NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = L.S.Kisslinger Found 52 matches. 2014KI02 Phys.Rev. C 89, 024914 (2014) L.S.Kisslinger, M.X.Liu, P.McGaughey Numerical integration of thermal noise in relativistic hydrodynamics
doi: 10.1103/PhysRevC.89.024914
2011KI05 Eur.Phys.J. A 47, 8 (2011) QCD: The Λ(1405) as a hybrid
doi: 10.1140/epja/i2011-11008-5
2010KI13 Nucl.Phys. A844, 171c (2010) Heavy quark hybrids, decay puzzles, and BES/CLEO/RHIC experiments
doi: 10.1016/j.nuclphysa.2010.05.030
2005KI08 Phys.Rev. D 71, 094021 (2005) L.S.Kisslinger, W.-h.Ma, P.Shen Single and double peripheral production of sigmas in proton-proton collisions NUCLEAR REACTIONS 1H(p, X), E=50 GeV; calculated single- and double-sigma production σ(E, θ). Pomeron formalism.
doi: 10.1103/PhysRevD.71.094021
2005WE17 Int.J.Mod.Phys. E14, 1197 (2005) H.Wen, L.S.Kisslinger, W.Greiner, G.Mao Neutron spin polarization in strong magnetic fields
doi: 10.1142/S021830130500379X
2003JO19 Nucl.Phys. A729, 729 (2003) M.B.Johnson, H.-M.Choi, L.S.Kisslinger Bubble collisions in a SU(2) model of QCD
doi: 10.1016/j.nuclphysa.2003.09.012
2002HE12 Nucl.Phys. A706, 163 (2002) E.M.Henley, W.-Y.P.Hwang, L.S.Kisslinger Nonleptonic Hyperon Decays with QCD Sum Rules
doi: 10.1016/S0375-9474(02)00757-1
2002KI18 Phys.Rev. C66, 045206 (2002) Light-cone representation of the quark Schwinger-Dyson equation
doi: 10.1103/PhysRevC.66.045206
2000KI21 Phys.Lett. 485B, 367 (2000) Pomeron and the Reggeized Glueball/Sigma
doi: 10.1016/S0370-2693(00)00715-2
1999KI01 Phys.Lett. 445B, 271 (1999) Sigma Signal for Hybrid Baryon Decay
doi: 10.1016/S0370-2693(98)01503-2
1999KI11 Phys.Rev. C59, 3377 (1999) Vector, Axial, Tensor, and Pseudoscalar Vacuum Susceptibilities
doi: 10.1103/PhysRevC.59.3377
1999KI25 Phys.Rev. C60, 065204 (1999) L.S.Kisslinger, M.Aw, A.Harey, O.Linsuain Quark Propagator, Instantons, and Gluon Propagator
doi: 10.1103/PhysRevC.60.065204
1999ME02 Phys.Rev. C59, 986 (1999) Mesons as (q-bar)-q Bound States from Euclidean Two-Point Correlators in the Bethe-Salpeter Approach
doi: 10.1103/PhysRevC.59.986
1998KI02 Phys.Rev. C57, 1528 (1998) Structure of Vacuum Condensates
doi: 10.1103/PhysRevC.57.1528
1998KI03 Nucl.Phys. A629, 30c (1998) Gluonic Hadrons
doi: 10.1016/S0375-9474(97)00662-3
1997KI23 Phys.Lett. 410B, 1 (1997) L.S.Kisslinger, J.Gardner, C.Vanderstraeten Mixed Scalar Glueballs and Mesons
doi: 10.1016/S0370-2693(97)00964-7
1996HE32 Phys.Lett. 367B, 21 (1996); Addendum Phys.Lett. 440B, 449 (1998) E.M.Henley, W.-Y.P.Hwang, L.S.Kisslinger The Weak Parity-Violating Pion-Nucleon Coupling NUCLEAR STRUCTURE 19F; analyzed parity violating limits, associated features. QCD sum rules.
doi: 10.1016/0370-2693(95)01403-9
1995JO16 Phys.Rev. C52, 1022 (1995) Δ(1232) in Nuclei and QCD Sum Rules
doi: 10.1103/PhysRevC.52.1022
1995JU03 Nucl.Phys. A586, 682 (1995) Non-Local Quark Condensate for the Nucleon Sea-Quark Distribution
doi: 10.1016/0375-9474(95)00004-K
1994KI04 Nucl.Phys. A570, 167c (1994) The QCD Sum Rule for the Light-Heavy Quark Systems
doi: 10.1016/0375-9474(94)90280-1
1993MA32 Nucl.Phys. A560, 997 (1993) Multiquark Cluster Effect in a Three-Body System NUCLEAR STRUCTURE 3He; calculated charge density; deduced multi-quark cluster effect role. Hybrid quark-hadron model.
doi: 10.1016/0375-9474(93)90176-X
1992MA46 Chin.J.Nucl.Phys. 14, No 3, 197 (1992) W.Ma, D.Strottman, Q.Wu, L.S.Kisslinger, S.Wang A Good Place for Dibaryon to Manifest Itself NUCLEAR REACTIONS 18O(π+, π-), E=164 MeV; calculated σ(θ); deduced dibaryon state role.
1991MA38 Nucl.Phys. A531, 493 (1991) The Hybrid Quark-Hadron Model for Three-Body Systems NUCLEAR STRUCTURE 3He, 3H; calculated charge, magnetic form factors. Quark-hadron model.
doi: 10.1016/0375-9474(91)90738-R
1990CA02 Phys.Rev. C41, 647 (1990) Deuteron Electromagnetic Form Factors in a Chiral Quark Model NUCLEAR STRUCTURE 2H; calculated electromagnetic form factors. Chiral quark model.
doi: 10.1103/PhysRevC.41.647
1989CA20 Phys.Rev. C40, 1722 (1989) Low-Energy Nucleon-Nucleon Scattering in a Relativised Quark Model NUCLEAR REACTIONS 1n, 1H(p, p), E(cm)=25-175 MeV; calculated phase shift vs E. Resonating group formalism.
doi: 10.1103/PhysRevC.40.1722
1989IT03 Phys.Rev. C40, 887 (1989) Tensor Polarization of the Elastic e- 2H Scattering and the Scaling Behavior of Six-Quark Dynamics NUCLEAR REACTIONS 2H(e, e), E not given; calculated tensor polarization vs momentum transfer. Resonating group method, six quark system. NUCLEAR STRUCTURE 2H; calculated D-, S-state wave functions, asymptotic D/S ratio, charge monopole, magnetic dipole form factors. Six quark system.
doi: 10.1103/PhysRevC.40.887
1989SI18 Phys.Rev. C40, 2218 (1989) R.R.Silbar, W.M.Kloet, L.S.Kisslinger, J.Dubach Pion-Exchange Contribution to the Parity-Violating Asymmetry in p(pol)p Scattering NUCLEAR REACTIONS 1H(polarized p, p), E=200-1000 MeV; calculated parity violating asymmetry vs E; deduced pion-exchange contribution.
doi: 10.1103/PhysRevC.40.2218
1987CH09 Phys.Rev. C35, 1432 (1987) Quark-Cluster Effects in Elastic Electron-Deuteron Scattering NUCLEAR STRUCTURE 2H; calculated electric, magnetic structure functions, charge, quadrupole form factors; deduced quark cluster role. Hybrid quark-hadron model.
doi: 10.1103/PhysRevC.35.1432
1987IT01 Ann.Phys.(New York) 174, 169 (1987) Nuclear Magnetic Moments in the Hybrid Quark-Hadron Model NUCLEAR MOMENTS 15N, 17O, 39K, 41Ca; calculated μ, B(M1). Hybrid quark-hadron model.
doi: 10.1016/0003-4916(87)90083-2
1987KI18 Phys.Rev. C36, 1081 (1987) European Muon Collaboration Effect in the Hybrid Quark-Hadron Model NUCLEAR STRUCTURE Fe, 2H; calculated structure function ratio.
doi: 10.1103/PhysRevC.36.1081
1987KI23 Phys.Rev. C36, 1747 (1987) Tensor Polarization of the Deuteron as a Test of Quantum Chromodynamics NUCLEAR REACTIONS 2H(e, e), E not given; calculated target tensor polarization. Quantum chromodynamics.
doi: 10.1103/PhysRevC.36.1747
1986CH31 Nucl.Phys. A457, 602 (1986) Possible Role of Six-Quark Clusters in Deuteron Electrodisintegration NUCLEAR REACTIONS 2H(e, n), E not given; calculated electrodisintegration σ(θ) vs E(np); deduced quark cluster, impulse, pionic processes role. Hybrid quark-hadron model.
doi: 10.1016/0375-9474(86)90470-7
1986HE01 Phys.Rev. C33, 608 (1986) Hybrid Quark-Hadron Model of Lambda Nonmesonic Decay: Finite nuclei NUCLEAR STRUCTURE 11C; calculated p-, s-shell nucleon pickup.
doi: 10.1103/PhysRevC.33.608
1986JO04 Phys.Lett. 168B, 26 (1986) Six-Quark Clusters and Pion Double Charge Exchange in the Δ33 Energy Region NUCLEAR REACTIONS 18O(π+, π-), E ≈ 20-320 MeV; calculated double IAS excitation σ(θ) vs E; deduced short-range quark effects at isobar resonance. Six-quark clusters, pion double charge exchange.
doi: 10.1016/0370-2693(86)91453-X
1986KI17 Nucl.Phys. A459, 645 (1986) L.S.Kisslinger, W.-H.Ma, P.Hoodbhoy Charge From Factors of 3He and 3H in Hybrid Quark Hadron Model NUCLEAR STRUCTURE 3He, 3H; calculated charge form factors. Hybrid quark hadron model.
doi: 10.1016/0375-9474(86)90166-1
1984HO22 Phys.Lett. 146B, 163 (1984) The 3He Charge Form Factor in the Hybrid Model NUCLEAR STRUCTURE 3He; calculated charge form factor. Hybrid quark model.
doi: 10.1016/0370-2693(84)91009-8
1984KE02 Nucl.Phys. A412, 301 (1984) Microscopic Two-Baryon Dynamics and the (p, π) Reaction NUCLEAR REACTIONS 12C(polarized p, π+), E=200 MeV; calculated σ(θ), analyzing power vs θ. Isobar-doorway model.
doi: 10.1016/0375-9474(84)90685-7
1984KI17 Phys.Lett. 146B, 159 (1984) Pion-Nucleus Optical Potential with Dirac Hartree-Fock Nuclear Densities NUCLEAR REACTIONS 40Ca, 16O(π, π), E=50 MeV; calculated σ(θ). Dirac Hartree-Fock model, relativistic pion-nucleon amplitude.
doi: 10.1016/0370-2693(84)91008-6
1983MI04 Phys.Rev. C27, 1669 (1983) Quark Contributions to the pp → dπ+, dπ+ → pp Reaction NUCLEAR REACTIONS 2H(π+, p), E not given; 1H(p, π+), E=570, 660 MeV; calculated σ(θ). Quark model.
doi: 10.1103/PhysRevC.27.1669
1981SA14 Phys.Rev. C23, 2140 (1981) A.N.Saharia, R.M.Woloshyn, L.S.Kisslinger Pion-Nucleus Optical Potential in the Isobar-Doorway Model NUCLEAR REACTIONS 16O(π+, π+), E=114, 163, 240 MeV; 12C(π-, π-), E=120, 150, 180, 200, 230 MeV; 12C(π+, π+), E=148, 168 MeV; 4He(π-, π-), E=110, 150, 180, 220 MeV; analyzed σ(θ); deduced pion-nucleus optical potential parameters. Isobar doorway model.
doi: 10.1103/PhysRevC.23.2140
1978EP02 Phys.Rev. C17, 1501 (1978) G.N.Epstein, F.Tabakin, C.M.Vincent, A.Gal, L.S.Kisslinger Distorted-Wave Impulse-Approximation Evaluation of Sum Rule for Hypernuclear Formation in Forward (K-, π-) NUCLEAR REACTIONS 12C, 40Ca(K-, π-), E=900 MeV/c; calculated σ.
doi: 10.1103/PhysRevC.17.1501
1976KI07 Ann.Phys. (New York) 99, 374 (1976) The Isobar-Doorway Theory for Pion-Nucleus Interactions NUCLEAR REACTIONS 12C(π-, π-), (π-, X), E=100-280 MeV; calculated σ(E, θ).
doi: 10.1016/0003-4916(76)90100-7
1975KI11 Phys.Rev. C12, 36 (1975) Coulomb Corrections for Extracting Spectroscopic Factors Using Analyticity NUCLEAR REACTIONS 3He(p, p), E=4-19.48 MeV; calculated S.
doi: 10.1103/PhysRevC.12.36
1974KI01 Phys.Rev. C9, 188 (1974) Pion-Nucleus Coordinate-Space Potential NUCLEAR REACTIONS 12C(π, π), E=120-280 MeV; calculated σ(θ): optical potential deduced from multiple-scattering theory.
doi: 10.1103/PhysRevC.9.188
1973KI03 Phys.Rev.Lett. 30, 1071 (1973) Pion-Nucleus Scattering in an Isobar-Doorway Model NUCLEAR REACTIONS 12C(π-, π-); calculated σ(E, θ); isobar-doorway model.
doi: 10.1103/PhysRevLett.30.1071
1973KI07 Phys.Lett. 47B, 93 (1973) Analysis of p-3He Elastic Scattering Using Analyticity NUCLEAR REACTIONS 3He(p, p), E=4-20 MeV; calculated σ(E). 3He deduced S.
doi: 10.1016/0370-2693(73)90577-7
1972KI07 Phys.Rev. C6, 469 (1972) L.S.Kisslinger, R.L.Burman, J.H.Koch, M.M.Sternheim Elastic Pion-Nucleus Scattering for Studies of the Nuclear Surface NUCLEAR REACTIONS 40Ca, 208Pb(π-, π-), (π+, π+), E=57-150 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.6.469
1972KI08 Phys.Rev.Lett. 29, 505 (1972) Determination of Nuclear Spectroscopic Factors by Dispersion Relations
doi: 10.1103/PhysRevLett.29.505
1971BO15 Nucl.Phys. A164, 422 (1971) G.Borse, W.-C.Huang, L.S.Kisslinger A Study of Self-Consistent Particle and Quasiparticle Equations of Motion NUCLEAR STRUCTURE 59Ni, 59Cu; calculated levels. Particle, quasiparticle equations of motion.
doi: 10.1016/0375-9474(71)90226-0
1963KI21 Rev.Mod.Phys. 35, 853 (1963) Spherical Nuclei with Simple Residual Forces
doi: 10.1103/RevModPhys.35.853
1962WU01 Bull.Am.Phys.Soc. 7, No.8, 539, J1 (1962) Estimate of the β-Decay Matrix Elements for Sb124 NUCLEAR STRUCTURE 124Sb; measured not abstracted; deduced nuclear properties.
1959KI11 Phys.Rev. 114, 292 (1959) Nuclear Structure Effects in Internal Conversion Coefficients by Configuration Mixing RADIOACTIVITY 203Tl(IT); calculated internal conversion coefficients for M1 and E2 transitions.
doi: 10.1103/PhysRev.114.292
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