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NSR database version of May 24, 2024.

Search: Author = L.S.Kisslinger

Found 52 matches.

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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
Citations: PlumX Metrics

2011KI05      Eur.Phys.J. A 47, 8 (2011)

L.S.Kisslinger, E.M.Henley

QCD: The Λ(1405) as a hybrid

doi: 10.1140/epja/i2011-11008-5
Citations: PlumX Metrics

2010KI13      Nucl.Phys. A844, 171c (2010)


Heavy quark hybrids, decay puzzles, and BES/CLEO/RHIC experiments

doi: 10.1016/j.nuclphysa.2010.05.030
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2002KI18      Phys.Rev. C66, 045206 (2002)

L.S.Kisslinger, O.Linsuain

Light-cone representation of the quark Schwinger-Dyson equation

doi: 10.1103/PhysRevC.66.045206
Citations: PlumX Metrics

2000KI21      Phys.Lett. 485B, 367 (2000)

L.S.Kisslinger, W.-H.Ma

Pomeron and the Reggeized Glueball/Sigma

doi: 10.1016/S0370-2693(00)00715-2
Citations: PlumX Metrics

1999KI01      Phys.Lett. 445B, 271 (1999)

L.S.Kisslinger, Z.Li

Sigma Signal for Hybrid Baryon Decay

doi: 10.1016/S0370-2693(98)01503-2
Citations: PlumX Metrics

1999KI11      Phys.Rev. C59, 3377 (1999)


Vector, Axial, Tensor, and Pseudoscalar Vacuum Susceptibilities

doi: 10.1103/PhysRevC.59.3377
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1999ME02      Phys.Rev. C59, 986 (1999)

T.Meissner, L.S.Kisslinger

Mesons as (q-bar)-q Bound States from Euclidean Two-Point Correlators in the Bethe-Salpeter Approach

doi: 10.1103/PhysRevC.59.986
Citations: PlumX Metrics

1998KI02      Phys.Rev. C57, 1528 (1998)

L.S.Kisslinger, T.Meissner

Structure of Vacuum Condensates

doi: 10.1103/PhysRevC.57.1528
Citations: PlumX Metrics

1998KI03      Nucl.Phys. A629, 30c (1998)


Gluonic Hadrons

doi: 10.1016/S0375-9474(97)00662-3
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1995JO16      Phys.Rev. C52, 1022 (1995)

M.B.Johnson, L.S.Kisslinger

Δ(1232) in Nuclei and QCD Sum Rules

doi: 10.1103/PhysRevC.52.1022
Citations: PlumX Metrics

1995JU03      Nucl.Phys. A586, 682 (1995)

H.Jung, L.S.Kisslinger

Non-Local Quark Condensate for the Nucleon Sea-Quark Distribution

doi: 10.1016/0375-9474(95)00004-K
Citations: PlumX Metrics

1994KI04      Nucl.Phys. A570, 167c (1994)

L.S.Kisslinger, Z.Li

The QCD Sum Rule for the Light-Heavy Quark Systems

doi: 10.1016/0375-9474(94)90280-1
Citations: PlumX Metrics

1993MA32      Nucl.Phys. A560, 997 (1993)

W.-H.Ma, Q.Wu, L.S.Kisslinger

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
Citations: PlumX Metrics

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)

W.-H.Ma, L.S.Kisslinger

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
Citations: PlumX Metrics

1990CA02      Phys.Rev. C41, 647 (1990)

Z.-J.Cao, L.S.Kisslinger

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
Citations: PlumX Metrics

1989CA20      Phys.Rev. C40, 1722 (1989)

Z.-J.Cao, L.S.Kisslinger

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
Citations: PlumX Metrics

1989IT03      Phys.Rev. C40, 887 (1989)

H.Ito, L.S.Kisslinger

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1987CH09      Phys.Rev. C35, 1432 (1987)

T.-S.Cheng, L.S.Kisslinger

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
Citations: PlumX Metrics

1987IT01      Ann.Phys.(New York) 174, 169 (1987)

H.Ito, L.S.Kisslinger

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
Citations: PlumX Metrics

1987KI18      Phys.Rev. C36, 1081 (1987)

L.S.Kisslinger, M.B.Johnson

European Muon Collaboration Effect in the Hybrid Quark-Hadron Model

NUCLEAR STRUCTURE Fe, 2H; calculated structure function ratio.

doi: 10.1103/PhysRevC.36.1081
Citations: PlumX Metrics

1987KI23      Phys.Rev. C36, 1747 (1987)

L.S.Kisslinger, H.Ito

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
Citations: PlumX Metrics

1986CH31      Nucl.Phys. A457, 602 (1986)

T.-S.Cheng, L.S.Kisslinger

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
Citations: PlumX Metrics

1986HE01      Phys.Rev. C33, 608 (1986)

D.P.Heddle, L.S.Kisslinger

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
Citations: PlumX Metrics

1986JO04      Phys.Lett. 168B, 26 (1986)

M.B.Johnson, L.S.Kisslinger

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1984HO22      Phys.Lett. 146B, 163 (1984)

P.Hoodbhoy, L.S.Kisslinger

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
Citations: PlumX Metrics

1984KE02      Nucl.Phys. A412, 301 (1984)

B.D.Keister, L.S.Kisslinger

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1983MI04      Phys.Rev. C27, 1669 (1983)

G.A.Miller, L.S.Kisslinger

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1976KI07      Ann.Phys. (New York) 99, 374 (1976)

L.S.Kisslinger, W.L.Wang

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
Citations: PlumX Metrics

1975KI11      Phys.Rev. C12, 36 (1975)

L.S.Kisslinger, K.Nichols

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
Citations: PlumX Metrics

1974KI01      Phys.Rev. C9, 188 (1974)

L.S.Kisslinger, F.Tabakin

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
Citations: PlumX Metrics

1973KI03      Phys.Rev.Lett. 30, 1071 (1973)

L.S.Kisslinger, W.L.Wang

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1972KI08      Phys.Rev.Lett. 29, 505 (1972)


Determination of Nuclear Spectroscopic Factors by Dispersion Relations

doi: 10.1103/PhysRevLett.29.505
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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
Citations: PlumX Metrics

1963KI21      Rev.Mod.Phys. 35, 853 (1963)

L.S.Kisslinger, R.A.Sorensen

Spherical Nuclei with Simple Residual Forces

doi: 10.1103/RevModPhys.35.853
Citations: PlumX Metrics

1962WU01      Bull.Am.Phys.Soc. 7, No.8, 539, J1 (1962)

C.S.Wu, L.S.Kisslinger

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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