating sensor.
[País não identificado] |
| 1. | - 2 -norm feature least mean square algorithm.
[Não foi possível obter dados do DOI] |
| 2. | 3D Correspondence and Point Projection Method for Structures Deformation Analysis.
[País não identificado] |
| 3. | A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution.
[País não identificado] |
| 4. | A Heterogeneous Edge-Fog Environment Supporting Digital Twins for Remote Inspections.
[País não identificado] |
| 5. | A Mathematical Model for the Interrogation of LPG Fiber Optical Sensors Based on Electrical Harmonic Analysis.
[País não identificado] |
| 6. | A measurement of the Higgs boson mass in the diphoton decay channel.
[País não identificado] |
| 7. | A multi-dimensional search for new heavy resonances decaying to boosted $$ ext{ W }{}{}$$ $$ ext{ W }{}{}$$ , $$ ext{ W }{}{}$$ $$ ext{ Z }{}{}$$ , or $$ ext{ Z }{}{}$$ $$ ext{ Z }{}{}$$ boson pairs in the dijet final state at 13$$ ext {Te} ext {V}$$.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 8. | A new approach for CMS RPC current monitoring using Machine Learning techniques.
[País não identificado] |
| 9. | A Robotic Cognitive Architecture for Slope and Dam Inspections.
[País não identificado] |
| 10. | A search for the standard model Higgs boson decaying to charm quarks.
[País não identificado] |
| 11. | Adhesively bonded aluminium double-strap joints: effects of patch part on failure load.
[País não identificado] |
| 12. | Aerial Human Activity Recognition Through a Cognitive Architecture and a New Automata Proposal.
[Não foi possível obter dados do DOI] |
| 13. | Aerial Image Instance Segmentation Through Synthetic Data Using Deep Learning.
[Não foi possível obter dados do DOI] |
| 14. | Aging study on Resistive Plate Chambers of the CMS Muon Detector for HL-LHC.
[País não identificado] |
| 15. | An Exact Expectation Model for the LMS Tracking Abilities.
[País não identificado] |
| 16. | An Experimental and Theoretical Investigation into the Formation of Ketene (H CCO) and Ethynol (HCCOH) in Interstellar Analog Ices.
[País não identificado] |
| 17. | Analysis of Failure Pressure of Defective Pipes Repaired with Composite Systems Considering the Plastic Deformation of Pipe.
[País não identificado] |
| 18. | Analysis of mechanical and thermal properties of epoxy multiwalled carbon nanocomposites.
[Não foi possível obter dados do DOI] |
| 19. | Bias-compensated FX-LMS algorithm.
[Não foi possível obter dados do DOI] |
| 20. | Biomass-derived porous activated carbon from Syzygium cumini fruit shells and Chrysopogon zizanioides roots for high-energy density symmetric supercapacitors.
[País não identificado] |
| 21. | Bose-Einstein correlations of charged hadrons in proton-proton collisions at s$$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 22. | Bulk Fill flow resin contraction using 3D finite element model and calibration by Fiber Bragg Grating measurement.
[Não foi possível obter dados do DOI] |
| 23. | CMS RPC activities during LHC LS-2.
[País não identificado] |
| 24. | Comparison of the properties of a-C:H films deposited from methane and heptane precursors: study of the mechanical, chemical and structural properties.
[País não identificado] |
| 25. | Composite repair system for corroded metallic pipelines: an overview of recent developments and modelling.
[País não identificado] |
| 26. | Correlated Time-Series in Multi-Day-Ahead Streamflow Forecasting Using Convolutional Networks.
[País não identificado] |
| 27. | Deep Learning Applied to Vegetation Identification and Removal Using Multidimensional Aerial Data.
[País não identificado] |
| 28. | Dependence of inclusive jet production on the anti-kT distance parameter in pp collisions at $$ sqrt{mathrm{s}} $$ = 13 TeV.
[País não identificado] |
| 29. | Determination of the strong coupling constant αS(mZ) from measurements of inclusive W± and Z boson production cross sections in proton-proton collisions at $$ sqrt{mathrm{s}} $$ = 7 and 8 TeV.
[País não identificado] |
| 30. | Distributed Adaptive Filtering on Wireless Sensor Networks with Shared Medium Competition.
[Não foi possível obter dados do DOI] |
| 31. | Effect of intralaminar hybridization on mode I fracture toughness of natural fiber-reinforced composites.
[País não identificado] |
| 32. | Effect of material on the mechanical properties of additive manufactured thermoplastic parts.
[País não identificado] |
| 33. | Effect of surface treatments on interfacial properties of natural intralaminar hybrid composites.
[Não foi possível obter dados do DOI] |
| 34. | Effects of heat treatment on the behavior of teak wood adherends bonded joints.
[País não identificado] |
| 35. | Effects of the electronic threshold on the performance of the RPC system of the CMS experiment.
[País não identificado] |
| 36. | Electropolymerization of p-phenylenediamine films on carbon fiber fabrics electrode for flexible supercapacitors: surface and electrochemical characterizations.
[País não identificado] |
| 37. | Estimation of statistical properties of rough surface profiles from the Hurst exponent of speckle patterns.
[País não identificado] |
| 38. | Evidence for $$ ext {W} ext {W}$$WW production from double-parton interactions in proton-proton collisions at $$sqrt{s} = 13 , ext {TeV} $$s=13TeV.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 39. | Evidence for Top Quark Production in Nucleus-Nucleus Collisions.
[Não foi possível obter dados do DOI] |
| 40. | Experiences from the RPC data taking during the CMS RUN-2.
[País não identificado] |
| 41. | Extraction and validation of a new set of CMS pythia8 tunes from underlying-event measurements.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 42. | Fault detection and classification in oil wells and production/service lines using random forest.
[País não identificado] |
| 43. | High Accuracy Homodyne Interferometric Method for Wide Dynamic Range Applications.
[País não identificado] |
| 44. | Identification of heavy, energetic, hadronically decaying particles using machine-learning techniques.
[País não identificado] |
| 45. | Improved sparsity-aware NSAF-SF adaptive algorithm.
[Não foi possível obter dados do DOI] |
| 46. | Inclusive search for highly boosted Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 47. | Influence of annealing temperature in nitrogen doped porous carbon balls derived from hypercross-linked polymer of anthracene for supercapacitor applications.
[País não identificado] |
| 48. | Interrogation system for optical sensor using filter bank and artificial neural network.
[Não foi possível obter dados do DOI] |
| 49. | Investigation into the event-activity dependence of ϒ(nS) relative production in proton-proton collisions at $$ sqrt{s} $$ = 7 TeV.
[País não identificado] |
| 50. | Ion Irradiation of Acetylene Ice in the ISM and the Outer Solar System: Laboratory Simulations.
Brazil, Germany. |
| 51. | Listening to pulses of radiation: design of a submersible thermoacoustic sensor.
Brazil. |
| 52. | Low-Cost Device to Measure Concentration of Saccharomyces cerevisiae Through Methylene Blue Reduction.
[País não identificado] |
| 53. | Magnetic properties of superconducting phases NiBi and NiBi3 formed during pulsed laser deposition of Ni-Bi films.
[País não identificado] |
| 54. | Manganese oxide nanofoam prepared by pulsed laser deposition for high performance supercapacitor electrodes.
[País não identificado] |
| 55. | Measurement of $$hbox {t}{ar{hbox {t}}}$$ normalised multi-differential cross sections in $${ ext {p}}{ ext {p}} $$ collisions at $$sqrt{s}=13,{ ext {TeV}} $$, and simultaneous determination of the strong coupling strength, top quark pole mass, and parton distribution functions.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 56. | Measurement of B c ( 2 S ) + and.
[Não foi possível obter dados do DOI] |
| 57. | Measurement of CKM matrix elements in single top quark t-channel production in proton-proton collisions at s = 13 TeV.
[País não identificado] |
| 58. | Measurement of differential cross sections and charge ratios for t-channel single top quark production in proton-proton collisions at $$sqrt{s}=13$$ $$, ext {Te} ext {V}$$.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 59. | Measurement of electroweak production of a $$mathrm{W} $$W boson in association with two jets in proton-proton collisions at $$sqrt{s}=13, ext {Te} ext {V} $$s=13Te.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 60. | Measurement of properties of $$ {mathrm{B}}_{mathrm{s}}^0 $$→ μ+μ− decays and search for B0→ μ+μ− with the CMS experiment.
[País não identificado] |
| 61. | Measurement of quark- and gluon-like jet fractions using jet charge in PbPb and pp collisions at 5.02 TeV.
[País não identificado] |
| 62. | Measurement of single-diffractive dijet production in proton-proton collisions at $$sqrt{s} = 8, ext {Te} ext {V} $$ with the CMS and TOTEM experiments.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 63. | Measurement of the cross section for $$ mathrm{t}overline{mathrm{t}} $$ production with additional jets and b jets in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 64. | Measurement of the cross section for electroweak production of a Z boson, a photon and two jets in proton-proton collisions at $$ sqrt{mathrm{s}} $$ = 13 TeV and constraints on anomalous quartic couplings.
[País não identificado] |
| 65. | Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 66. | Measurement of the top quark pair production cross section in dilepton final states containing one τ lepton in pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 67. | Measurement of the top quark Yukawa coupling from t t ¯ kinematic distributions in the dilepton final state in proton-proton collisions at.
[Não foi possível obter dados do DOI] |
| 68. | Measurement of the Y(1S) pair production cross section and search for resonances decaying to Y(1S)μ+μ− in proton-proton collisions at s = 13.
[País não identificado] |
| 69. | Measurement of top quark pair production in association with a Z boson in proton-proton collisions at s$$ sqrt{mathrm{s}} $$ = 13 TeV.
[País não identificado] |
| 70. | Measurements of production cross sections of WZ and same-sign WW boson pairs in association with two jets in proton-proton collisions at s = 13.
[País não identificado] |
| 71. | Measurements of t t ¯ H Production and the C.
[Não foi possível obter dados do DOI] |
| 72. | Measurements of the W boson rapidity, helicity, double-differential cross sections, and charge asymmetry in p p collisions at s =.
[Não foi possível obter dados do DOI] |
| 73. | Mechanical and Thermal Characterization of Natural Intralaminar Hybrid Composites Based on Sisal.
Brazil. |
| 74. | Mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles in $$mathrm {PbPb}$$ collisions at $$sqrt{smash [b]{s_{_{mathrm {NN}}}}} = 2.76$$ and 5.02$$, ext {TeV}$$.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 75. | Multiparticle correlation studies in p Pb collisions at s N N = 8.16 TeV.
[Não foi possível obter dados do DOI] |
| 76. | Nickel nanoparticles supported by commercial carbon paper as a catalyst for urea electro-oxidation.
[País não identificado] |
| 77. | Novel Proportionate Adaptive Filters with Coefficient Vector Reusing.
[País não identificado] |
| 78. | Observation of electroweak production of Wγ with two jets in proton-proton collisions at s = 13 TeV.
[País não identificado] |
| 79. | Observation of the B s 0 → X ( 38.
[Não foi possível obter dados do DOI] |
| 80. | Observation of the Production of Three Massive Gauge Bosons at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 81. | On the Analysis of the Incremental $$ell _0$$-LMS Algorithm for Distributed Systems.
[País não identificado] |
| 82. | On the Performance Analysis of Normalized Subband Adaptive Filtering Algorithm with Sparse Subfilters.
[País não identificado] |
| 83. | On the steady-state performance of bias-compensated LMS algorithm.
[Não foi possível obter dados do DOI] |
| 84. | Photoelectric performance evaluation of DSSCs using the dye extracted from different color petals of Leucanthemum vulgare flowers as novel sensitizers.
[País não identificado] |
| 85. | Pileup mitigation at CMS in 13 TeV data.
[País não identificado] |
| 86. | Prediction of the burst pressure for defective pipelines using different semi-empirical models.
France, Italy, Brazil. |
| 87. | Radiolysis of Ices by Cosmic-Rays: CH 4 and H 2 O Ices Mixtures Irradiated by 40 MeV 58 Ni 11+ Ions.
[País não identificado] |
| 88. | Radiolysis of NH3:CO ice mixtures - Implications for Solar System and Interstellar Ices. ROYAL ASTRONOMICAL SOCIETY.
[Não foi possível obter dados do DOI] |
| 89. | Reconstruction of signal amplitudes in the CMS electromagnetic calorimeter in the presence of overlapping proton-proton interactions.
[País não identificado] |
| 90. | RPC system in the CMS Level-1 Muon Trigger.
[País não identificado] |
| 91. | Search for a charged Higgs boson decaying into top and bottom quarks in events with electrons or muons in proton-proton collisions at $$ sqrt{mathrm{s}} $$ = 13 TeV.
[País não identificado] |
| 92. | Search for a heavy Higgs boson decaying to a pair of W bosons in proton-proton collisions at s$$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 93. | Search for a heavy pseudoscalar Higgs boson decaying into a 125 GeV Higgs boson and a Z boson in final states with two tau and two light leptons at s$$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 94. | Search for a light charged Higgs boson in the H ± → c s channel in proton-proton collisions at s /.
[País não identificado] |
| 95. | Search for a light pseudoscalar Higgs boson in the boosted μμττ final state in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 96. | Search for an excited lepton that decays via a contact interaction to a lepton and two jets in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 97. | Search for bottom-type, vectorlike quark pair production in a fully hadronic final state in proton-proton collisions at s = 13 - - TeV.
[País não identificado] |
| 98. | Search for charged Higgs bosons decaying into a top and a bottom quark in the all-jet final state of pp collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 99. | Search for dark matter particles produced in association with a Higgs boson in proton-proton collisions at s$$ sqrt{mathrm{s}} $$ = 13 TeV.
[País não identificado] |
| 100. | Search for decays of the 125 GeV Higgs boson into a Z boson and a ρ or - meson.
[País não identificado] |
| 101. | Search for direct top squark pair production in events with one lepton, jets, and missing transverse momentum at 13 TeV with the CMS experiment.
[País não identificado] |
| 102. | Search for disappearing tracks in proton-proton collisions at s = 13 TeV.
[País não identificado] |
| 103. | Search for electroweak production of a vector-like T quark using fully hadronic final states.
[País não identificado] |
| 104. | Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 105. | Search for high mass dijet resonances with a new background prediction method in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 106. | Search for lepton flavour violating decays of a neutral heavy Higgs boson to μτ and eτ in proton-proton collisions at s$$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 107. | Search for new neutral Higgs bosons through the H→ZA→-+-−bb¯$$ mathrm{H} o mathrm{ZA} o {ell}^{+}{ell}^{-}mathrm{b}overline{mathrm{b}} $$ process in pp collisions at s$$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 108. | Search for physics beyond the standard model in events with jets and two same-sign or at least three charged leptons in proton-proton collisions at $$sqrt{s}=13,{ ext {TeV}} $$.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 109. | Search for physics beyond the standard model in multilepton final states in proton-proton collisions at s$$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 110. | Search for production of four top quarks in final states with same-sign or multiple leptons in proton-proton collisions at $$sqrt{s}=13$$ $$, ext {TeV}$$.
Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 111. | Search for resonant pair production of Higgs bosons in the b b Z Z channel in proton-proton collisions at s = 13 -.
[Não foi possível obter dados do DOI] |
| 112. | Search for supersymmetry in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV in events with high-momentum Z bosons and missing transverse momentum.
[País não identificado] |
| 113. | Search for top squark pair production in a final state with two tau leptons in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 114. | Searches for physics beyond the standard model with the $$M_{mathrm {T2}}$$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $$sqrt{s}=13, ext {Te} ext {V} $$.
South Korea, Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 115. | Sensors Fusion and Multidimensional Point Cloud Analysis for Electrical Power System Inspection.
[País não identificado] |
| 116. | Strange hadron production in pp and p Pb collisions at s N N = 5.02.
[Não foi possível obter dados do DOI] |
| 117. | Study of central exclusive 'Equation missing' production in proton-proton collisions at $$sqrt{s} = 5.02$$ and 13TeV.
South Korea, Turkey, France, Montenegro, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 118. | Surveillance Architecture for Human Activity Recognition using Unmanned Aerial Vehicle.
[Não foi possível obter dados do DOI] |
| 119. | The effect of environment and fatigue loading on the behaviour of TEPs-modified adhesives.
[Não foi possível obter dados do DOI] |
| 120. | The elusive cyclotriphosphazene molecule and its Dewar benzene-type valence isomer (P N ).
[Não foi possível obter dados do DOI] |
| 121. | The production of isolated photons in PbPb and pp collisions at $$ sqrt{s_{mathrm{NN}}} $$ = 5.02 TeV.
[País não identificado] |
| 122. | Transient Analysis of the Block Least Mean Squares Algorithm.
[País não identificado] |
| 123. | Tuning the morphology of manganese oxide nanostructures for obtaining both high gravimetric and volumetric capacitance.
Brazil. |
| 124. | W + W − boson pair production in proton-proton collisions at s = 13.
[Não foi possível obter dados do DOI] |
| 1. | A Framework for Analyzing Fog-Cloud Computing Cooperation Applied to Information Processing of UAVs.
[Não foi possível obter dados do DOI] |
| 2. | Advances on the analysis of the LMS algorithm with a colored measurement noise.
[País não identificado] |
| 3. | An Open-Source Simulator Applied to Prism Coupling Sensors Based on Kretschmann's Configuration.
[País não identificado] |
| 4. | Asymmetric supercapacitor based on carbon nanofibers as the anode and two-dimensional copper cobalt oxide nanosheets as the cathode.
[País não identificado] |
| 5. | Autonomous Unmanned Aerial Vehicles in Search and Rescue Missions Using Real-Time Cooperative Model Predictive Control.
[País não identificado] |
| 6. | Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in $${ ext {p}} { ext {p}} $$ pp collisions at $$sqrt{s}=13, ext {Te} ext {V} $$ s = 13 Te.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 7. | Bonded composite repair of metallic pipeline using energy release rate method.
[Não foi possível obter dados do DOI] |
| 8. | Case study for monitoring the rhythmic masticatory muscle activity during sleep bruxism episodes by using fiber Bragg gratings.
[País não identificado] |
| 9. | Centrality and pseudorapidity dependence of the transverse energy density in p Pb collisions at s N N = 5.02.
[Não foi possível obter dados do DOI] |
| 10. | Characterization of Wide Band Chirp of Laser Diodes with Time-Resolved Spectroscopy.
[País não identificado] |
| 11. | Charged-particle angular correlations in XeXe collisions at s N N = 5.44 TeV.
[Não foi possível obter dados do DOI] |
| 12. | Combined measurements of Higgs boson couplings in proton-proton collisions at $$sqrt{s}=13, ext {Te} ext {V} $$ s = 13 Te.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 13. | Comments on -A Generic Approach for Permittivity Measurement of Dielectric Materials Using a Discontinuity in a Rectangular Waveguide-.
[País não identificado] |
| 14. | Comparative performance analysis of relative humidity sensor based on intermodal interference using tapered square no-core optical fiber and tapered cylindrical optical fiber.
[País não identificado] |
| 15. | Compressive holography with resolution improvement and lensless adjustable magnification.
[País não identificado] |
| 16. | Critical Issues of Double-Metal Layer Coating on FBG for Applications at High Temperatures.
[País não identificado] |
| 17. | Debonding on Demand of Adhesively Bonded Joints: A Critical Review.
[Não foi possível obter dados do DOI] |
| 18. | Dentistry applications of fiber Bragg gratings: irradiation protocols for bulk fill flow dental composites.
[País não identificado] |
| 19. | Digital interface device for field soil hydraulic conductivity measurement.
[País não identificado] |
| 20. | Effect of chemical treatment on the thermal properties of hybrid natural fiber-reinforced composites.
[Não foi possível obter dados do DOI] |
| 21. | Efficient Volterra systems identification using hierarchical genetic algorithms.
[País não identificado] |
| 22. | Exact Expectation Analysis of the Deficient-Length LMS Algorithm.
[País não identificado] |
| 23. | Exact Expectation Analysis of the LMS Adaptive Identification of Nonlinear Systems.
[Não foi possível obter dados do DOI] |
| 24. | Exact Expectation Evaluation and Design of Variable Step-Size Adaptive Algorithms.
[País não identificado] |
| 25. | Experimental analysis of adhesively bonded joints in synthetic- and natural fibre-reinforced polymer composites.
[Não foi possível obter dados do DOI] |
| 26. | Fabrication of Brushite Coating on AZ91D and AZ31 Alloys by Two-Step Chemical Treatment and Its Surface Protection in Simulated Body Fluid.
[País não identificado] |
| 27. | Formation of Glyoxylic Acid (HCOCOOH) in Interstellar Ices - A Key Entry Point for Prebiotic Chemistry.
[Não foi possível obter dados do DOI] |
| 28. | Functionally graded adhesive joints by using thermally expandable particles.
[Não foi possível obter dados do DOI] |
| 29. | High Accuracy Homodyne Interferometric Method for Wide Dynamic Range Applications.
[País não identificado] |
| 30. | Hybrid Methodology for Path Planning and Computational Vision Applied to Autonomous Mission: A New Approach.
[País não identificado] |
| 31. | Inclusive search for supersymmetry in pp collisions at s = 13 $$ sqrt{s}=13 $$ TeV using razor variables and boosted object identification in zero and one lepton final states.
[País não identificado] |
| 32. | Influence of adherend properties on the strength of adhesively bonded joints.
[País não identificado] |
| 33. | Integral transform analysis of heat and mass diffusion in chemically reacting systems with Michaelis-Menten kinetics.
[País não identificado] |
| 34. | Interfacial adhesion between embedded fibre optic sensors and epoxy matrix in composites.
[Não foi possível obter dados do DOI] |
| 35. | Interference in beer bitterness measurements caused by polymer tubes.
[País não identificado] |
| 36. | Interlaminar adhesion assessment of carbon-epoxy laminates under salt water ageing using peel tests.
[Não foi possível obter dados do DOI] |
| 37. | Low-cost fluorescence-based method for beer bitterness measurement.
[País não identificado] |
| 38. | Macrobending SMS fiber-optic anemometer and flow sensor.
[País não identificado] |
| 39. | Measurement of associated production of a $$mathrm {W}$$ W boson and a charm quark in proton-proton collisions at $$sqrt{s} = 13, ext {Te} ext {V} $$ s = 13 Te.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 40. | Measurement of differential cross sections for inclusive isolated-photon and photon+jet production in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$s=13TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Lebanon, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 41. | Measurement of exclusive $$mathrm {Upsilon }$$ - photoproduction from protons in $$mathrm {p}$$ p Pb collisions at $$sqrt{smash [b]{s_{_{mathrm {NN}}}}} = 5.02, ext {TeV} $$ s NN = 5.02 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 42. | Measurement of inclusive and differential Higgs boson production cross sections in the diphoton decay channel in proton-proton collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 43. | Measurement of inclusive very forward jet cross sections in proton-lead collisions at s N N $$ sqrt{s_{mathrm{NN}}} $$ = 5.02 TeV.
[País não identificado] |
| 44. | Measurement of the energy density as a function of pseudorapidity in proton-proton collisions at $$sqrt{s} =13, ext {TeV} $$ s = 13 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 45. | Measurement of the top quark mass in the all-jets final state at $$sqrt{s}=13, ext {TeV} $$ s = 13 TeV and combination with the lepton+jets channel.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Latvia, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 46. | Measurements of t t ¯ $$ mathrm{t}overline{mathrm{t}} $$ differential cross sections in proton-proton collisions at s = 13 $$ sqrt{mathrm{s}}=13 $$ TeV using events containing two leptons.
[País não identificado] |
| 47. | Measurements of the pp → WZ inclusive and differential production cross sections and constraints on charged anomalous triple gauge couplings at s $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 48. | Mechanical characterization of a modern epoxy adhesive for automotive industry.
[País não identificado] |
| 49. | Mechanical Characterization of Bonded Joints Made of Additive Manufactured Adherends.
[País não identificado] |
| 50. | Mechanical characterization of intralaminar natural fibre-reinforced hybrid composites.
[País não identificado] |
| 51. | Methodology for Autonomous Crossing Narrow Passages Applied on Assistive Mobile Robots.
[País não identificado] |
| 52. | Mobile Robot Localization Based on the Novel Leader-Based Bat Algorithm.
[País não identificado] |
| 53. | N-O bearing molecules produced by radiolysis of N2O and N2O:CO2 ices.
[País não identificado] |
| 54. | Neutrinos Angra experiment: commissioning and first operational measurements.
[País não identificado] |
| 55. | Novel Proportionate Adaptive Filters with Coefficient Vector Reusing.
[País não identificado] |
| 56. | Origin of alkylphosphonic acids in the interstellar medium.
[Não foi possível obter dados do DOI] |
| 57. | PAH Products and Processing by Different Energy Sources.
[País não identificado] |
| 58. | Photonic Generation of NLFM Microwave Pulses from DFB-Laser Chirp.
[País não identificado] |
| 59. | Prediction of Failure Pressure for Defective Pipelines Reinforced with Composite System, Accounting for Pipe Extremities.
[País não identificado] |
| 60. | Probing the chiral magnetic wave in p Pb and PbPb collisions at s NN = 5.02 TeV.
[Não foi possível obter dados do DOI] |
| 61. | Rate-Distortion Performance and Incremental Transmission Scheme of Compressive Sensed Measurements in Wireless Sensor Networks.
[País não identificado] |
| 62. | RECEPÇÃO ACÚSTICA SUBMARINA POR MEIO DE HIDROFONES BASEADOS EM FBG (FIBER BRAGG GRATING).
[Não foi possível obter dados do DOI] |
| 63. | Search for a heavy pseudoscalar boson decaying to a Z and a Higgs boson at $$sqrt{s}=13, ext {Te} ext {V} $$ s = 13 Te.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 64. | Search for a heavy resonance decaying to a top quark and a vector-like top quark in the lepton + jets final state in pp collisions at $$sqrt{s} = 13, ext {TeV} $$ s = 13 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 65. | Search for a W- boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state.
[País não identificado] |
| 66. | Search for anomalous triple gauge couplings in WW and WZ production in lepton + jet events in proton-proton collisions at $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 67. | Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 68. | Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at $$sqrt{s}=13, ext {Te} ext {V} $$ s = 13 Te.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 69. | Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 70. | Search for excited leptons in --γ final states in proton-proton collisions at s = 13 $$ sqrt{mathrm{s}}=13 $$ TeV.
[País não identificado] |
| 71. | Search for heavy Majorana neutrinos in same-sign dilepton channels in proton-proton collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 72. | Search for heavy neutrinos and third-generation leptoquarks in hadronic states of two τ leptons and two jets in proton-proton collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 73. | Search for heavy resonances decaying into two Higgs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 TeV.
[País não identificado] |
| 74. | Search for new particles decaying to a jet and an emerging jet.
[País não identificado] |
| 75. | Search for nonresonant Higgs boson pair production in the b b ¯ b b ¯ $$ mathrm{b}overline{mathrm{b}}mathrm{b}overline{mathrm{b}} $$ final state at s $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 76. | Search for production of Higgs boson pairs in the four b quark final state using large-area jets in proton-proton collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 77. | Search for rare decays of $$mathrm {Z}$$ Z and Higgs bosons to $${mathrm {J}/psi } $$ J / ψ and a photon in proton-proton collisions at $$sqrt{s}$$ s = 13 $$, ext {TeV}$$ TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 78. | Search for resonant production of second-generation sleptons with same-sign dimuon events in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$ s = 13 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 79. | Search for resonant t t ¯ $$ mathrm{t}overline{mathrm{t}} $$ production in proton-proton collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 80. | Search for single production of vector-like quarks decaying to a top quark and a $$mathrm {W} $$ W boson in proton-proton collisions at $$sqrt{s} = 13 , ext {TeV} $$ s = 13 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 81. | Search for supersymmetry in events with a photon, a lepton, and missing transverse momentum in proton-proton collisions at s=13$$ sqrt{s} = 13 $$ TeV.
[País não identificado] |
| 82. | Search for supersymmetry using Higgs boson to diphoton decays at s$$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 83. | Search for supersymmetry with a compressed mass spectrum in the vector boson fusion topology with 1-lepton and 0-lepton final states in proton-proton collisions at s $$ sqrt{s} $$ = 13 TeV.
[País não identificado] |
| 84. | Search for t t ¯ H $$ mathrm{t}overline{mathrm{t}}mathrm{H} $$ production in the H → b b ¯ $$ mathrm{H} o mathrm{b}overline{mathrm{b}} $$ decay channel with leptonic t t ¯ $$ mathrm{t}overline.
[País não identificado] |
| 85. | Search for the associated production of the Higgs boson and a vector boson in proton-proton collisions at s $$ sqrt{s} $$ = 13 TeV via Higgs boson decays to τ leptons.
[País não identificado] |
| 86. | Search for vector-like quarks in events with two oppositely charged leptons and jets in proton-proton collisions at $$sqrt{s} = 13, ext {Te} ext {V} $$ s = 13 Te.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 87. | Sensitivity of fiber-based modalmetric devices intended for optical detection of acoustic signals.
[Não foi possível obter dados do DOI] |
| 88. | Sparsity-Aware Reuse of Coefficients NLMS.
[Não foi possível obter dados do DOI] |
| 89. | Strain sensing based on a core diameter mismatch structure.
[Não foi possível obter dados do DOI] |
| 90. | Study of the underlying event in top quark pair production in $$mathrm {p}mathrm {p}$$ p p collisions at 13 $$~ ext {Te} ext {V}$$ Te.
South Korea, Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 91. | Theoretical assessment of the elastic modulus of natural fiber-based intra-ply hybrid composites.
[País não identificado] |
| 92. | Untangling the Formation of Methoxymethanol (CH OCH OH) and Dimethyl Peroxide (CH OOCH ) in Star-forming Regions.
[País não identificado] |
| 93. | Wind Generation Impact in Transmission Expansion Planning.
[País não identificado] |
| 1. | A 99.95% linearity readout circuit with 72dB dynamic range for active pixel sensors.
[Não foi possível obter dados do DOI] |
| 2. | A Case Study on the Bandwidth Broadening of a Skeletal Biconical Antenna.
[País não identificado] |
| 3. | A Combined Experimental and Theoretical Study on the Formation of Interstellar Propylene Oxide (CH CHCH O)-A Chiral Molecule.
[País não identificado] |
| 4. | A Mechanistical Study on the Formation of Dimethyl Ether (CH OCH ) and Ethanol (CH CH OH) in Methanol-containing Ices and Implications for the Chemistry of Star-forming Regions.
[País não identificado] |
| 5. | A Photoionization Reflectron Time-of-flight Mass Spectrometric Study on the Formation of Acetic Acid (CH COOH) in Interstellar Analog Ices.
[País não identificado] |
| 6. | A Vacuum Ultraviolet Photoionization Study on the Formation of -methyl Formamide (HCONHCH ) in Deep Space: A Potential Interstellar Molecule with a Peptide Bond.
[País não identificado] |
| 7. | An assessment of composite repair system in offshore platform for corroded circumferential welds in super duplex steel pipe.
Italy, Brazil. |
| 8. | An interstellar synthesis of phosphorus oxoacids.
France, United States, Taiwan, Brazil. |
| 9. | Analysis of ITU-R VHF/UHF propagation prediction methods performance on irregular terrains covered by forest.
[Não foi possível obter dados do DOI] |
| 10. | Analysis of Optical Erasure Efficiency in WDM-PONs Employing Carrier Remodulation.
[Não foi possível obter dados do DOI] |
| 11. | Assessment of failure pressure of a GFRP composite repair system for wall loss defect in metallic pipelines.
[Não foi possível obter dados do DOI] |
| 12. | Automated System for Femtosecond Laser Writing of Photonic Structures.
[País não identificado] |
| 13. | Avaliação da transmissão de temperatura da resina acrílica para os ossos cortical e medular por meio de redes de Bragg.
[Não foi possível obter dados do DOI] |
| 14. | Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $$sqrt{s}= 13~hbox {TeV}$$s=13TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 15. | Biocompatible hydrophilic brushite coatings on AZX310 and AM50 alloys for orthopaedic implants.
[País não identificado] |
| 16. | Bonded repair of composite structures in aerospace application: a review on environmental issues.
[País não identificado] |
| 17. | Bose-Einstein correlations in p p , p Pb , and PbPb collisions at s N N.
[Não foi possível obter dados do DOI] |
| 18. | Case study of muscle fatigue in parafunctional patient using occlusal device with fiber Bragg grating sensors.
[País não identificado] |
| 19. | Charged-particle nuclear modification factors in XeXe collisions at sNN=5.44$$ sqrt{s_{mathrm{NN}}} = 5.44 $$ TeV.
[País não identificado] |
| 20. | Chemical reactions in the nitrogen-acetone ice induced by cosmic ray analogues: relevance for the Solar system. ROYAL ASTRONOMICAL SOCIETY.
[Não foi possível obter dados do DOI] |
| 21. | Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 22. | Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at sNN=5.02$$ sqrt{s_{mathrm{NN}}}=5.02 $$ TeV.
[País não identificado] |
| 23. | Constraining the Molecular Complexity in the Interstellar Medium-The Formation of Ethyl Methyl Ether (CH OCH CH ) in Star-forming Regions.
[País não identificado] |
| 24. | Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in p Pb and PbPb collisions at the CERN Large Hadron Collider.
[Não foi possível obter dados do DOI] |
| 25. | Constraints on the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 26. | Dopant Effects of Gd3+ on the Electrochemical Pseudocapacitive Characteristics of Electroactive Mesoporous NiO Electrodes for Supercapacitors.
[Não foi possível obter dados do DOI] |
| 27. | Dynamics of single-bubble sonoluminescence. An alternative approach to the Rayleigh-Plesset equation.
[País não identificado] |
| 28. | Effect of Babassu Natural Filler on PBAT/PHB Biodegradable Blends: An Investigation of Thermal, Mechanical, and Morphological Behavior.
[País não identificado] |
| 29. | Effect of moisture on the adhesion of CFRP-to-steel bonded joints using peel tests.
[País não identificado] |
| 30. | Effect of Temperature and Moisture on the Tensile Properties of a TEPs-Modified Adhesive.
Romania, Brazil. |
| 31. | Effect of Water on the Behaviour of Adhesives Modified with Thermally Expandable Particles.
[País não identificado] |
| 32. | Effects of Birefringence on the Electromagnetic Guidance of Structures Produced by Femtosecond Laser.
[País não identificado] |
| 33. | Electroweak production of two jets in association with a Z boson in proton-proton collisions at $$sqrt{s}= $$s= 13$$, ext {TeV}$$TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 34. | Erratum: Radiolysis of N2O:CO2 Ice by Heavy Ions: Simulation of Cosmic Ray Effects.
[Não foi possível obter dados do DOI] |
| 35. | Event shape variables measured using multijet final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 36. | Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying τ leptons at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 37. | Exact analysis of the least-mean-square algorithm with coloured measurement noise.
[Não foi possível obter dados do DOI] |
| 38. | Experimental and numerical study on refractive index sensors based on fibre Bragg gratings inscribed in multimode fibre.
[País não identificado] |
| 39. | Frequency Response Characterization of a Sonoluminescence Acoustic Resonator by Using a FPGA-Based Instrumentation.
[País não identificado] |
| 40. | Highly Spectrally Efficient Discrete Multi-Tone Transmission over Step Index PMMA optical fibre for Short-Range Optical Communication.
[País não identificado] |
| 41. | Influence of nanostructured TiO2 film thickness in dye-sensitized solar cells using naturally extracted dye from Thunbergia erecta flowers as a photosensitizer.
[País não identificado] |
| 42. | Infrared Spectroscopy of Matrix-Isolated Neutral and Ionized Anthracoronene in Argon.
[Não foi possível obter dados do DOI] |
| 43. | Investigation of nanostructured TiO2 thin film coatings for DSSCs application using natural dye extracted from jabuticaba fruit as photosensitizers.
[País não identificado] |
| 44. | Ion irradiation of N2O ices and NO2:N2O4 ice mixtures: first steps to understand the evolution of molecules with the N−O bond in space.
[Não foi possível obter dados do DOI] |
| 45. | Jet properties in PbPb and pp collisions at sNN=5.02$$ sqrt{s_{mathrm{N};mathrm{N}}}=5.02 $$ TeV.
[País não identificado] |
| 46. | Low-frequency detection of acoustic signals using fiber as an ultrasonic guide with a distant in-fiber Bragg grating.
[Não foi possível obter dados do DOI] |
| 47. | Manufacture of Tapered Fibers and FBG Writing.
[País não identificado] |
| 48. | MARTA: a high-energy cosmic-ray detector concept for high-accuracy muon measurement.
United States, Portugal, Italy, Argentina, Spain, Czech Republic, Brazil. |
| 49. | Measurement of associated Z + charm production in proton-proton collisions at $$sqrt{s} = 8$$s=8 $$, ext {TeV}$$TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 50. | Measurement of b hadron lifetimes in pp collisions at $$sqrt{s} = 8$$s=8 $$, ext {Te} ext {V}$$TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 51. | Measurement of differential cross sections in the kinematic angular variable -* for inclusive Z boson production in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 52. | Measurement of normalized differential tt¯$$ mathrm{t}overline{mathrm{t}} $$ cross sections in the dilepton channel from pp collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 53. | Measurement of prompt and nonprompt charmonium suppression in $$ ext {PbPb}$$PbPb collisions at 5.02$$, ext {Te} ext {V}$$TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 54. | Measurement of the $$mathrm {Z}/gamma ^{*} ightarrow au au $$Z/γ∗→ττ cross section in pp collisions at $$sqrt{s} = 13 hbox { TeV}$$s=13TeV and validation of $$ au $$τ lepton analysis techniques. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 55. | Measurement of the groomed jet mass in PbPb and pp collisions at sNN=5.02$$ sqrt{s_{mathrm{NN}}}=5.02 $$ TeV.
[País não identificado] |
| 56. | Measurement of the inclusive tt¯$$ mathrm{t}overline{mathrm{t}} $$ cross section in pp collisions at s=5.02$$ sqrt{s}=5.02 $$ TeV using final states with at least one charged lepton.
[País não identificado] |
| 57. | Measurement of the inelastic proton-proton cross section at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 58. | Measurement of the top quark mass with lepton+jets final states using $$mathrm {p}$$p $$mathrm {p}$$p collisions at $$sqrt{s}=13, ext {TeV} $$s=13TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 59. | Measurement of the weak mixing angle using the forward-backward asymmetry of Drell-Yan events in $$mathrm {p}mathrm {p}$$pp collisions at 8$$, ext {TeV}$$TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 60. | Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 61. | Measurements of the $$mathrm {p}mathrm {p} ightarrow mathrm{Z}mathrm{Z}$$pp→ZZ production cross section and the $$mathrm{Z} ightarrow 4ell $$Z→4- branching fraction, and constraints on anomalous triple gauge couplings at $$sqrt{s} = 13, ext {TeV} $$s=13TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 62. | Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 63. | Modalmetric interferometer under disturbances: The effect of lateral offset between the single-mode and multimode fiber splice.
[Não foi possível obter dados do DOI] |
| 64. | Multi-material adhesive joints for automotive industry.
[País não identificado] |
| 65. | Novel polyaniline/manganese hexacyanoferrate nanoparticles on carbon fiber as binder-free electrode for flexible supercapacitors.
[País não identificado] |
| 66. | Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer.
[País não identificado] |
| 67. | On the Synthesis of Chocolate Flavonoids (Propanols, Butanals) in the Interstellar Medium.
[Não foi possível obter dados do DOI] |
| 68. | Photonic Generation and Transmission of Linearly Chirped Microwave Pulses with High TBWP by Self-Heterodyne Technique.
[País não identificado] |
| 69. | Practical splicing of poly-methyl-methacrylate plastic optical fibers.
[País não identificado] |
| 70. | Promising Hard Carbon Coatings on Cu Substrates: Corrosion and Tribological Performance with Theoretical Aspect.
[País não identificado] |
| 71. | Pseudorapidity and transverse momentum dependence of flow harmonics in p Pb and PbPb collisions.
[Não foi possível obter dados do DOI] |
| 72. | Pseudorapidity distributions of charged hadrons in proton-lead collisions at sNN=5.02$$ sqrt{s_{mathrm{NN}}}=5.02 $$ and 8.16 TeV.
[País não identificado] |
| 73. | Radiolysis of N2O:CO2 ice by heavy ions: simulation of cosmic ray effects.
[Não foi possível obter dados do DOI] |
| 74. | Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 75. | Search for a heavy resonance decaying into a Z boson and a vector boson in the νν¯qq¯$$ u overline{ u}mathrm{q}overline{mathrm{q}} $$ final state.
[País não identificado] |
| 76. | Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2-2q final states at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 77. | Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 78. | Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 79. | Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 80. | Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 81. | Search for additional neutral MSSM Higgs bosons in the τ τ final state in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 82. | Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 83. | Search for beyond the standard model Higgs bosons decaying into a bb¯$$ mathrm{b}overline{mathrm{b}} $$ pair in pp collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 84. | Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 85. | Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 86. | Search for dark matter produced in association with a Higgs boson decaying to γγ or τ +τ − at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 87. | Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 88. | Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 89. | Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 90. | Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 91. | Search for high-mass resonances in dilepton final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 92. | Search for high-mass resonances in final states with a lepton and missing transverse momentum at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 93. | Search for lepton flavour violating decays of the Higgs boson to μτ and eτ in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 94. | Search for lepton-flavor violating decays of heavy resonances and quantum black holes to eμ final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 95. | Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 96. | Search for narrow and broad dijet resonances in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV and constraints on dark matter mediators and other new particles.
[País não identificado] |
| 97. | Search for natural and split supersymmetry in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV in final states with jets and missing transverse momentum.
[País não identificado] |
| 98. | Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 99. | Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 100. | Search for new physics in dijet angular distributions using proton-proton collisions at $$sqrt{s}=13hbox {TeV}$$s=13TeV and constraints on dark matter and other models. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 101. | Search for new physics in events with a leptonically decaying Z boson and a large transverse momentum imbalance in proton-proton collisions at $$sqrt{s} $$s = 13$$, ext {TeV}$$TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 102. | Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at s=8$$ sqrt{s}=8 $$ and 13 TeV.
[País não identificado] |
| 103. | Search for resonant and nonresonant Higgs boson pair production in the bb¯-ν-ν$$ mathrm{b}overline{mathrm{b}}mathit{ell u ell u } $$ final state in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 104. | Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV.
[País não identificado] |
| 105. | Search for single production of vector-like quarks decaying to a b quark and a Higgs boson.
[País não identificado] |
| 106. | Search for standard model production of four top quarks with same-sign and multilepton final states in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$s=13TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 107. | Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 108. | Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 109. | Search for the decay of a Higgs boson in the --γ channel in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 110. | Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 111. | Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 112. | Search for tt¯H$$ mathrm{t}overline{mathrm{t}}mathrm{H} $$ production in the all-jet final state in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 113. | Search for vector-like T and B quark pairs in final states with leptons at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 114. | Search for ZZ resonances in the 2-2ν final state in proton-proton collisions at 13 TeV.
[País não identificado] |
| 115. | Search for Zγ resonances using leptonic and hadronic final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 116. | Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 117. | Strain rate dependence of adhesive joints for the automotive industry at low and high temperatures.
[Não foi possível obter dados do DOI] |
| 118. | Studies of $${mathrm {B}} ^{*}_{{mathrm {s}}2}(5840)^0 $$Bs2∗(5840)0 and $${mathrm {B}} _{{mathrm {s}}1}(5830)^0 $$Bs1(5830)0 mesons including the observation of the $${mathrm {B}} ^{*}_{{mathrm {s}}2}(5840)^0 ightarrow {mathrm {B}} ^0 mathrm {K} ^0_{mathrm {S}} $$Bs2∗(5840)0→B0KS0 decay in proton-proton collisions at $$sqrt{s}=8, ext {TeV} $$s=8TeV. EUROPEAN PHYSICAL JOURNAL C.
South Korea, Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 119. | Study of dijet events with a large rapidity gap between the two leading jets in pp collisions at $$sqrt{s}=7$$s=7 $$, ext {TeV}$$TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 120. | Superconductivity in Bi/Ni bilayer system: Clear role of superconducting phases found at Bi/Ni interface.
[País não identificado] |
| 121. | Vertical organic field effect transistor: on-off state definition related to ambipolar gate biasing. APPLIED PHYSICS.
[País não identificado] |
| 1. | A review on the temperature and moisture degradation of adhesive joints.
[Não foi possível obter dados do DOI] |
| 2. | A search for new phenomena in pp collisions at $$sqrt{s} = 13, ext {TeV} $$ s = 13 TeV in final states with missing transverse momentum and at least one jet using the $$alpha _{mathrm {T}}$$ α T variable.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 3. | A simple strategy to design broadband low power consumption distributed Raman amplifier.
[País não identificado] |
| 4. | Acoustic Sensor Self-Localization: Models and Recent Results.
[Não foi possível obter dados do DOI] |
| 5. | Analysis of the resonant layer effect in multilayer nanostructured optical waveguides. Optical Engineering (Bellingham.
[País não identificado] |
| 6. | Behavior of environmentally degraded epoxy adhesives as a function of temperature.
[Não foi possível obter dados do DOI] |
| 7. | Binder-free polyaniline interconnected metal hexacyanoferrates nanocomposites (Metal = Ni, Co) on carbon fibers for flexible supercapacitors.
[País não identificado] |
| 8. | Caracterização de um Transdutor de Pressão para Instrumentos Submarinos.
[Não foi possível obter dados do DOI] |
| 9. | Characterization of femtosecond-inscribed fiber Bragg gratings in the visible spectral region.
[País não identificado] |
| 10. | Charged-particle nuclear modification factors in PbPb and pPb collisions at sNN=5.02$$ sqrt{s_{mathrm{N};mathrm{N}}}=5.02 $$ TeV.
[País não identificado] |
| 11. | Debonding on command of multi-material adhesive joints.
[Não foi possível obter dados do DOI] |
| 12. | Decentralisation of power flow solution for facilitating active network management.
[Não foi possível obter dados do DOI] |
| 13. | Degradation of Adenine on the Martian Surface in the Presence of Perchlorates and Ionizing Radiation: A Reflectron Time-of-flight Mass Spectrometric Study.
[País não identificado] |
| 14. | Diamond-coated fiber Bragg grating through the hot filament chemical vapor process for chemical durability improvement.
[País não identificado] |
| 15. | Effect of material on the mechanical behaviour of adhesive joints for the automotive industry.
[Não foi possível obter dados do DOI] |
| 16. | Effects of postdeposition heat treatment on the structural and magnetic properties of CoFe 2 O 4 nanoparticles produced by pulsed laser deposition.
[Não foi possível obter dados do DOI] |
| 17. | Electrochemical synthesis and surface protection of polypyrrole-CeO2 nanocomposite coatings on AA2024 alloy.
[País não identificado] |
| 18. | Electron Radiolysis of Ammonium Perchlorate: A Reflectron Time-of-Flight Mass Spectrometric Study.
[Não foi possível obter dados do DOI] |
| 19. | Evidence for collectivity in pp collisions at the LHC.
[País não identificado] |
| 20. | Failure pressure analysis of composite repair system for wall loss defect of metallic pipelines.
[País não identificado] |
| 21. | Formation of Methylamine and Ethylamine in Extraterrestrial Ices and Their Role as Fundamental Building Blocks of Proteinogenic -amino Acids.
[País não identificado] |
| 22. | Inclusive search for supersymmetry using razor variables in p p collisions at s = 13 - -.
[Não foi possível obter dados do DOI] |
| 23. | Interface adhesion assessment of composite-to-metal bonded joints under salt spray conditions using peel tests.
[País não identificado] |
| 24. | Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV.
[País não identificado] |
| 25. | Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s=8$$ sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV.
[País não identificado] |
| 26. | Measurement of double-differential cross sections for top quark pair production in pp collisions at $$sqrt{s} = 8$$ s = 8 $$, ext {TeV}$$ TeV and impact on parton distribution functions.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 27. | Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s=8$$ sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings.
[País não identificado] |
| 28. | Measurement of inclusive jet cross sections in p p and PbPb collisions at s NN = 2.76.
[Não foi possível obter dados do DOI] |
| 29. | Measurement of prompt and nonprompt $$mathrm{J}/{psi }$$ J / ψ production in $$mathrm {p}mathrm {p}$$ p p and $$mathrm {p}mathrm {Pb}$$ p Pb collisions at $$sqrt{s_{mathrm {NN}}} =5.02, ext {TeV} $$.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 30. | Measurement of the $$mathrm{t}overline{mathrm{t}} $$ t t ¯ production cross section using events in the $$mathrm {e}mu $$ e μ final state in pp collisions at $$sqrt{s}=13, ext {TeV} $$ s =.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 31. | Measurement of the cross section for electroweak production of Z γ in association with two jets and constraints on anomalous quartic gauge couplings in proton-proton collisions at s = 8 TeV /.
[País não identificado] |
| 32. | Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 33. | Measurement of the mass difference between top quark and antiquark in pp collisions at s = 8 TeV.
[País não identificado] |
| 34. | Measurement of the production cross section of a Wboson in association with two b jets in pp collisions at $$sqrt{s} = 8{,mathrm{{TeV}}} $$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 35. | Measurement of the top quark mass using single top quark events in proton-proton collisions at $$sqrt{s}= 8$$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 36. | Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 37. | Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s=8$$ sqrt{s}=8 $$ TeV using H → WW decays.
[País não identificado] |
| 38. | Measurement of the WZ production cross section in pp collisions at.
[País não identificado] |
| 39. | Measurement of the WZ production cross section in pp collisions at $$sqrt{s} = 7$$ s = 7 and 8 $$, ext{TeV}$$ TeV and search for anomalous triple gauge couplings at $$sqrt{s} = 8, ext{TeV} $$ s =.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 40. | Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at s = 8.
[Não foi possível obter dados do DOI] |
| 41. | Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 42. | Measurements of jet charge with dijet events in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 43. | Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 44. | Measurements of the $$mathrm{t}overline{mathrm{t}}$$ t t ¯ production cross section in lepton+jets final states in pp collisions at 8 $$, ext {TeV}$$ TeV and ratio of 8 to 7 $$, ext {TeV}$$ TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 45. | Measurements of the charm jet cross section and nuclear modification factor in pPb collisions at.
[País não identificado] |
| 46. | Measurements of the indoor/outdoor atmospheric turbulence through optical triangulation method.
[País não identificado] |
| 47. | Mechanical stability of the CMS strip tracker measured with a laser alignment system.
[País não identificado] |
| 48. | Moisture and temperature degradation of double cantilever beam adhesive joints.
[Não foi possível obter dados do DOI] |
| 49. | Multiplicity and rapidity dependence of strange hadron production in pp, pPb, and PbPb collisions at the LHC.
[País não identificado] |
| 50. | Observation of Charge-Dependent Azimuthal Correlations in p − Pb Collisions and Its Implication for the Search for the Chiral Magnetic Effect.
[Não foi possível obter dados do DOI] |
| 51. | Observation of Y(1S) pair production in proton-proton collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 52. | On the Design of Conical Antennas for Broadband Impedance Matching Performance.
[Não foi possível obter dados do DOI] |
| 53. | On the Formation of the C H O Isomers Ethanol (C H OH) and Dimethyl Ether (CH OCH ) in Star-forming Regions.
[País não identificado] |
| 54. | Optical Fiber Bragg Grating Strain Sensor for Bone Stress Analysis in Bovine during Masticatory Movements.
[País não identificado] |
| 55. | Photochemistry of coronene in cosmic water ice analogs at different concentrations.
[País não identificado] |
| 56. | Principal-component analysis of two-particle azimuthal correlations in PbPb and p Pb collisions at CMS.
[Não foi possível obter dados do DOI] |
| 57. | Processing of N2O ice by fast ions: Implications on nitrogen chemistry in cold astrophysical environments.
[Não foi possível obter dados do DOI] |
| 58. | Pseudorapidity dependence of long-range two-particle correlations in p Pb collisions at s NN = 5.02.
[Não foi possível obter dados do DOI] |
| 59. | Relative Modification of Prompt ψ ( 2 S ) and J / ψ.
[Não foi possível obter dados do DOI] |
| 60. | Search for a heavy resonance decaying to a top quark and a vector-like top quark at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 61. | Search for a light pseudoscalar Higgs boson produced in association with bottom quarks in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 62. | Search for anomalous couplings in boosted W W / W Z.
[País não identificado] |
| 63. | Search for anomalous Wtb couplings and flavour-changing neutral currents in t-channel single top quark production in pp collisions at s=7$$ sqrt{s}=7 $$ and 8 TeV.
[País não identificado] |
| 64. | Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 65. | Search for associated production of dark matter with a Higgs boson decaying to bb¯$$ mathrm{b}overline{mathrm{b}} $$ or γγ at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 66. | Search for CP violation in tt¯$$ toverline{t} $$ production and decay in proton-proton collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 67. | Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at s = 8 - - TeV.
[Não foi possível obter dados do DOI] |
| 68. | Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 69. | Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at $$sqrt{s}= 13, ext{TeV} $$ s = 13 TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 70. | Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 71. | Search for dijet resonances in proton-proton collisions at s = 13 TeV and constraints on dark matter and other models.
[País não identificado] |
| 72. | Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 73. | Search for electroweak production of a vector-like quark decaying to a top quark and a Higgs boson using boosted topologies in fully hadronic final states.
[País não identificado] |
| 74. | Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 75. | Search for heavy gauge W - bosons in events with an energetic lepton and large missing transverse momentum at s = 13 TeV.
[País não identificado] |
| 76. | Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 77. | Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos, and b quarks.
[País não identificado] |
| 78. | Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 79. | Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at $$sqrt{s} = 13$$ s = 13 $$, ext {TeV}$$ TeV. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 80. | Search for high-mass diphoton resonances in proton-proton collisions at 13 TeV and combination with 8 TeV search.
[País não identificado] |
| 81. | Search for high-mass Z γ resonances in proton-proton collisions at and 13 TeV using jet substructure techniques.
[País não identificado] |
| 82. | Search for high-mass Zγ resonances in e+e−γ and μ + μ −γ final states in proton-proton collisions at s=8 $$ sqrt{s}=8 $$ and 13 TeV.
[País não identificado] |
| 83. | Search for massive resonances decaying into WW, WZ or ZZ bosons in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 84. | Search for narrow resonances in dilepton mass spectra in proton-proton collisions at s = 13 TeV and combination with 8 TeV data.
[País não identificado] |
| 85. | Search for new phenomena with the $$M_{mathrm {T2}}$$ M T 2 variable in the all-hadronic final state produced in proton-proton collisions at $$sqrt{s} = 13$$ s = 13 $$, ext {TeV}$$. EUROPEAN PHYSICAL JOURNAL C.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 86. | Search for new physics with dijet angular distributions in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 87. | Search for R -parity violating supersymmetry with displaced vertices in proton-proton collisions at s = 8 - -.
[Não foi possível obter dados do DOI] |
| 88. | Search for single production of a heavy vector-like T quark decaying to a Higgs boson and a top quark with a lepton and jets in the final state.
[País não identificado] |
| 89. | Search for single production of vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 90. | Search for standard model production of four top quarks in proton-proton collisions at.
[País não identificado] |
| 91. | Search for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 92. | Search for supersymmetry in events with photons and missing transverse energy in pp collisions at 13 TeV.
[País não identificado] |
| 93. | Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s=8$$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 94. | Search for top squark pair production in compressed-mass-spectrum scenarios in proton-proton collisions at s = 8 TeV using the α T variable.
[País não identificado] |
| 95. | Search for top squark pair production in pp collisions at s=13$$ sqrt{s}=13 $$ TeV using single lepton events.
[País não identificado] |
| 96. | Search for tt¯$$ mathrm{t}overline{mathrm{t}} $$ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at s=13$$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 97. | Searches for invisible decays of the Higgs boson in pp collisions at s$$ sqrt{s} $$ = 7, 8, and 13 TeV.
[País não identificado] |
| 98. | Searches for pair production of third-generation squarks in $$sqrt{s}=13$$ s = 13 $$, ext {TeV}$$ TeV pp collisions.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 99. | Strength and failure modes of single- L adhesive joints between aluminium and composites.
[País não identificado] |
| 100. | Suppression and azimuthal anisotropy of prompt and nonprompt $${mathrm{J}}/psi $$ J / ψ production in PbPb collisions at $$sqrt{{s_{_{ ext {NN}}}}} =2.76$$ s NN = 2.76.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 101. | Suppression of ϒ(1S), ϒ(2S), and ϒ(3S) quarkonium states in PbPb collisions at s NN = 2.76.
[País não identificado] |
| 102. | The CMS trigger system.
[País não identificado] |
| 103. | The force magnitude of a human bite measured at the molar intercuspidation using fiber Bragg gratings.
[País não identificado] |
| 104. | The Influence of Water on the Fracture Envelope of an Adhesive Joint.
[País não identificado] |
| 105. | Thermal characterization of Bragg gratings in polarization maintaining optical fibres: analysis of birefringence and regeneration.
[País não identificado] |
| 106. | Water assessment using ultra-weak bioluminescence.
[País não identificado] |
| 107. | Water Diffusion in Double Cantilever Beam Adhesive Joints.
[País não identificado] |
| 1. | A correction method for the analytical model in Raman amplifiers systems based on energy conservation assumption.
[País não identificado] |
| 2. | A simple and inexpensive optical power monitor for two visible wavelength WDM channels in plastic optical fibre links.
[País não identificado] |
| 3. | Affine Projection Subband Adaptive Filter With Low Computational Complexity.
[País não identificado] |
| 4. | An Evolutionary Method for Synthesizing Low-Sensitivity Lossless Matching Networks.
[País não identificado] |
| 5. | An in situ evaluation of the polymerization shrinkage, degree of conversion, and bond strength of resin cements used for luting fiber posts.
[País não identificado] |
| 6. | An updated review of adhesively bonded joints in composite materials.
[País não identificado] |
| 7. | Analysis of Strain and Temperature Induced by Acrylic Resins in Splinting Methods used for Dental Implant Impressions.
[País não identificado] |
| 8. | Angular analysis of the decay B 0 → K -0 μ + μ − from pp collisions at.
[País não identificado] |
| 9. | Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at s = 7 $$ sqrt{s}=7 $$ TeV.
[País não identificado] |
| 10. | Biogenic approaches using citrus extracts for the synthesis of metal nanoparticles: the role of flavonoids in gold reduction and stabilization.
Brazil, Uruguay. |
| 11. | Combined search for anomalous pseudoscalar HVV couplings in production and H → VV decay.
[País não identificado] |
| 12. | Correlations between jets and charged particles in PbPb and pp collisions at s N N = 2.76 $$ sqrt{s_{mathrm{NN}}}=2.76 $$ TeV.
[País não identificado] |
| 13. | Curvature and Vibration Sensing Based on Core Diameter Mismatch Structures.
[País não identificado] |
| 14. | DECA: distributed energy conservation algorithm for process reconstruction with bounded relative error in wireless sensor networks.
[País não identificado] |
| 15. | Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at sNN=2.76 $$ sqrt{s_{mathrm{N};mathrm{N}}}=2.76 $$ TeV.
[País não identificado] |
| 16. | Development and qualification of a new polymeric matrix laminated composite for pipe repair.
[País não identificado] |
| 17. | Effect of Low Temperature on Tensile Strength and Mode I Fracture Energy of a Room Temperature Vulcanizing Silicone Adhesive.
[País não identificado] |
| 18. | Effect of the size reduction on the bulk tensile and double cantilever beam specimens used in cohesive zone models. Proceedings of the Institution of Mechanical Engineers.
[Não foi possível obter dados do DOI] |
| 19. | Erratum to: Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 20. | Event generator tunes obtained from underlying event and multiparton scattering measurements.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 21. | Evidence for exclusive γγ → W + W − production and constraints on anomalous quartic gauge couplings in pp collisions at s = 7 $$ sqrt{s}=7 $$ and 8 TeV.
[País não identificado] |
| 22. | Experimental analysis of metal-composite repair of floating offshore units (FPSO).
[Não foi possível obter dados do DOI] |
| 23. | Formation of Nitrogen and Oxygen-Bearing Molecules from Radiolysis of Nitrous Oxide Ices - Implications for Solar System and Interstellar Ices.
France, Brazil. |
| 24. | Forward-backward asymmetry of Drell-Yan lepton pairs in pp collisions at $$sqrt{s} = 8$$ s = 8 $$,mathrm{TeV}$$ TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 25. | IN SITU DETECTION OF CHLORINE DIOXIDE (ClO ) IN THE RADIOLYSIS OF PERCHLORATES AND IMPLICATIONS FOR THE STABILITY OF ORGANICS ON MARS.
United States, Brazil. |
| 26. | In Situ Detection of Organics in the Comet 67P/Churyumov-Gerasimenko.
[País não identificado] |
| 27. | Influence of Adherend Surface Roughness on the Adhesive Bond Strength.
[País não identificado] |
| 28. | Infrared complex refractive index of astrophysical ices exposed to cosmic rays simulated in the laboratory.
[Não foi possível obter dados do DOI] |
| 29. | ION IRRADIATION OF ETHANE AND WATER MIXTURE ICE AT 15 K: IMPLICATIONS FOR THE SOLAR SYSTEM AND THE ISM.
[País não identificado] |
| 30. | Measurement of $$mathrm {t}overline{mathrm {t}}$$ t t ¯ production with additional jet activity, including $$mathrm {b}$$ b quark jets, in the dilepton decay channel using pp collisions at $$sqrt{s} = 8, ext {TeV} $$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 31. | Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at s = 7 $$ sqrt{s}=7 $$ and 8 TeV.
[País não identificado] |
| 32. | Measurement of differential cross sections for Higgs boson production in the diphoton decay channel in pp collisions at $$sqrt{s}=8, ext {TeV} $$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 33. | Measurement of dijet azimuthal decorrelation in ppcollisions at $$sqrt{s}=8,mathrm{TeV} $$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 34. | Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at s=8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 35. | Measurement of inclusive jet production and nuclear modifications in pPb collisions at $$sqrt{s_{_mathrm {NN}}} =5.02,mathrm{TeV} $$ s NN = 5.02 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 36. | Measurement of Long-Range Near-Side Two-Particle Angular Correlations in p p Collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 37. | Measurement of spin correlations in production using the matrix element method in the muon+jets final state in pp collisions at.
[País não identificado] |
| 38. | Measurement of the $$mathrm{t}overline{{mathrm{t}}}$$ t t ¯ production cross section in the all-jets final state in pp collisions at $$sqrt{s}=8$$ s = 8 $$, ext {TeV}$$ TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 39. | Measurement of the $${{mathrm{W} }^{+} }mathrm{W}^{-} $$ W + W - cross section in pp collisions at $$sqrt{s} = 8$$ s = 8 TeVand limits on anomalous gauge couplings. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 40. | Measurement of the charge asymmetry in top quark pair production in p p collisions at s = 8 - - TeV.
[Não foi possível obter dados do DOI] |
| 41. | Measurement of the CP-violating weak phase - s and the decay width difference -- s using the decay channel in pp collisions at.
[País não identificado] |
| 42. | Measurement of the differential cross section and charge asymmetry for inclusive $$mathrm {p}mathrm {p} ightarrow mathrm {W}^{pm }+X$$ p p → W ± + X production at $${sqrt{s}} = 8$$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 43. | Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in collisions at and 8TeV.
[Não foi possível obter dados do DOI] |
| 44. | Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$ s = 13 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 45. | Measurement of the inelastic cross section in proton-lead collisions at.
[País não identificado] |
| 46. | Measurement of the integrated and differential t t ¯ production cross sections for high- p.
[Não foi possível obter dados do DOI] |
| 47. | Measurement of the mass of the top quark in decays with a J/ψ meson in pp collisions at 8 TeV.
[País não identificado] |
| 48. | Measurement of the production cross section in pp collisions at and limits on anomalous ZZ γ and Z γγ trilinear gauge boson couplings.
[País não identificado] |
| 49. | Measurement of the t t ¯ $$ mathrm{t}overline{mathrm{t}} $$ production cross section in the eμ channel in proton-proton collisions at s = 7 $$ sqrt{s}=7 $$ and 8 TeV.
[País não identificado] |
| 50. | Measurement of the top quark mass using charged particles in p p collisions at s = 8 - -.
[Não foi possível obter dados do DOI] |
| 51. | Measurement of the top quark mass using proton-proton data at ( s ) = 7 and 8TeV.
[Não foi possível obter dados do DOI] |
| 52. | Measurement of the Top Quark Pair Production Cross Section in Proton-Proton Collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 53. | Measurement of the W boson helicity fractions in the decays of top quark pairs to lepton + jets final states produced in pp collisions at.
[País não identificado] |
| 54. | Measurement of the ZZ production cross section and Z→-+-−--+--− branching fraction in pp collisions at.
[País não identificado] |
| 55. | Measurement of top quark polarisation in t-channel single top quark production.
[País não identificado] |
| 56. | Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ sqrt{s_{mathrm{NN}}}=2.76 $$ TeV.
[País não identificado] |
| 57. | Measurements of charge asymmetry using dilepton final states in pp collisions at.
[País não identificado] |
| 58. | Measurements of t t ¯ spin correlations and top quark polarization using dilepton final states in p.
[Não foi possível obter dados do DOI] |
| 59. | Methods to increase the toughness of structural adhesives with micro particles: an overview with focus on cork particles.
[Não foi possível obter dados do DOI] |
| 60. | New sensor and non-contact geometrical survey for the vibrating wire technique.
[País não identificado] |
| 61. | Observation of top quark pairs produced in association with a vector boson in pp collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 62. | Phenomenological MSSM interpretation of CMS searches in pp collisions at s=7 $$ sqrt{s}=7 $$ and 8 TeV.
[País não identificado] |
| 63. | Photorefractive moiré-like patterns for the multifringe projection method in Fourier transform profilometry. Applied Optics (Cessou em 1989. Foi desdobrado em três: ISSN 1540-8973 Applied Optics. Information Processing, Applied Optics.
[País não identificado] |
| 64. | PMD Emulator based on PZTs attached to pieces of an Hi-Bi fiber.
[País não identificado] |
| 65. | Propagation Characteristics of Optical Long Period Fiber Gratings using Graphical Solution Methods.
[País não identificado] |
| 66. | Proposal of fault Prediction System for Underground Installations.
[País não identificado] |
| 67. | Robust Acoustic Self-Localization of Mobile Devices.
[País não identificado] |
| 68. | Search for a low-mass pseudoscalar Higgs boson produced in association with a pair in pp collisions at.
[País não identificado] |
| 69. | Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 70. | Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 71. | Search for anomalous single top quark production in association with a photon in pp collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 72. | Search for dark matter and unparticles produced in association with a Z boson in proton-proton collisions at s = 8 -.
[Não foi possível obter dados do DOI] |
| 73. | Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets.
[País não identificado] |
| 74. | Search for dark matter particles in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV using the razor variables.
[País não identificado] |
| 75. | Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 76. | Search for direct pair production of supersymmetric top quarks decaying to all-hadronic final states in pp collisions at $$sqrt{s} = 8; ext {TeV} $$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 77. | Search for excited leptons in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 78. | Search for heavy Majorana neutrinos in e±e±+ jets and e± μ ±+ jets events in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 79. | Search for heavy resonances decaying to two Higgs bosons in final states containing four b quarks.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 80. | Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width.
[País não identificado] |
| 81. | Search for lepton flavour violating decays of heavy resonances and quantum black holes to an $$mathrm {e}mu $$ e μ pair in proton-proton collisions at $$sqrt{s}=8~ ext {TeV} $$ s = 8 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 82. | Search for long-lived charged particles in proton-proton collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 83. | Search for massive WH resonances decaying into the $$ell u mathrm{b} overline{mathrm{b}} $$ - ν b b ¯ final state at $$sqrt{s}=8$$ s = 8 $$~ ext {TeV}$$ TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 84. | Search for Narrow Resonances Decaying to Dijets in Proton-Proton Collisions at s = 13 - - TeV.
[Não foi possível obter dados do DOI] |
| 85. | Search for Narrow Resonances in Dijet Final States at s = 8 - - TeV with the Novel CMS Technique of Data Scouting.
[Não foi possível obter dados do DOI] |
| 86. | Search for neutral MSSM Higgs bosons decaying to μ + μ − in pp collisions at.
[País não identificado] |
| 87. | Search for neutral resonances decaying into a Z boson and a pair of b jets or τ leptons.
[País não identificado] |
| 88. | Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s=13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 89. | Search for new physics in same-sign dilepton events in proton-proton collisions at $$sqrt{s} = 13, ext {TeV} $$ s = 13 TeV.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Ecuador, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 90. | Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ sqrt{s}=13 $$ TeV.
[País não identificado] |
| 91. | Search for pair production of first and second generation leptoquarks in proton-proton collisions at s = 8 - - TeV.
[Não foi possível obter dados do DOI] |
| 92. | Search for pair-produced vectorlike B quarks in proton-proton collisions at s = 8 - - TeV.
[Não foi possível obter dados do DOI] |
| 93. | Search for R-parity violating decays of a top squark in proton-proton collisions at.
[País não identificado] |
| 94. | Search for Resonant Production of High-Mass Photon Pairs in Proton-Proton Collisions at s = 8 and 13TeV.
[Não foi possível obter dados do DOI] |
| 95. | Search for s channel single top quark production in pp collisions at s = 7 $$ sqrt{s}=7 $$ and 8 TeV.
[País não identificado] |
| 96. | Search for single production of scalar leptoquarks in proton-proton collisions at s = 8 - - TeV.
[Não foi possível obter dados do DOI] |
| 97. | Search for supersymmetry in electroweak production with photons and large missing transverse energy in pp collisions at.
[País não identificado] |
| 98. | Search for supersymmetry in events with a photon, a lepton, and missing transverse momentum in pp collisions at.
[País não identificado] |
| 99. | Search for supersymmetry in events with soft leptons, low jet multiplicity, and missing transverse energy in proton-proton collisions at.
[País não identificado] |
| 100. | Search for supersymmetry in pp collisions at s = 13 $$ sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets.
[País não identificado] |
| 101. | Search for supersymmetry in the multijet and missing transverse momentum final state in pp collisions at 13 TeV.
[País não identificado] |
| 102. | Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 103. | Search for the production of an excited bottom quark decaying to tW in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 104. | Search for two Higgs bosons in final states containing two photons and two bottom quarks in proton-proton collisions at 8TeV.
[Não foi possível obter dados do DOI] |
| 105. | Search for vectorlike charge 2 / 3 - T quarks in proton-proton collisions at.
[Não foi possível obter dados do DOI] |
| 106. | Search for W - decaying to tau lepton and neutrino in proton-proton collisions at.
[País não identificado] |
| 107. | Search for W- → tb in proton-proton collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 108. | Searches for a heavy scalar boson H decaying to a pair of 125 GeV Higgs bosons hh or for a heavy pseudoscalar boson A decaying to Zh, in the final states with h → ττ.
[País não identificado] |
| 109. | Searches for R -parity-violating supersymmetry in p p collisions at s l.
[Não foi possível obter dados do DOI] |
| 110. | Studies of inclusive four-jet production with two b -tagged jets in proton-proton collisions at 7TeV.
[Não foi possível obter dados do DOI] |
| 111. | Study of B Meson Production in p + Pb Collisions at s N.
[Não foi possível obter dados do DOI] |
| 112. | Study of Z boson production in pPb collisions at.
[País não identificado] |
| 113. | Test methods for bond strength of glass fiber posts to dentin: a review.
[Não foi possível obter dados do DOI] |
| 114. | The effect of photo-anode surface morphology and gel-polymer electrolyte on dye-sensitized solar cells with natural dyes. Journal of Materials Science.
[País não identificado] |
| 115. | Transient analysis of l0-LMS and l0-NLMS algorithms.
[País não identificado] |
| 116. | Transverse momentum spectra of inclusive b jets in pPb collisions at.
[País não identificado] |
| 1. | A simple model for ice compaction data induced by low energy ion irradiation.
[País não identificado] |
| 2. | A Study on Microstructure Characteristics of TEPs-modified Adhesives.
[Não foi possível obter dados do DOI] |
| 3. | Adhesive Joints for Low and High Temperature Use: An Overview.
[Não foi possível obter dados do DOI] |
| 4. | Adhesive Selection for Single Lap Bonded Joints: Experimentation and Advanced Techniques for Strength Prediction.
[Não foi possível obter dados do DOI] |
| 5. | Adhesive thickness effects of a ductile adhesive by optical measurement techniques.
[País não identificado] |
| 6. | Advanced techniques for estimation of the tensile fracture toughness of adhesive joints.
Italy, Brazil. |
| 7. | Bent optical fiber taper for refractive index measurements with tunable sensitivity.
[Não foi possível obter dados do DOI] |
| 8. | Branch-cut algorithm for optical phase unwrapping.
[País não identificado] |
| 9. | Compaction of porous ices rich in water by swift heavy ions. Icarus (New York, N.Y.
[País não identificado] |
| 10. | Comparative Failure Assessment of Single and Double Lap Joints with Varying Adhesive Systems.
[Não foi possível obter dados do DOI] |
| 11. | Comparison of the Z/γ ∗ + jets to γ + jets cross sections in pp collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 12. | Constraints on parton distribution functions and extraction of the strong coupling constant from the inclusive jet cross section in pp collisions at $$sqrt{s} = 7$$ s = 7 $$, ext {TeV}$$ TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 13. | Constraints on the pMSSM, AMSB model and on other models from the search for long-lived charged particles in proton-proton collisions at $$sqrt{s} =8, ext {TeV} $$ s = 8 TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 14. | Constraints on the spin-parity and anomalous H V V couplings of the Higgs boson in proton collisions at 7 and 8TeV. Physical Review.
[Não foi possível obter dados do DOI] |
| 15. | Controlled and compact first- and second-order polarization mode dispersion emulator.
[Não foi possível obter dados do DOI] |
| 16. | Debonding on command of adhesive joints for the automotive industry.
[País não identificado] |
| 17. | Development of a SCADA system for a Free Electron Laser operation.
[Não foi possível obter dados do DOI] |
| 18. | Differential cross section measurements for the production of a W boson in association with jets in proton?proton collisions at s**(1/2)= 7 TeV. Physics Letters.
[País não identificado] |
| 19. | Digital holographic moiré-like patterns and an application to Fourier transform profilometry.
[País não identificado] |
| 20. | Distributions of topological observables in inclusive three- and four-jet events in pp collisions at $$sqrt{s} = 7$$ s = 7 $$, ext {TeV}$$ TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 21. | Effect of surface roughness using different adherend materials on the adhesive bond strength.
[País não identificado] |
| 22. | Effects on nitrogen-acetone ice induced by energetic heavy ion collisions. Journal of Physics.
[País não identificado] |
| 23. | Erratum to: Measurement of jet multiplicity distributions in $$mathrm {t}overline{mathrm {t}}$$ t t ¯ production in pp collisions at $$sqrt{s} = 7, ext {TeV} $$ s = 7 TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 24. | Erratum to: Search for new physics in events with same-sign dileptons and jets in pp collisions at s $$ sqrt{s} $$ = 8 TeV.
[País não identificado] |
| 25. | Etched FBG written in multimode fibers: sensing characteristics and applications in the liquid fuels sector.
[País não identificado] |
| 26. | Evidence for Collective Multiparticle Correlations in p − Pb Collisions.
[Não foi possível obter dados do DOI] |
| 27. | Evidence for transverse-momentum- and pseudorapidity-dependent event-plane fluctuations in PbPb and p Pb collisions. Physical Review. C.
[Não foi possível obter dados do DOI] |
| 28. | Fast wavelength conversion to generate 560 nm fluorescence for data transmission in polymer optical fibres.
[Não foi possível obter dados do DOI] |
| 29. | Fiber Loop Mirror Sensors Interrogated and Multiplexed by OTDR.
[País não identificado] |
| 30. | Fiber optic displacement sensor based on a double-reflecting OTDR technique.
[Não foi possível obter dados do DOI] |
| 31. | Fibre Bragg Gratings, towards a Better Thermal Stability at High Temperatures.
[País não identificado] |
| 32. | In Vitro and In Situ Fiber Bragg Grating Sensor Analysis of Two Dental Resin Cements.
[País não identificado] |
| 33. | In Vivo Pattern Classification of Ingestive Behavior in Ruminants Using FBG Sensors and Machine Learning.
[País não identificado] |
| 34. | Limits on the Higgs boson lifetime and width from its decay to four charged leptons. Physical Review.
[Não foi possível obter dados do DOI] |
| 35. | Low cost electronic beam tilting of microstrip antennas by the use of tunable parasites.
[Não foi possível obter dados do DOI] |
| 36. | Measurement of and Prompt Double-Differential Cross Sections in Collisions at.
[Não foi possível obter dados do DOI] |
| 37. | Measurement of diffractive dissociation cross sections in p p collisions at s = 7 -. Physical Review.
[Não foi possível obter dados do DOI] |
| 38. | Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at $$sqrt{s}=8, ext {TeV}$$ s = 8 TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 39. | Measurement of the differential cross section for top quark pair production in pp collisions at $$sqrt{s} = 8, ext {TeV} $$ s = 8 TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 40. | Measurement of the inclusive 3-jet production differential cross section in proton-proton collisions at 7 TeVand determination of the strong coupling constant in the TeVrange. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 41. | Measurement of the pp→ZZ production cross section and constraints on anomalous triple gauge couplings in four-lepton final states at s**(1/2)=8 TeV. Physics Letters.
[País não identificado] |
| 42. | Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at s = 2.76 $$ sqrt{s}=2.76 $$ TeV.
[País não identificado] |
| 43. | Measurement of the W boson helicity in events with a single reconstructed top quark in pp collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 44. | Measurement of the Zγ production cross section in pp collisions at 8 TeV and search for anomalous triple gauge boson couplings.
[País não identificado] |
| 45. | Measurements of differential and double-differential Drell-Yan cross sections in proton-proton collisions at $$sqrt{s} = 8$$ s = 8 $$, ext {TeV}$$ TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 46. | Measurements of jet multiplicity and differential production cross sections of Z+jetsl. Physical Review.
[Não foi possível obter dados do DOI] |
| 47. | Measurements of the $$mathrm{Z}$$ Z $$mathrm{Z}$$ Z production cross sections in the $$2mathrm{l} 2 u $$ 2 l 2 ν channel in proton-proton collisions at $$sqrt{s} = 7$$ s = 7 and $$8~mathrm{TeV} $$ 8 TeV and combined constraints on triple gauge couplings. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 48. | Non-disturbing optical power monitor for links in the visible spectrum using a polymer optical fibre.
[País não identificado] |
| 49. | Normalized Subband Adaptive Filtering Algorithm With Reduced Computational Complexity.
[País não identificado] |
| 50. | Novel Optical Current Sensor for Metering and Protection in High Power Applications.
[Não foi possível obter dados do DOI] |
| 51. | Nuclear effects on the transverse momentum spectra of charged particles in pPb collisions at $$sqrt{s_{_mathrm {NN}}} =5.02$$ s NN = 5.02 $$, ext {TeV}$$ TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 52. | Numerical Modeling of Magnetic Devices for a Free Electron Laser.
[Não foi possível obter dados do DOI] |
| 53. | Observation of the rare Bs0 →µ+µ− decay from the combined analysis of CMS and LHCb data.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Saudi Arabia, Spain, Oman, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Romania, Qatar, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt, Sri Lanka. |
| 54. | Performance of photon reconstruction and identification with the CMS detector in protonproton collisions at vs=8TeV.
[País não identificado] |
| 55. | Performance of the CMS missing transverse momentum reconstruction in pp data at √ s = 8 TeV.
[País não identificado] |
| 56. | Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 $$, ext {TeV}$$ TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 57. | Production of leading charged particles and leading charged-particle jets at small transverse momenta in p p collisions at s = 8 . Physical Review.
[Não foi possível obter dados do DOI] |
| 58. | Proposal of fault Prediction System for Underground Installations. Measurement (London.
[País não identificado] |
| 59. | Radiation effects in astrophysical ices. Journal of Physics.
[País não identificado] |
| 60. | Radiolysis of Nitrogen and Water Ice Mixture by fast ions: Implications for Kuiper Belt Objects.
[País não identificado] |
| 61. | Redes de Bragg utilizadas para mensuração da contração de polimerização de duas resinas acrílicas na moldagem aberta de prótese sobre implantes.
[País não identificado] |
| 62. | Search for a charged Higgs boson in pp collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 63. | Search for a Higgs boson in the mass range from 145 to 1000 GeV decaying to a pair of W or Z bosons.
[País não identificado] |
| 64. | Search for a light charged Higgs boson decaying to c s ¯ $$ mathrm{c}overline{mathrm{s}} $$ in pp collisions at s = 8 $$ sqrt{s}=8 $$ TeV.
[País não identificado] |
| 65. | Search for a standard model Higgs boson produced in association with a top-quark pair and decaying to bottom quarks using a matrix element method. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |
| 66. | Search for dark matter, extra dimensions, and unparticles in monojet events in proton-proton collisions at $$sqrt{s} = 8$$ s = 8 $$,{mathrm{TeV}},$$ TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece. |
| 67. | Search for decays of stopped long-lived particles produced in proton-proton collisions at $$sqrt{s}= 8, ext {TeV} $$ s = 8 TeV. European Physical Journal.
Turkey, France, Finland, United States, Portugal, Malaysia, Ireland, Italy, Thailand, Georgia, Estonia, Colombia, Taiwan, Cyprus, Hungary, Mexico, Serbia, United Kingdom, Lithuania, Spain, New Zealand, Pakistan, India, Czech Republic, China, Armenia, Ukraine, Russia, Bulgaria, Austria, Brazil, Belarus, Iran, Belgium, Croatia, Switzerland, Germany, Poland, Greece, Egypt. |