ScholarWorks@Korea University: Hong, Byungsik

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Hong, Byungsik (홍병식)

College of Science (Department of Physics)

Research Area: 핵반응, 중이온 충돌, 핵구조, Nuclear Reaction, Heavy Ion Collisions, Nuclear Structure

Tel 02-3290-3105
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CMS:252||HadronHadron scattering (experiments):194||Physics:179||HadronHadron Scattering:164||Beyond Standard Model:87||Supersymmetry:64||Higgs physics:58||Top physics:49||Higgs:39||Resistiveplate chambers:29||Jets:27||QCD:21||Heavyion collision:20||Gaseous detectors:20||LHC:19||Particle and resonance production:17||Dark matter:16||Performance of High Energy Physics Detectors:16||Top quark:14||Jet physics:13||Higgs Physics:11||Muon spectrometers:11||B physics:11||Large detectorsystems performance:11||Top Physics:10||Exotica:10||Large detector systems for particle and astroparticle physics:10||Particle tracking detectors:9||Jet substructure:9||Heavy ions:9||Quark gluon plasma:8||LAMPS:8||RAON:8||Heavy ion:8||Photon production:8||protonproton scattering:8||BSM:8||Electroweak:7||Top:7||Lepton production:7||Cross section:7||Diboson:7||Particle tracking detectors (Gaseous detectors):7||Particle identification methods:7||SUSY:7||HadronHadron scattering:7||Calorimeters:6||Forward physics:6||Pattern recognition, cluster finding, calibration and fitting methods:6||VBS:6||Flow:6||Exotics:6||Higgs boson:6||Heavy flavor:6||Tau Physics:6||Jet:5||QGP:5||Frontend electronics for detector readout:5||Upsilon:5||MSSM:5||Nuclear symmetry energy:5||GEANT4:5||Computing:5||NMSSM:5||Particle correlations and fluctuations:5||pPb:5||Heavy ion collisions:5||B2G:5||PHENIX:5||Quarkonium:5||Electroweak interaction:5||Resonances:5||Heavy Ions:5||Heavy Ion Experiments:5||Trigger detectors:5||CMS experiment:5||Photons:4||W ':4||Equation of state:4||Dimuons:4||Extra dimensions:4||vectorlike quarks:4||SM:4||Muons:4||Graviton:4||Photon:4||Software:4||Flavour Changing Neutral Currents:4||Muon:4||Calorimeter methods:4||Z boson:4||Neutron detector:4||Resistive plate chambers:4||Tau:4||Relativistic heavy ion physics:4||Missing Transverse Energy studies:3||aQGC:3||ZZ:3||CP Violation:3||Symmetry energy:3||collectivity:3||Standard model:3||Particle tracking detectors (Solidstate detectors):3||Dijet:3||Pattern recognition:3||Si microstrip and pad detectors:3||UPC:3||Quark Gluon Plasma:3||Heavy quark production:3||Hadrons:3||Leptoquarks:3||Z ':3||Vector Boson Production:3||Detector alignment and calibration methods (lasers, sources, particlebeams):3||Neutron beam:3||Resonance:3||Leptons:3||Dilepton:3||Ridge:3||Standard model physics:3||quarkgluon plasma:3||Radioactive ion beam:3||Scintillation fiber:3||Quarkonium production:3||2HDM:3||Radiationhard detectors:3||Spectra:3||Collectivity:3||Dose verification:3||Jet quenching:3||Diphoton:3||Proton therapy:2||heavy ion:2||Strong coupling constant:2||VH:2||Dileptons:2||Quarkonium polarization:2||CP violation:2||Top quark mass:2||Diboson resonances:2||W boson:2||Lifetime:2||direct photons:2||Large Hadron Collider:2||Neutron star:2||Gaseous ionization detector:2||Aging effect:2||Bottomonium:2||Quarkonia:2||Vector boson:2||tau:2||PbPb:2||small systems:2||Data acquisition circuits:2||Quarkgluon plasma:2||Z:2||Materials for gaseous detectors:2||HeavyIon Collision:2||Excited quarks:2||SMP:2||Search:2||RPC:2||Leptonflavourviolation:2||Low missing transverse energy:2||Dimuon:2||Heavyions:2||Trigger concepts and systems (hardware and software):2||Longlived particles:2||Radiation calculations:2||RCNP:2||small system:2||Time projection chamber:2||Elliptic flow:2||Combination:2||Hadronic:2||Charge asymmetry:2||GMSB:2||Fasttiming measurement:2||TPC:2||Gas electron multiplier:2||Resistive plate chamber:2||Radion:2||Black holes:2||PDF:2||Dielectron:2||top squark:2||collective flow:2||Inverse kinematics:2||Spin:2||J/psi:2||flow:2||Bphysics:2||Electrons:2||iRPC:2||Top Squark:2||Experimental results:2||Substructure:2||Detector design and construction technologies and materials:2||Proton cyclotrons:2||VBF:2||MET:2||Vectorlike quarks:2||Heavyflavor:2||Tprime:2||Heavy neutrino:2||cluster finding:2||calibration and fitting methods:2||Charm physics:2||heavy flavor:2||Compact Muon Solenoid:2||Correlation:2||Small Systems:2||Cherenkov detectors:1||CKM matrix:1||Disappearing tracks:1||Riemann fitting:1||Flavor spectroscopy:1||Nuclear modification factor:1||Renormalization:1||Gaugemediated supersymmetry:1||Hidden sector:1||BSM Higgs physics:1||NaI(Tl) scintillator:1||Strangeness:1||Nuclear structure:1||Spectroscopic study:1||Alpha scattering:1||Chirallike pair band:1||Simulation:1||Particlebeam profiles:1||Beam monitor:1||Rate capability:1||Rare isotope:1||pi0:1||Proton accelerator:1||Differential cross sections:1||Quarkonium suppression:1||Elliptic Flow:1||Prompt J/psi:1||Ultraperipheral collisions:1||Shadowing:1||Observation:1||EXO:1||extra dimensions:1||Matrix element method:1||Taus:1||diHiggs:1||3jet mass:1||W plus jets:1||Stop:1||Strong:1||Constant:1||Exotic quarkonia:1||Inelastic cross section:1||Asymmetry:1||Simulation methods and programs:1||Toplike:1||Event shapes:1||Electromagnetic fields:1||Gammarays:1||Detectors:1||Particle detectors:1||5.02 TeV:1||Lepton Production:1||γray spectroscopy:1||LaBr3(ce):1||KHALA:1||Resistive Plate Chambers:1||Detector performance:1||Data reduction methods:1||Extra Higgs boson:1||QPG:1||SCINFUL:1||B Physics:1||Time reference:1||Time Projection Chamber:1||Heavy baryon:1||Lightbylight:1||Models and simulations:1||small/large collision systems:1||chargedhadron multiplicities:1||quarkonia:1||dileptons:1||Scattering length:1||Isomer:1||Inbeam gammaray spectroscopy:1||Quantum Chromodynamics:1||Commissioning:1||Drip line:1||Trigger:1||Hadron beam:1||SiCsI:1||Bragg distribution:1||Bragg peak:1||Currentmode electronics:1||K0 cross section:1||Gamma irradiation:1||Neutron irradiation:1||Muon trigger:1||CME:1||correlations:1||Vector boson fusion:1||B0 decays:1||Diffraction:1||Four leptons:1||Higgs tagging:1||Top quark cross section:1||BSM searches:1||Spin0:1||Anomalous couplings:1||Helicity:1||13 TeV:1||Gamma detectors (scintillators, CZT, HPG, HgI etc):1||Rparityviolation:1||Field theories in dimensions other than four:1||Detector modelling and simulations I (interaction of radiation with matter, interaction of photons with matter, interaction of hadrons with matter, etc):1||Longitudinal:1||Polarized:1||pulse shape discrimination (PSD):1||Scintillators:1||Interpolation:1||Hybrid detectors:1||VectorLike Quarks:1||Legacy reprocessing:1||X6 silicon detector:1||Data acquisition:1||IDATEN:1||Photonproton:1||Detector aging:1||VLL:1||Yukawa couplings:1||Hadron physics:1||Lambda(c) baryons:1||WW production:1||Single top:1||Model independent:1||HVT:1||Open heavyflavor:1||Azimuthal angle:1||LaBr3(Ce) scintillator:1||sPHENIX:1||backward physics:1||Twoparticle angular correlations:1||QCD critical point:1||neutron star merger:1||quark gluon plasma:1||S pi RIT TPC:1||Gaselectron multiplier:1||Plastic scintillator:1||APV25:1||Doseverification measurement:1||Scintillation fibers:1||Highpower laser:1||Lutetium Yttrium Oxyorthosilicate:1||Neutron calorimeter:1||high density QCD:1||Muon trigger detector:1||Energy Loss Mechanism:1||Particle Correlation:1||Missing energy:1||diHiggs boson resonance:1||Excited top quark:1||alphas:1||Top quark physics:1||Photons and missing transverse energy:1||Semileptonic:1||Radial flow:1||QCD medium effects:1||Monophoton:1||btagging:1||Resonance production:1||Electroweak corrections:1||Branching fraction:1||Leptoquark:1||HardonHadron Scattering:1||Threejet resonances:1||W bosons:1||ADD:1||Gravitons:1||Statistics:1||Multileptons:1||Performance of High Energy Physics detectors:1||Oscillations:1||Neutrons:1||Alignment:1||nuclear cluster:1||Ne18(a,p)Na21:1||Active target time projection chamber:1||TexAT_v2:1||HH:1||Selfcoupling:1||Gas detectors:1||Background:1||Muon system:1||RPC backend electronics:1||FPGA:1||Composite fermions:1||Vectorlike leptons:1||Transport model:1||Backend electronics:1||Time resolution:1||Radiationhard electronics:1||Scintillators, scintillation and light emission processes (solid, gas and liquid scintillators):1||Heavyflavor spectroscopy:1||Xenonxenon:1||B meson:1||Cs133:1||sPHENIX beam test:1||initial state:1||multiparticle correlation:1||Nuclear scattering:1||RI beam production:1||Nuclear phase diagram:1||Timing detectors:1||FOPI:1||SIS:1||CMS RPC muon trigger:1||Charmonia:1||cumulant:1||Hadron spectroscopy:1||2HDM+S:1||Dmeson:1||Cross sections:1||Heavy flavour:1||Beyond two generations:1||boson pair production:1||Parton energy loss:1||Ultraperipheral collisions:1||VLQ:1||Bottomonia:1||Narrow resonances:1||Hidden sectors:1||Boosted topology:1||Dijets:1||Top squark:1||Width:1||Quark:1||Coupling:1||Event shape:1||Total cross section:1||J/psi Mesons:1||FCNC Interaction:1||EWK:1||DAQ:1||SC:1||Scalar:1||Rare decays psi root:1||Particle Correlations and Fluctuations:1||Beyond the Standard Model:1||RPC link system:1||Heavy leptons:1||Upgrade:1||Muon detection:1||Adjustment:1||Beauty baryon:1||b physics:1||WZ:1||forward physics:1||ELPH:1||Hyperonnucleon interaction:1||Muon triggers:1||Iodine:1||Fluctuation:1||Trigger detector performance:1||Timeofflight detector:1||Lambda:1||Constantfraction discriminator:1||Rare Isotope:1||Symmetry Energy:1||Prompt gammaray:1||harmonic analysis:1||suppression:1||Density dependence:1||Time of flight:1||fragmentation function:1||Invisible decays:1||Y:1||Prompt psi(2S):1||pp collisions:1||Heavy flavour spectroscopy:1||Exotic decays:1||Extradimensions:1||Charmtagging:1||J/Psi:1||Exotic spin:1||Dalitz decay:1||Protonproton:1||New scalar:1||KK graviton:1||Relativistic heavyion collisions:1||CKM:1||harmonic flow:1||Pair:1||Forward energy:1||Searches:1||Detector modelling and simulations I (interaction of radiation with matter, interaction of photons with matter, interaction of hadrons with matter,etc):1||Particle physics:1||Small systems:1||Heavy radioactive isotope collisions:1||Antisymmetrized molecular dynamics:1||NE213:1||TP:1||RI beam:1||Rareisotope beam:1||Machine Learning:1||Jet Physics:1||Large detector systems for particle and astropartide physics:1||Trigger algorithms:1||S pi RIT:1||GENFIT:1||2HD+1S:1||</bold>:1||Instrumentation and methods for timeofflight (TOF) spectroscopy:1||T1044:1||neutron star:1||Magnetic field:1||Detector control systems (detector and experiment monitoring and slowcontrol systems, architecture, hardware, algorithms, databases):1||Timeprojection chamber:1||Particle identification:1||resistiveplate chambers:1||muon spectrometers:1||Mesytec:1||Birksmodel kB parameter:1||Nuclear equation of state:1||Multigap RPCs:1||Chargeintegration mode:1||RHIC:1||Line scanning:1||Resistive Plate Chamber (RPC):1||Zprime:1||WW:1||NonGaussian flow fluctuations:1||ZZjets:1||bJets:1||Open heavyflavour:1||HighpT:1||RandallSundrum:1||Heavy resonance:1||Rare B decays:1||Anomalous coupling:1||Z boson production:1||BPhysics:1||Pwave states:1||Longrange:1||Highmultiplicity:1||Properties:1||Jet shapes:1||Btag:1||New phenomena:1||Fourth generation:1||RPV:1||Eventbyevent fluctuation:1||Shape:1||Search for new physics:1||Detector:1||explosive stellar environments:1||Gaugino:1||LaBr<sub>3</sub>(Ce) scintillator detector:1||RPC slow control emulator:1||EventbyEvent fluctuation:1||Harmonic Flow:1||Cascade model:1||Neutron detection efficiency:1||Light response functions:1||Vector boson scattering:1||Tracking:1||Vertex reconstruction:1||Photoproduction:1||Rare decays<bold>:1||Overall mechanics design (support structures and materials, vibration analysis etc):1||Dark photon:1||quark matter 2018:1||Relativistic heavyion collision:1||Parity:1||Relativistic heavy ion collision:1||Rare isotope beams:1||MIPS:1||Isospin:1||MonteCarlo simulation:1||HPL:1||KoRIA:1||jet:1||Hadron therapy:1||Absorbed dose:1||pion induced reaction:1||Proton spin:1||Heavyion physics:1||photoproduction:1||psi(2S):1||Heavy Flavor:1||system size:1||b hadrons:1||Suppression:1||Exo:1||Multijets:1||W ' decays:1||Z boson differential cross section:1||RS1:1||Tau leptons:1||Electron:1||AlphaS:1||Stealth:1||Baryon number:1||Heavy ion physics:1||Mass:1||Longlived:1||Displaced:1||W and Z pair production:1||Top pair:1||MSUGRA:1||Detector modelling and simulations (interaction of radiation with matter, interaction of photons with matter, interaction of hadrons with matter, etc):1||Charm:1||vectorlike quarks:1||Minimum bias:1||neutron detection:1||neutrongamma discrimination:1||Bars:1||BSM particles:1||Tracker:1||HipPy:1||BEE:1||resonant scattering:1||thicktarget method in inverse kinematics:1||W pairs:1||Bbtautau:1||Collective Flow:1||Heavy Quark Production:1||Monitoring tools:1||Forward Physics:1||Top quarks:1||Relativistic Heavy Ion Physics:1||RAVE:1||Measurement:1||nPDF:1||Multiplicity:1||Dynamic range:1||Charged Higgs:1||New light boson:1||MC generators:1||Scintillation detector:1||heavy ion collision:1||hadrons:1||Partial wave analysis:1||Alpha cluster:1||Chirality:1||KOBRA:1||Gas systems and purification:1||Silicon:1||Voltagethreshold discriminator:1||Equation of State:1||Directed flow:1||Muon trigger detectors:1||heavyion collisions:1||Isoscaling parameter:1||Beam profiles:1||Korea rareisotope accelerator:1||Prompt gammas:1||reaction plane:1||Compact Muon Solenoid (CMS):1||BNL:1||Higgs boson coupling modifiers:1||Eventbyevent elliptic flow:1||Unfolding:1||Nuclear Modification Factor:1||Production:1||Event Shape Engineering:1||Lightbylight scattering:1||Proton:1||Compressed:1||Electroweak production:1||pp:1||pPb collisions:1||Contact interactions:1||Lepton:1||Correlations:1||Technicolor:1||Tracking efficiency:1||KaluzaKlein:1||DrellYan:1||Multijets ratio:1||Flavor physics:1||Cluster productions:1||Wgamma resonances:1||MillePedeII:1||alphacluster structure:1||energy level properties:1||Boosted jets:1||HLLHC:1||14O(a,p)17F:1||TexAT:1||Electroweakino:1||Bottom Quarks:1||Beauty quark:1||b jets:1||CMS phase2 upgrade:1||v2:1||Neutron detection array:1||

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