ScholarWorks@SUNGKYUNKWAN UNIVERSITY: YU, IN TAE

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YU, IN TAE (유인태)

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CMS:228||HadronHadron scattering (experiments):187||Physics:155||HadronHadron Scattering:136||Beyond Standard Model:84||Supersymmetry:61||Higgs physics:55||Top physics:41||Jets:29||Higgs:28||QCD:18||Particle and resonance production:15||LHC:14||Top quark:14||Dark matter:12||Higgs Physics:12||Jet physics:12||Top Physics:11||B physics:10||Performance of High Energy Physics Detectors:10||Exotica:10||Heavyion collision:10||Large detector systems for particle and astroparticle physics:10||Large detectorsystems performance:9||Electroweak:9||Tau Physics:8||Particle identification methods:8||Lepton production:7||Photon production:7||Quark gluon plasma:7||Cross section:7||SUSY:7||Heavy ions:7||Diboson:7||Heavy ion:7||Higgs boson:6||BSM:6||Hadronhadron scattering:6||Resonances:6||VBS:6||Top:6||vectorlike quarks:5||Jet:5||Flow:5||Heavy flavor:5||Exotics:5||Z boson:5||B2G:5||Photon:5||Jet substructure:5||SM:5||Muon spectrometers:4||Quarkonium:4||Neutrino detectors:4||Computing:4||Electroweak interaction:4||Calorimeters:4||Forward physics:4||calibration and fitting methods:4||cluster finding:4||Particle correlations and fluctuations:4||Particle tracking detectors:4||Dilepton:4||Standard model:4||Pattern recognition:4||Pattern recognition, cluster finding, calibration and fitting methods:4||pPb:4||protonproton scattering:4||Tau:4||CMS experiment:4||Muon:4||NMSSM:4||Ridge:4||Graviton:3||protonproton scattering:3||Standard model physics:3||Rare decays:3||Dijets:3||Relativistic heavy ion physics:3||Dijet:3||MSSM:3||Software:3||Leptons:3||Heavy Ions:3||Dimuons:3||aQGC:3||Top quark mass:3||W &apos:3||Quarkonia:3||ZZ:3||Resistive plate chambers:3||Resonance:3||RPC:3||Vector Boson Production:3||Vector boson:3||Jet quenching:3||Leptoquarks:3||Heavy ion collisions:3||UPC:3||Muons:3||CP Violation:3||Search:3||Upsilon:3||top squark:3||Gaseous detectors:3||Flavour Changing Neutral Currents:3||Quark Gluon Plasma:3||Photons:3||Vector boson scattering:2||QGP:2||Diphoton:2||Quarkonium suppression:2||Correlation:2||GMSB:2||Correlations:2||2HDM:2||CDF:2||Radion:2||Bottomonium:2||Electrons:2||SC:2||Lifetime:2||Liquid detectors:2||HLLHC:2||Longlived particles:2||Longrange:2||Low missing transverse energy:2||Single top:2||Small Systems:2||MET:2||Spectra:2||Charmtagging:2||DAQ:2||Dark Matter:2||Strong coupling constant:2||Substructure:2||TP:2||Missing Transverse Energy studies:2||Tevatron:2||Cherenkov detectors:2||Heavy Ion Experiments:2||Top Squark:2||Collectivity:2||Combination:2||Tprime:2||Trigger detectors:2||VBF:2||VH:2||Heavy neutrino:2||Jet Physics:2||VectorLike Quarks:2||Vectorlike quarks:2||Heavy quark production:2||BEE:2||W boson:2||Heavyflavor:2||Diboson resonances:2||Dielectron:2||Heavyions:2||Water Cherenkov detector:2||Calorimeter methods:2||Z &apos:2||PDF:2||Experimental results:2||Extra dimensions:2||Particle Correlations and Fluctuations:2||b jets:2||Highmultiplicity:2||collectivity:2||Particle tracking detectors (Gaseous detectors):2||flow:2||iRPC:2||PbPb:2||Dileptons:2||Flavor physics:2||Dimuon:2||:2||Massive gluon:1||Measurement:1||MillePedeII:1||Minimum bias:1||Missing energy:1||Missing transverse momentum:1||Model independent:1||Monitoring tools:1||Multijets ratio:1||Multileptons:1||Multiplicity:1||Multivariate techniques:1||Muon system:1||Muon triggers:1||Narrow resonances:1||Neutrino:1||Neutrino–antineutrino oscillation:1||Neutrino Detectors and Telescopes (experiments):1||Neutrino detector:1||Neutrino oscillation:1||Neutrino source from decay at rest:1||Neutron:1||Neutron tagging:1||New light boson:1||New phenomena:1||NonGaussian flow fluctuations:1||Nuclear Modification Factor:1||Nuclear modification factor:1||Observation:1||Open heavyflavor:1||Open heavyflavour:1||Oscillation:1||Oscillations:1||PDFs:1||Pair:1||Particle Correlation:1||Particle and Resonance Production:1||Particle tracking detectors (Solidstate detectors):1||Parton energy loss:1||Pattern recogn:1||Photonproton:1||Photons and missing transverse energy:1||Photoproduction:1||Polarized:1||Production:1||Prompt J/psi:1||Prompt psi(2S):1||Properties:1||Proton:1||Pulseshape discrimination:1||Quantum chromodynamics:1||Quark:1||Quarkgluon plasma:1||Quarkonium polarization:1||Quarkonium production:1||Rparityviola:1||RENO:1||RPC backend electronics:1||RPC link system:1||RPC slow control emulator:1||RPV:1||RS1:1||Radial flow:1||Randall–Sundrum:1||Rapidity d sigma/dy:1||Rare B decays:1||Reactor antineutrino:1||Relativistic heavyion collisions:1||Renormalization:1||Resistive Plate Chambers:1||Resonance production:1||SMP:1||Scalar:1||Scintillators, scintillation and light emission processes (solid, gas and liquid scintillators):1||Search for new physics:1||Searches:1||Selfcoupling:1||Semileptonic:1||Shadowing:1||Si microstrip and pad detectors:1||Silicon sensor:1||Simulation:1||Small systems:1||Solar neutrino:1||Spin0:1||Stealth:1||Sterile neutrino:1||Stop:1||Strong:1||Suppression:1||Tau leptons:1||Technicolor:1||Third generation:1||Threejet resonances:1||Top pair:1||Top quark physics:1||Top resonances:1||Top squark:1||Toplike:1||Tracker:1||Tracking ef:1||Trigger algorithms:1||Trigger concepts and systems (hardware and software):1||Trijet:1||Ultraperipheral collisions:1||Ultraperipheral collisions:1||Unfolding:1||VLQ:1||Vector boson fusion:1||W ':1||W and Z pair production:1||W bosons:1||W pairs:1||W plus jets:1||W' search:1||W+jets:1||WW:1||WW production:1||WZ:1||Wgamma resonances:1||Width:1||Xenonxenon:1||Y:1||Z:1||Z ':1||Z boson production:1||ZZjets:1||Zprime:1||aTGC:1||alphas:1||b hadrons:1||b physics:1||boson pair production:1||correlations:1||cumulant:1||diHiggs:1||diHiggs boson resonance:1||diphoton:1||elementary particle jets:1||extra dimensions:1||heavy ion:1||highenergy elementary particle interactions:1||nPDF:1||photoproduction:1||pp:1||pp collisions:1||protonproton inclusive interactions:1||psi(2S):1||quarkgluon plasma:1||small system:1||sparticle production:1||system size:1||tZq:1||tau:1||vectorlike quarks:1||2HD+1S:1||2HDM + S:1||3D structures:1||3jet mass:1||5.02 TeV:1||ADD:1||Acrylic:1||Aging:1||Alignment:1||Allhadronic channe:1||AlphaS:1||AlphaT:1||Anomalous coupling:1||Asymmetry:1||Azimuthal angle:1||B meson:1||B mesons:1||Bphysics:1||B0 decays:1||BPH:1||BSM Higgs physics:1||BSM particles:1||BSM searches:1||Background:1||Baryon number:1||Bbtautau:1||Beauty baryon:1||Beauty quark:1||Beyond the Standard Model:1||Beyond two generations:1||Black holes:1||Boosted jets:1||Boosted top:1||Boosted topology:1||Bottom Quarks:1||Bottomonia:1||C03:1||C04:1||C12:1||C32:1||C43:1||CKM:1||CKM matrix:1||CME:1||CMS phase2 upgrade:1||CP violation:1||Charge asymmetry:1||Charge ratio:1||Charged Higgs:1||Charm:1||Charm physics:1||Charm quark:1||Charmonia:1||Collective Flow:1||Compact Muon Solenoid:1||Composite fermions:1||Compressed:1||Constant:1||Contact interactions:1||Convolutional neural network:1||Cosmic rays:1||Coupling:1||Cross sections:1||Crosssection:1||Dmeson:1||D0:1||Dark photon:1||Data Processing:1||Data acquisition circuits:1||Deep learning:1||Detector:1||Detector aging:1||Detector alignment and calibration methods (lasers, sources, particlebeams):1||Detector modelling and simulations I (interaction of radiation with matter, interaction of photons with matter, interaction of hadrons with matter, etc):1||Detector performance:1||Differential cross sections:1||Diffraction:1||Disappearing tracks:1||Doublemask:1||DrellYan:1||EWK:1||EXO:1||Electromagnetic fields:1||Electron:1||Electron antineutrinos:1||Electroweak corrections:1||Electroweak production:1||Electroweakino:1||Elliptic Flow:1||Elliptic flow:1||Energy Loss Mechanism:1||Event Shape Engineering:1||Event shape:1||Event shapes:1||Eventbyevent elliptic flow:1||Eventbyevent fluctuation:1||Ex:1||Excited quar:1||Excited quarks:1||Excited top quark:1||Exo:1||Exotic decays:1||Exotic quarkonia:1||Exotic spin:1||Extradimensions:1||FCNC Interaction:1||FPGA:1||Fast neutron:1||Flavor spectroscopy:1||Forward Physics:1||Four leptons:1||Fourth g:1||GEM:1||Gadolinium:1||Gamma detectors (scintillators, CZT, HPG, HgI etc):1||Gamma detectors (scintillators, CZT, HPGe, HgI etc):1||Gas detectors:1||Gaugemediated supersymmetry:1||Gaugino:1||Global features:1||HH:1||HVT:1||Hadron spectroscopy:1||HadronHadron Scattering Op:1||Hadronic:1||Hadronization:1||Hadrons:1||HardonHadron Scattering:1||Heavy Flavor:1||Heavy Quark Production:1||Heavy baryon:1||Heavy flavour:1||Heavy flavour spectroscopy:1||Heavy leptons:1||Heavy resonance:1||HeavyIon Collision:1||Heavyflavor spectroscopy:1||Heavyflavour:1||Heavyion physics:1||Helicity:1||Hidden sector:1||Higgs boson coupling modifiers:1||Higgs boson searches:1||Higgs tagging:1||High luminosity LHC:1||HighpT:1||HipPy:1||Inelastic cross section:1||Inverse beta decay:1||Invisible decays:1||J/Psi:1||J/psi:1||J/psi Mesons:1||Jet energy:1||Jet resolution:1||KK graviton:1||KaluzaKlein:1||Lambda(c) baryons:1||Larg:1||Large Hadron Collider:1||Large detector systems for particle and astropartide physics:1||Leakage test:1||Legacy reprocessing:1||Lepton:1||Lepton Production:1||Lepton momentum spectrum:1||Leptoquark:1||Lightbylight:1||Lightbylight scattering:1||Liquid scintillator:1||Longlived:1||Longitudinal:1||MC generators:1||MSUGRA:1||Machine Learning:1||Mass:1||

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(03063) 25-2, SUNGKYUNKWAN-RO, JONGNO-GU, SEOUL, KOREAsamsunglib@skku.edu

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