NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = M.Rho Found 92 matches. 2020MA48 Phys.Rev.Lett. 125, 142501 (2020) Quenched gA in Nuclei and Emergent Scale Symmetry in Baryonic Matter NUCLEAR STRUCTURE 100Sn; analyzed available data; deduced an analogy in the way scale symmetry manifests in a nuclear medium to the continuity from the unitarity limit at low density (in light nuclei) to the dilaton limit at high density (in compact stars).
doi: 10.1103/PhysRevLett.125.142501
2019LI30 Phys.Rev. C 99, 055808 (2019) Topology change and nuclear symmetry energy in compact-star matter
doi: 10.1103/PhysRevC.99.055808
2019MA75 Phys.Rev.Lett. 123, 172301 (2019) Y.-L.Ma, M.A.Nowak, M.Rho, I.Zahed Baryon as a Quantum Hall Droplet and the Quark-Hadron Duality
doi: 10.1103/PhysRevLett.123.172301
2018LI40 Chin.Phys.C 42, 094102 (2018) Nuclear axial currents from scale-chiral effective field theory
doi: 10.1088/1674-1137/42/9/094102
2018LI55 Phys.Rev. C 98, 044318 (2018) Nonquenching of gA in nuclei, Landau-Migdal fixed-point theory, and emergence of scale symmetry in dense baryonic matter
doi: 10.1103/PhysRevC.98.044318
2017RH01 Int.J.Mod.Phys. E26, 1740023 (2017) In search of a pristine signal for (scale-)chiral symmetry in nuclei
doi: 10.1142/S0218301317400237
2016PA22 Phys.Rev. C 93, 055203 (2016) W.-G.Paeng, T.T.S.Kuo, H.K.Lee, M.Rho Scale-invariant hidden local symmetry, topology change, and dense baryonic matter
doi: 10.1103/PhysRevC.93.055203
2015PA04 Phys.Rev. C 91, 015801 (2015) Kaon condensation in baryonic Fermi liquid at high density
doi: 10.1103/PhysRevC.91.015801
2014LE05 Eur.Phys.J. A 50, 14 (2014) Topology change and tensor forces for the EoS of dense baryonic matter
doi: 10.1140/epja/i2014-14014-1
2014LE29 Phys.Rev. C 90, 045201 (2014) Nuclear symmetry energy with strangeness in heavy-ion collisions
doi: 10.1103/PhysRevC.90.045201
2014RH01 Nucl.Phys. A928, 144 (2014) A new topological "twist" to BR scaling
doi: 10.1016/j.nuclphysa.2014.03.003
2013DO05 Phys.Rev. C 87, 054332 (2013) H.Dong, T.T.S.Kuo, H.K.Lee, R.Machleidt, M.Rho Half-Skyrmions and the equation of state for compact-star matter
doi: 10.1103/PhysRevC.87.054332
2013LE12 Int.J.Mod.Phys. E22, 1330005 (2013) Flavor symmetry and topology change in nuclear symmetry energy for compact stars
doi: 10.1142/S0218301313300051
2011KI20 Phys.Rev. C 84, 035810 (2011) Dense stellar matter with strange quark matter driven by kaon condensation
doi: 10.1103/PhysRevC.84.035810
2011LE08 Phys.Rev. C 83, 025206 (2011); Erratum Phys.Rev. C 84, 059902 (2011) Half-Skyrmions, tensor forces, and symmetry energy in cold dense matter
doi: 10.1103/PhysRevC.83.025206
2010LE24 Nucl.Phys. A844, 80c (2010) Dilatons for dense hadronic matter
doi: 10.1016/j.nuclphysa.2010.05.018
2010PA06 Phys.Rev. C 81, 035203 (2010) Kaons in dense half-Skyrmion matter
doi: 10.1103/PhysRevC.81.035203
2009LE32 Nucl.Phys. A829, 76 (2009) Dilatons in hidden local symmetry for hadrons in dense matter
doi: 10.1016/j.nuclphysa.2009.08.002
2008PA16 Nucl.Phys. A807, 28 (2008) The role of the dilaton in dense skyrmion matter
doi: 10.1016/j.nuclphysa.2008.03.015
2007BR03 Phys.Rep. 439, 161 (2007) G.E.Brown, J.W.Holt, C.-H.Lee, M.Rho Vector manifestation and matter formed in relativistic heavy-ion processes
doi: 10.1016/j.physrep.2006.12.002
2007KI14 Nucl.Phys. A792, 249 (2007) Y.Kim, K.Kubodera, D.-P.Min, F.Myhrer, M.Rho The effect of kaon condensation on quark-antiquark condensate in dense matter
doi: 10.1016/j.nuclphysa.2007.05.005
2006BR02 Phys.Rev.Lett. 96, 062303 (2006) G.E.Brown, C.-H.Lee, H.-J.Park, M.Rho Strangeness Condensation by Expanding about the Fixed Point of the Harada-Yamawaki Vector Manifestation
doi: 10.1103/PhysRevLett.96.062303
2006BR08 Phys.Rev.Lett. 96, 132301 (2006) Matter Formed at the BNL Relativistic Heavy Ion Collider
doi: 10.1103/PhysRevLett.96.132301
2006BR16 Phys.Rev. C 74, 024906 (2006) Vector manifestation of hidden local symmetry, hadronic freedom, and the STAR ρ0/π- ratio NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed meson yield ratio; deduced hadronic freedom. Vector manifestation fixed-point scenario.
doi: 10.1103/PhysRevC.74.024906
2006PA45 Nucl.Phys. A774, 889 (2006) H.-J.Park, C.-H.Lee, G.E.Brown, M.Rho The Problem of Mass: Mesonic Bound States Above Tc NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV/nucleon; calculated neutral ρ-meson to negative pion ratio. Bielefeld lattice gauge simulation. Comparison with data.
doi: 10.1016/j.nuclphysa.2006.06.159
2005BR01 Nucl.Phys. A747, 530 (2005) Chemical equilibration in relativistic heavy ion collisions
doi: 10.1016/j.nuclphysa.2004.09.108
2004BR07 Phys.Rep. 391, 353 (2004) G.E.Brown, L.Grandchamp, C.-H.Lee, M.Rho Nature of the chiral restoration transition in QCD
doi: 10.1016/j.physrep.2003.10.009
2004BR22 Phys.Rep. 396, 1 (2004) Double decimation and sliding vacua in the nuclear many-body system
doi: 10.1016/j.physrep.2004.02.002
2004BR32 Nucl.Phys. A740, 171 (2004) G.E.Brown, C.-H.Lee, M.Rho, E.Shuryak The (q-bar)q bound states and instanton molecules at T ≥ Tc
doi: 10.1016/j.nuclphysa.2004.04.116
2004BR37 J.Phys.(London) G30, S1275 (2004) G.E.Brown, C.-H.Lee, M.Rho, E.Shuryak The instanton molecule liquid and 'sticky molasses' above Tc
doi: 10.1088/0954-3899/30/8/107
2004BR39 Phys.Rep. 398, 301 (2004) Matching the QCD and hadron sectors and medium-dependent meson masses; hadronization in relativistic heavy ion collisions
doi: 10.1016/j.physrep.2004.05.006
2004HA03 Nucl.Phys. A730, 379 (2004) M.Harada, Y.Kim, M.Rho, C.Sasaki The pion velocity at chiral restoration and the vector manifestation
doi: 10.1016/j.nuclphysa.2003.10.021
2004LE30 Nucl.Phys. A741, 161 (2004) H.-J.Lee, B-Y.Park, M.Rho, V.Vento The pion velocity in dense skyrmion matter
doi: 10.1016/j.nuclphysa.2004.06.010
2004PA14 Nucl.Phys. A736, 129 (2004) Vector mesons and dense skyrmion matter
doi: 10.1016/j.nuclphysa.2004.02.131
2003HA34 Nucl.Phys. A727, 437 (2003) M.Harada, Y.Kim, M.Rho, C.Sasaki Effective degrees of freedom at chiral restoration and the vector manifestation in HLS theory
doi: 10.1016/j.nuclphysa.2003.07.014
2003LE13 Nucl.Phys. A723, 427 (2003) H.-J.Lee, B.-Y.Park, D.-P.Min, M.Rho, V.Vento A unified approach to high density: pion fluctuations in skyrmion matter
doi: 10.1016/S0375-9474(03)01452-0
2003LE17 Nucl.Phys. A726, 69 (2003) H.-J.Lee, B.-Y.Park, M.Rho, V.Vento Sliding vacua in dense skyrmion matter
doi: 10.1016/S0375-9474(03)01626-9
2003PA19 Phys.Rev. C 67, 055206 (2003) T.-S.Park, L.E.Marcucci, R.Schiavilla, M.Viviani, A.Kievsky, S.Rosati, K.Kubodera, D.-P.Min, M.Rho Parameter-free effective field theory calculation for the solar proton-fusion and hep processes NUCLEAR REACTIONS 1H, 3He(p, e+ν), E=low; calculated threshold astrophysical S-factors, dependence on cutoff parameters. Effective field theory.
doi: 10.1103/PhysRevC.67.055206
2003RH01 J.Korean Phys.Soc. 43, S63 (2003) QCD and Nuclei
2002BR09 Nucl.Phys. A698, 483c (2002) Broad Band Equilibration of Strangeness NUCLEAR REACTIONS Ni(Ni, X), E ≈ 1.8 GeV/nucleon; analyzed particle yield ratios; deduced kaon production equilibration features, in-medium effects.
doi: 10.1016/S0375-9474(01)01409-9
2002BR18 Phys.Rep. 363, 85 (2002) On the Manifestation of Chiral Symmetry in Nuclei and Dense Nuclear Matter
doi: 10.1016/S0370-1573(01)00084-9
2002PA37 Nucl.Phys. A707, 381 (2002) B.-Y.Park, D.-P.Min, M.Rho, V.Vento Atiyah-Manton Approach to Skyrmion Matter
doi: 10.1016/S0375-9474(02)00963-6
2001BR26 Nucl.Phys. A690, 184c (2001) Strangeness Equilibration at GSI Energies
doi: 10.1016/S0375-9474(01)00942-3
2001PA17 Nucl.Phys. A684, 101c (2001) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho Effective Field Theory for Nuclei: Confronting fundamental questions in astrophysics
doi: 10.1016/S0375-9474(01)00494-8
2001RH01 Yad.Fiz. 64, No 4, 696 (2001); Phys.Atomic Nuclei 64, 637 (2001) Effective Field Theories, Landau-Migdal Fermi Liquid Theory, and Effective Chiral Lagrangians for Nuclear Matter
doi: 10.1134/1.1368222
2000KI19 Phys.Rev. C62, 015202 (2000) Y.Kim, R.Rapp, G.E.Brown, M.Rho Schematic Model for ρ-a1 Mixing at Finite Density and In-Medium Effective Lagrangian
doi: 10.1103/PhysRevC.62.015202
2000PA03 Phys.Lett. 472B, 232 (2000) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho Effective Field Theory Approach to n(pol) + p(pol) → d + γ at Threshold NUCLEAR REACTIONS 1H(polarized n, γ), E not given; calculated polarization observables. Effective field theory, polarized target.
doi: 10.1016/S0370-2693(99)01438-0
2000RH01 Nucl.Phys. A676, 273 (2000) M.Rho, E.Shuryak, A.Wirzba, I.Zahed Generalized Mesons in Dense QCD
doi: 10.1016/S0375-9474(00)00190-1
1999FR09 Phys.Rev. C59, 3357 (1999) Scaling of Chiral Lagrangians and Landau Fermi Liquid Theory for Dense Hadronic Matter
doi: 10.1103/PhysRevC.59.3357
1999LA29 Nucl.Phys. A660, 475 (1999) Quark Condensation, Induced Symmetry Breaking and Color Superconductivity at High Density
doi: 10.1016/S0375-9474(99)00417-0
1999LE39 Nucl.Phys. A657, 75 (1999) H.-J.Lee, D.-P.Min, B.-Y.Park, M.Rho, V.Vento The Proton Spin in the Chiral Bag Model: Casimir contributions and Cheshire Cat principle NUCLEAR STRUCTURE 1H; calculated flavor singlet axial charge. Chiral bag model, Cheshire Cat principle.
doi: 10.1016/S0375-9474(99)00320-6
1999PA05 Nucl.Phys. A646, 83 (1999) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho The Power of Effective Field Theories in Nuclei: The deuteron, NN scattering and electroweak processes NUCLEAR REACTIONS 1H(p, e+), (n, γ), E=low; calculated phase shifts, matrix elements; deduced pion role, cut-off parameter. Effective field theory.
doi: 10.1016/S0375-9474(98)00614-9
1998BR26 Acta Phys.Pol. B29, 2309 (1998) G.E.Brown, G.Q.Li, R.Rapp, M.Rho, J.Wambach Medium Dependence of the Vector-Meson Mass: Dynamical and/or Brown-Rho Scaling ? NUCLEAR REACTIONS 197Au(Pb, X), E=158 GeV/nucleon; calculated dilepton mass spectra; deduced dilepton production mechanism features. Dynamical and Brown-Rho scaling compared.
1998PA21 Phys.Rev. C58, R637 (1998) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho Effective Field Theory for Low-Energy Two-Nucleon Systems NUCLEAR REACTIONS 1H(n, γ), E(cm) < 220 MeV; calculated phase shift, M1 transition amplitude; deduced little cutoff dependence. Effective field theory.
doi: 10.1103/PhysRevC.58.R637
1998RH01 Acta Phys.Pol. B29, 2297 (1998) Effective Field Theories for Nuclei and Dense Matter
1998SO10 Phys.Lett. 424B, 226 (1998) Thermodynamic Properties of Effective Chiral Lagrangians with Brown-Rho Scaling
doi: 10.1016/S0370-2693(98)00232-9
1997LA25 Nucl.Phys. A622, 620 (1997) K.Langfeld, H.Reinhardt, M.Rho A New State of Hadronic Matter at High Density
doi: 10.1016/S0375-9474(97)00364-3
1997RH01 Nucl.Phys. A622, 538 (1997) Color Anomaly and Flavor-Singlet Axial Charge of the Proton in the Chiral Bag: The Cheshire Cat revisited
doi: 10.1016/S0375-9474(97)00362-X
1997SO20 Phys.Rev. C56, 2244 (1997) C.Song, G.E.Brown, D.-P.Min, M.Rho Fluctuations in ' Brown-Rho Scaled ' Chiral Lagrangians
doi: 10.1103/PhysRevC.56.2244
1997WA11 Nucl.Phys. A617, 449 (1997) Effective Kaon Mass in Dense Baryonic Matter: Role of correlations
doi: 10.1016/S0375-9474(97)00020-1
1996BR03 Nucl.Phys. A596, 503 (1996) From Chiral Mean Field to Walecka Mean Field and Kaon Condensation
doi: 10.1016/0375-9474(95)00420-3
1996BR28 Nucl.Phys. A609, 519 (1996) A Mean-Field Theory of the Chiral Phase Transition
doi: 10.1016/S0375-9474(96)00295-3
1996FR13 Nucl.Phys. A606, 303 (1996) From Chiral Lagrangians to Landau-Fermi Liquid Theory of Nuclear Matter
doi: 10.1016/0375-9474(96)00215-1
1996LA02 Nucl.Phys. A596, 451 (1996) Quark Confinement in a Constituent Quark Model
doi: 10.1016/0375-9474(95)00410-6
1996LE10 Nucl.Phys. A602, 334 (1996) The Role of Λ(1405) in Kaon-Proton Interactions NUCLEAR REACTIONS 1H(K-, X), E ≈ threshold; calculated leading order contributions. 1H(K+, K+), E at ≤ 300 MeV/c; calculated S-wave phase shifts; deduced Λ(1405) role. Heavy-baryon chiral perturbation theory.
doi: 10.1016/0375-9474(96)00086-3
1996PA04 Nucl.Phys. A596, 515 (1996) Chiral Lagrangian Approach to Exchange Vector Currents in Nuclei NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated σ. Chiral Lagrangian approach, exchange vector currents.
doi: 10.1016/0375-9474(95)00406-8
1995BR25 Nucl.Phys. A590, 527c (1995) Chiral Restoration in Hot Matter
doi: 10.1016/0375-9474(95)00270-B
1995KI15 Phys.Rev. C52, R1184 (1995) Finite-Temperature Corrections in the Dilated Chiral Quark Model
doi: 10.1103/PhysRevC.52.R1184
1995LE09 Nucl.Phys. A585, 401 (1995) C.-H.Lee, G.E.Brown, D.-P.Min, M.Rho An Effective Chiral Lagrangian Approach to Kaon-Nuclear Interactions. Kaonic Atom and Kaon Condensation
doi: 10.1016/0375-9474(94)00623-U
1995LE18 Phys.Lett. 348B, 290 (1995) A Renormalization Group Flow Analysis of Meson Condensations in Dense Matter
doi: 10.1016/0370-2693(95)00171-G
1995PA38 Phys.Rev.Lett. 74, 4153 (1995) Radiative Neutron-Proton Capture in Effective Chiral Lagrangians NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated total capture σ(E). Chiral perturbation theory.
doi: 10.1103/PhysRevLett.74.4153
1994BR04 Nucl.Phys. A567, 937 (1994) G.E.Brown, C.-H.Lee, M.Rho, V.Thorsson From Kaon-Nuclear Interactions to Kaon Condensation
doi: 10.1016/0375-9474(94)90335-2
1994LE13 Phys.Lett. 326B, 14 (1994) C.-H.Lee, H.Jung, D.-P.Min, M.Rho Kaon-Nucleon Scattering from Chiral Lagrangians NUCLEAR REACTIONS 1H, 1n(K-, K-), E=high; calculated s-wave amplitude vs E. Scattering from chiral Lagrangians.
doi: 10.1016/0370-2693(94)91185-1
1994LE21 Phys.Lett. 335B, 266 (1994) Kaon Condensation in ' Nuclear Star ' Matter
doi: 10.1016/0370-2693(94)90348-4
1993BR04 Nucl.Phys. A553, 705c (1993) Vector Meson Masses in the Nuclear Medium NUCLEAR REACTIONS 4,3He(e, e'p), E not given; compiled, reviewed response function data, analyses; deduced in-medium vector meson masses implications.
doi: 10.1016/0375-9474(93)90684-P
1993SO07 Nucl.Phys. A556, 355 (1993) In-Medium Behaviour of Vector Mesons and the Longitudinal and Transverse Response Functions in (e, e'p) Reactions NUCLEAR REACTIONS 4,3He, 40Ca(e, e'p), E not given; calculated longitudinal to transverse response function ratio vs momentum transfer; deduced in-medium vector meson behaviour role in quenching.
doi: 10.1016/0375-9474(93)90366-6
1991KU18 Phys.Rev.Lett. 67, 3479 (1991) Axial-Charge Transitions in Heavy Nuclei and In-Medium Effective Chiral Lagrangians NUCLEAR STRUCTURE A=205-212; analyzed first forbidden β-decay related axial-charge matrix enhancement; deduced hadron scaling evidence. Effective Lagrangian, chiral, scale QCD invariances.
doi: 10.1103/PhysRevLett.67.3479
1991OH04 Nucl.Phys. A534, 493 (1991) Y.Oh, D.-P.Min, M.Rho, N.N.Scoccola Massive-Quark Baryons as Skyrmions Magnetic Moments NUCLEAR STRUCTURE 1n, 1H; calculated μ. Skyrmion description.
doi: 10.1016/0375-9474(91)90458-I
1990BR06 Phys.Lett. 237B, 3 (1990) In-Medium Stiffening of the Nucleon-Nucleon Spin-Isospin Interaction NUCLEAR STRUCTURE 208Pb; calculated longitudinal, transverse response function ratio. In-medium nucleon-nucleon interaction stiffening.
doi: 10.1016/0370-2693(90)90450-K
1990PA23 Nucl.Phys. A517, 561 (1990) Strange Component in the Magnetic Moment of the Proton NUCLEAR STRUCTURE 1H; calculated strange component in μ. Chiral hyperbag, SU(3) collective coordinate quantization.
doi: 10.1016/0375-9474(90)90218-B
1989PA04 Phys.Lett. 220B, 7 (1989) Neutron-Proton Mass Difference in the Chiral Hyperbag NUCLEAR STRUCTURE 1H, 1n; calculated mass difference. Chiral hyperbag model.
doi: 10.1016/0370-2693(89)90003-8
1986BR10 Nucl.Phys. A454, 669 (1986) Phenomenological Delineation of the Quark-Gluon Structure from Nucleon Electromagnetic Form Factors NUCLEAR STRUCTURE 1H; calculated charge form factor. Topological chiral models.
doi: 10.1016/0375-9474(86)90112-0
1981BR27 Nucl.Phys. A372, 397 (1981) The Giant Gamow-Teller Resonance NUCLEAR STRUCTURE 208Pb; calculated Gamow-Teller resonance strength distribution. Boson exchange model, isobar coupling.
doi: 10.1016/0375-9474(81)90043-9
1980BR06 Nucl.Phys. A338, 269 (1980) Velocity Dependence of the Nucleon-Nucleon Interaction, Exchange Currents and Enhancement of the Dipole Sum Rule in Nuclei NUCLEAR STRUCTURE 208Pb; calculated enhancement of dipole sum rule in GDR region. Velocity dependent nucleon-nucleon interaction, exchange currents.
doi: 10.1016/0375-9474(80)90033-0
1976DA11 Nucl.Phys. A264, 507 (1976) Weak Interactions in Deuterons: Exchange Currents and Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(p, π+d); calculated interaction.
doi: 10.1016/0375-9474(76)90420-6
1976GI03 J.Phys.(Paris) 37, 189 (1976) Two Quasi-Particle Excitations with Particle-Hole Core Polarization in Even-Even Single Closed Shell Nuclei NUCLEAR STRUCTURE 86Kr, 88Sr, 90Zr, 92Mo, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 114,116,118,120,122,124Sn, 198,200,202,204,206Pb; calculated B(λ).
doi: 10.1051/jphys:01976003703018900
1974CH28 Phys.Rev. C10, 344 (1974) Deuteron Electromagnetic Structure at Large Momentum Transfer NUCLEAR STRUCTURE 2H; calculated form factors.
doi: 10.1103/PhysRevC.10.344
1972SH34 Phys.Lett. 42B, 45 (1972) Exotic Muon Capture in Nuclei and Lepton Conservation
doi: 10.1016/0370-2693(72)90711-3
1971CH05 Nucl.Phys. A163, 1 (1971); Erratum Nucl.Phys. A212, 628 (1973) Meson Exchange Currents in Nuclear Weak and Electromagnetic Interactions RADIOACTIVITY 3H; calculated Gamow-Teller matrix element. 3H, 3He; calculated exchange effects in isoscalar, isovector magnetic moments.
doi: 10.1016/0375-9474(71)90520-3
1968GI08 Phys.Letters 27B, 483 (1968) V.Gillet, B.Giraud, J.Picard, M.Rho Collective Properties of N = 50 Isotones
doi: 10.1016/0370-2693(68)90200-1
1965RH01 Nucl.Phys. 65, 497 (1965) Quasi-Particle Interactions in Even Spherical Nuclei NUCLEAR STRUCTURE N=82; calculated single particle energies, levels, B(E2). 140Ce level calculated g. 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd calculated B(E2).
doi: 10.1016/0029-5582(65)90013-1
1964MA17 Phys.Rev. 134, B1196 (1964) R.D.Macfarlane, J.O.Rasmussen, M.Rho Theoretical Calculations of Properties of Rare-Earth Alpha Emitters NUCLEAR STRUCTURE 154Yb, 150Dy, 148Gd, 152Er, 144Nd, 146Sm; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B1196
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