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NSR database version of May 30, 2024.

Search: Author = K.Tsushima

Found 85 matches.

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2024CO03      Phys.Rev. C 109, 025202 (2024)

J.J.Cobos-Martinez, K.Tsushima

η and η' mesons in nuclear matter and nuclei

doi: 10.1103/PhysRevC.109.025202
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2022CO01      Phys.Rev. C 105, 025204 (2022)

J.J.Cobos-Martinez, G.N.Zeminiani, K.Tsushima

Υ and ηbnuclear bound states

NUCLEAR STRUCTURE 4He, 12C, 16O, 40,48Ca, 90Zr, 197Au, 208Pb; calculated energies of Υ- and ηb-nucleus bound states, Υ- and ηb-nucleus potentials.

doi: 10.1103/PhysRevC.105.025204
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2022HU01      Nucl.Phys. A1017, 122356 (2022)

P.T.P.Hutauruk, A.Sulaksono, K.Tsushima

Effects of neutrino magnetic moment and charge radius constraints and medium modifications of the nucleon form factors on the neutrino mean free path in dense matter

doi: 10.1016/j.nuclphysa.2021.122356
Citations: PlumX Metrics


2021ZE04      Eur.Phys.J. A 57, 259 (2021)

G.N.Zeminiani, J.J.Cobos-Martinez, K.Tsushima

Υ and ηb mass shifts in nuclear matter

doi: 10.1140/epja/s10050-021-00569-7
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2019HU02      Phys.Rev. C 99, 015202 (2019)

P.T.P.Hutauruk, Y.Oh, K.Tsushima

Electroweak properties of pions in a nuclear medium

doi: 10.1103/PhysRevC.99.015202
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2018DE04      Nucl.Phys. A970, 325 (2018)

W.R.B.de Araujo, J.P.B.C.de Melo, K.Tsushima

Study of the in-medium nucleon electromagnetic form factors using a light-front nucleon wave function combined with the quark-meson coupling model

NUCLEAR STRUCTURE 1n, 1H; calculated magnetic moment, mean-square radius, electric to magnetic form factors vs energy using quark-meson coupling model. Presented also results for nuclear matter. Compared with available data.

doi: 10.1016/j.nuclphysa.2017.12.005
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2017CO11      Phys.Rev. C 96, 035201 (2017)

J.J.Cobos-Martinez, K.Tsushima, G.Krein, A.W.Thomas

Φ-meson-nucleus bound states

doi: 10.1103/PhysRevC.96.035201
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2017SH15      Phys.Lett. B 770, 236 (2017)

R.Shyam, K.Tsushima

Production of L+c hypernuclei in antiproton-nucleus collisions

NUCLEAR REACTIONS 16O(p-bar, X), E<20 GeV; measured reaction products. 16O; deduced hypernuclei production σ(θ).

doi: 10.1016/j.physletb.2017.04.057
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2015SH20      Nucl.Phys. A939, 101 (2015)

Shubhchintak, Neelam, R.Chatterjee, R.Shyam, K.Tsushima

Coulomb breakup of 37Mg and its ground state structure

NUCLEAR REACTIONS Pb(37Mg, x), E=244 MeV/nucleon; calculated pure Coulomb one-neutron removal σ, σ(E), σ(E, θ) vs neutron separation energy and vs deformation, parallel momentum distribution using FR DWBA.

doi: 10.1016/j.nuclphysa.2015.03.011
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2014DE31      Phys.Rev. C 90, 035201 (2014)

J.P.B.C.de Melo, K.Tsushima, B.El-Bennich, E.Rojas, T.Frederico

Pion structure in the nuclear medium

doi: 10.1103/PhysRevC.90.035201
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2014WH01      Phys.Rev. C 89, 065801 (2014)

D.L.Whittenbury, J.D.Carroll, A.W.Thomas, K.Tsushima, J.R.Stone

Quark-meson coupling model, nuclear matter constraints, and neutron star properties

doi: 10.1103/PhysRevC.89.065801
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2013CA02      Phys.Rev. C 87, 015801 (2013)

M.E.Carrillo-Serrano, I.C.Cloet, K.Tsushima, A.W.Thomas, I.R.Afnan

Variations of nuclear binding with quark masses

NUCLEAR STRUCTURE 7Li, 12C, 16O; calculated single-particle energies versus quark masses. 2,3H, 7Li, 12C, 16O; calculated variation of binding energy, and the 1S0 antibound pole position versus quark mass. Quark-meson coupling (QMD) and one boson-exchange (OBE) models. 7Li; calculated abundance using Big Bang nucleosynthesis computer code of Kawano.

doi: 10.1103/PhysRevC.87.015801
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2013CH31      Nucl.Phys. A913, 116 (2013)

R.Chatterjee, R.Shyam, K.Tsushima, A.W.Thomas

Structure and Coulomb dissociation of 23O within the quark-meson coupling model

NUCLEAR REACTIONS Pb(23O, n22O), E=422 MeV/nucleon; calculated Coulomb dissociation σ(E), longitudinal momentum distribution using QMC (quark-meson coupling) model. Compared with available data.

NUCLEAR STRUCTURE 23N, 23O, 31Ne, 35Mg, 37Na, 45S, 49Ar; calculated valence neutron separation energy, 23O density distribution, neutron, proton radii using QMC (quark-meson coupling) model. Compared with available data.

doi: 10.1016/j.nuclphysa.2013.06.004
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2013CH40      Phys.Rev. C 87, 065502 (2013)

M.K.Cheoun, K.S.Choi, K.S.Kim, K.Saito, T.Kajino, K.Tsushima, T.Maruyama

Effects of the density-dependent weak form factors on the neutrino reaction via neutral current for the nucleon in nuclear matter and 12C

NUCLEAR REACTIONS 12C(ν, ν'), (ν-bar, ν-bar'), E<80 MeV; calculated density-dependent form factors for electron neutrino and electron antineutrino collisions with 12C, σ(E). Large asymmetry in the antineutrino cross sections due to difference in helicities of neutrino and antineutrino. Quark-meson-coupling (QMC) model.

doi: 10.1103/PhysRevC.87.065502
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2013MI04      Phys.Rev. C 87, 035201 (2013)

T.Mizutani, C.Fayard, B.Saghai, K.Tsushima

Faddeev-chiral unitary approach to the K-d scattering length

doi: 10.1103/PhysRevC.87.035201
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2013RA01      J.Phys.(London) G40, 015102 (2013)

G.Ramalho, K.Tsushima, A.W.Thomas

Octet baryon electromagnetic form factors in nuclear medium

doi: 10.1088/0954-3899/40/1/015102
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2012SH11      Nucl.Phys. A881, 255 (2012)

R.Shyam, K.Tsushima, A.W.Thomas

Production of cascade hypernuclei via the (K-, K+) reaction within a quark-meson coupling model

NUCLEAR REACTIONS 1H(K-, K+-, E at 1-4 GeV/c;12C, 28Si(K-, K+), E at 0.5-2 GeV/c; calculated Ξ-, bound hypernuclei 12ΞBe, 28ΞMg hypernuclei production σ, σ(θ) using covariant effective Lagrangian model including Λ and Σ resonance intermediate states. Compared with data.

doi: 10.1016/j.nuclphysa.2012.01.025
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2011TS06      Phys.Rev. C 83, 065208 (2011)

K.Tsushima, D.H.Lu, G.Krein, A.W.Thomas

J/ψ-nuclear bound states

doi: 10.1103/PhysRevC.83.065208
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2010TS03      Int.J.Mod.Phys. E19, 2546 (2010)

K.Tsushima, P.A.M.Guichon, R.Shyam, A.W.Thomas

Binding of hypernuclei, and photoproduction of Λ-hypernuclei in the latest quark-meson coupling model

NUCLEAR STRUCTURE 16,17O, 40,41,49Ca, 89Y, 91Zr, 208,209Pb; calculated hypernuclei single-particle energies. Quark-meson coupling model, comparison with experimental data.

doi: 10.1142/S021830131001706X
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2009GU13      Phys.Rev. C 79, 055205 (2009)

V.Guzey, A.W.Thomas, K.Tsushima

Medium modifications of the bound nucleon generalized parton distributions and the quark contribution to the spin sum rule

doi: 10.1103/PhysRevC.79.055205
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2009PE08      Int.J.Mod.Phys. E18, 705 (2009)

M.A.Perez-Garcia, K.Tsushima, A.Valcarce

Simulation of symmetric nuclei and the role of Pauli potential in binding energies and radii

NUCLEAR STRUCTURE 16O; calculated binding energy per nucleon, matter RMS radius. Semiclassical Monte Carlo many-body simulation, Pauli potential.

doi: 10.1142/S0218301309012811
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2008GU18      Nucl.Phys. A814, 66 (2008)

P.A.M.Guichon, A.W.Thomas, K.Tsushima

Binding of hypernuclei in the latest quark-meson coupling model

NUCLEAR STRUCTURE 17O, 41,49Ca, 91Zr, 209Pb; calculated hypernuclei binding energies using quark-meson coupling model. Comparison with data.

doi: 10.1016/j.nuclphysa.2008.10.001
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2008MI12      Phys.Rev. C 77, 055203 (2008)

H.Mineo, J.A.Tjon, K.Tsushima, S.N.Yang

Faddeev calculation of the pentaquark Θ+ in the Jona-Lasinio model-based diquark picture

doi: 10.1103/PhysRevC.77.055203
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2007SA01      Prog.Part.Nucl.Phys. 58, 1 (2007)

K.Saito, K.Tsushima, A.W.Thomas

Nucleon and hadron structure changes in the nuclear medium and the impact on observables

doi: 10.10106/j.ppnp.2005.07.003
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2007TS05      Eur.Phys.J. A 31, 626 (2007)

K.Tsushima, K.Saito, A.W.Thomas, A.Valcarce

Nucleon sigma term and quark condensate in nuclear matter

doi: 10.1140/epja/i2006-10179-4
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2005MA78      Nucl.Phys. A760, 319 (2005)

T.Maruyama, T.Muto, T.Tatsumi, K.Tsushima, A.W.Thomas

Kaon condensation and lambda-nucleon loop in the relativistic mean-field approach

doi: 10.1016/j.nuclphysa.2005.06.008
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2005NA04      Phys.Lett. B 606, 335 (2005)

F.S.Navarra, M.Nielsen, K.Tsushima

A QCD sum rule study of Θ+ in nuclear matter

doi: 10.1016/j.physletb.2004.12.016
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2005SA68      Eur.Phys.J. A 26, 159 (2005)

K.Saito, H.Kouno, K.Tsushima, A.W.Thomas

Two-scale scalar mesons in nuclei

NUCLEAR STRUCTURE 40Ca; calculated single-particle energies, charge and neutron density distributions. Chiral invariant model based on linear σ model.

doi: 10.1140/epja/i2005-10170-7
Citations: PlumX Metrics


2005TS02      Phys.Lett. B 612, 5 (2005)

K.Tsushima, K.Saito, F.M.Steffens

Effect of bound nucleon internal structure change on nuclear structure functions

doi: 10.1016/j.physletb.2005.02.056
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2004ST17      Phys.Lett. B 595, 237 (2004)

F.M.Steffens, A.W.Thomas, K.Tsushima

Quark distributions in a medium

doi: 10.1016/j.physletb.2004.06.042
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2004TS08      Phys.Rev. C 70, 038501 (2004)

K.Tsushima, H.Kim, K.Saito

Effect of the bound nucleon form factors on charged-current neutrino-nucleus scattering

NUCLEAR REACTIONS 12C(ν, μ-X), E=0-300 MeV; calculated bound nucleon form factors, σ(E), σ. Quark-meson coupling model.

doi: 10.1103/PhysRevC.70.038501
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2004TS11      J.Phys.(London) G30, 1765 (2004)

K.Tsushima, F.C.Khanna

L+c, Σc, Ξc and Λb hypernuclei in the quark-meson coupling model

NUCLEAR STRUCTURE 17O, 41,49Ca, 91Zr, 209Pb; calculated hypernucleus binding energies, single-particle energies, hyperon-nucleus potential features. Quark-meson coupling model.

doi: 10.1088/0954-3899/30/12/001
Citations: PlumX Metrics


2003SA37      Phys.Lett. B 575, 4 (2003)

K.Saito, K.Tsushima

Scalar and vector form factors of the in-medium nucleon

doi: 10.1016/j.physletb.2003.09.055
Citations: PlumX Metrics


2003SI04      Phys.Rev. C 67, 055201 (2003)

A.Sibirtsev, K.Tsushima, S.Krewald

Systematic Regge theory analysis of ω photoproduction

NUCLEAR REACTIONS 1H(γ, X), E ≈ 1-130 GeV; analyzed ω meson production σ, σ(E, θ); deduced Pomeron exchange contribution, related features. Regge theory.

doi: 10.1103/PhysRevC.67.055201
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2003TS01      Phys.Lett. 552B, 138 (2003)

K.Tsushima, F.C.Khanna

Properties of charmed and bottom hadrons in nuclear matter: a plausible study

doi: 10.1016/S0370-2693(02)03157-X
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2003TS02      Phys.Rev. C 67, 015211 (2003)

K.Tsushima, F.C.Khanna

Λ+c and Λb hypernuclei

NUCLEAR STRUCTURE 41Ca, 209Pb; calculated hypernucleus density distributions, potential strengths. 16,17O, 40,41,49Ca, 89Y, 91Zr, 208,209Pb; calculated hypernucleus single-particle energies. Quark-meson coupling model.

doi: 10.1103/PhysRevC.67.015211
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2003TS05      Phys.Rev. C 68, 034612 (2003)

K.Tsushima, K.Nakayama

Near-threshold ω and φ meson productions in pp collisions

NUCLEAR REACTIONS 1H(p, p'X), E ≈ threshold; calculated ω and φ meson production σ, σ(θ), resonance effects. Relativistic effective Lagrangian.

doi: 10.1103/PhysRevC.68.034612
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2003TS07      Nucl.Phys. A721, 633c (2003)

K.Tsushima, K.Nakayama

Near-threshold ω-meson production in proton-proton collisions: With or without resonance excitations?

NUCLEAR REACTIONS 1H(p, pX), (π-, X), E ≈ threshold; calculated ω meson production σ, σ(θ); deduced resonance contributions.

doi: 10.1016/S0375-9474(03)01140-0
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2002ME14      Eur.Phys.J. A 14, 105 (2002)

W.Melnitchouk, K.Tsushima, A.W.Thomas

Quark-Hadron Duality and the Nuclear EMC Effect

NUCLEAR STRUCTURE 4He; calculated medium modification to proton form factors, role of quark-hadron duality.

doi: 10.1007/s10050-002-8795-0
Citations: PlumX Metrics


2002SA26      Nucl.Phys. A705, 119 (2002)

K.Saito, M.Ueda, K.Tsushima, A.W.Thomas

Structure Functions of Unstable Lithium Isotopes

NUCLEAR STRUCTURE 6,7,8,9,11Li; calculated neutron and proton separation energies, radii, single-particle level energies, spin-average and spin-dependent structure functions. Comparisons with data.

doi: 10.1016/S0375-9474(02)00624-3
Citations: PlumX Metrics


2001GU22      Phys.Rev. D64, 054503 (2001)

V.Guzey, A.W.Thomas, K.Tsushima, K.Saito, M.Strikman

Nonsinglet Structure Function of the 3He-3H System and Divergence of the Gottfried Integral

NUCLEAR STRUCTURE 3H, 3He; calculated nonsinglet structure function, nuclear shadowing effects.

doi: 10.1103/PhysRevD.64.054503
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2001SA55      Phys.Lett. 517B, 93 (2001)

K.Saito, V.Guzey, K.Tsushima, A.W.Thomas

Pions in Isospin Asymmetric Nuclei

NUCLEAR STRUCTURE 3H, 3He; calculated pion distributions, medium effects, flavor nonsinglet structure functions.

doi: 10.1016/S0370-2693(01)00947-9
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2001SI14      Phys.Rev. C63, 044906 (2001)

A.Sibirtsev, K.Tsushima, A.W.Thomas

Charmonium Absorption by Nucleons

NUCLEAR REACTIONS 1n, 1H(γ, X), E(cm)=4-200 GeV; calculated J/ψ production σ. Nucleon collisions with J/ψ particles discussed.

doi: 10.1103/PhysRevC.63.044906
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2001TS01      Nucl.Phys. A680, 280c (2001)

K.Tsushima, A.Sibirtsev, K.Saito, A.W.Thomas, D.H.Lu

Effect of Changes in Meson Properties in a Nuclear Medium: J/ψ dissociation in nuclear matter, and meson-nucleus bound states

doi: 10.1016/S0375-9474(00)00428-0
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2001TS04      J.Phys.(London) G27, 349 (2001)

K.Tsushima, A.Sibirtsev, A.W.Thomas

Kaon Properties and Cross Sections in the Nuclear Medium

doi: 10.1088/0954-3899/27/3/312
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2000PO24      Eur.Phys.J. A 9, 115 (2000)

M.V.Polyakov, A.Sibirtsev, K.Tsushima, W.Cassing, K.Goeke

On the Search for a Narrow Penta-quark Z+-baryon in NN Interactions

NUCLEAR REACTIONS 1H(p, X), E=threshold+100, 200 MeV; calculated neutron-kaon invariant mass spectra; deduced possiblilty of penta-quark Z+-baryon detection.

doi: 10.1007/s100500070061
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2000SA49      Phys.Lett. 493B, 288 (2000)

K.Saito, C.Boros, K.Tsushima, F.Bissey, I.R.Afnan, A.W.Thomas

Deep Inelastic Scattering on Asymmetric Nuclei

NUCLEAR STRUCTURE 3H, 3He; calculated structure functions for deep inelastic scattering, flavor asymmetry features.

doi: 10.1016/S0370-2693(00)01166-7
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2000SI21      Phys.Lett. 484B, 23 (2000)

A.Sibirtsev, K.Tsushima, K.Saito, A.W.Thomas

Novel Features of J/ψ Dissociation in Matter

NUCLEAR REACTIONS Pb(Pb, X), E=high; calculated J/ψ transverse energy, relative yield; deduced in-medium effects.

doi: 10.1016/S0370-2693(00)00635-3
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2000TH06      Nucl.Phys. A663-664, 973c (2000)

A.W.Thomas, D.B.Leinweber, K.Tsushima, S.V.Wright

Chiral Corrections on Baryon Masses Calculated within Lattice QCD

doi: 10.1016/S0375-9474(99)00742-3
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2000TS02      Nucl.Phys. A670, 198c (2000)

K.Tsushima

Study of ω-, η'- and D--Mesic Nuclei

NUCLEAR STRUCTURE 208Pb; calculated D- meson bound state potential. 6He, 11B, 16O, 26Mg, 40Ca, 90Zr, 208Pb; calculated ω, η, and η' bound state energies.

doi: 10.1016/S0375-9474(00)00098-1
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2000TS07      Phys.Rev. C62, 064904 (2000)

K.Tsushima, A.Sibirtsev, A.W.Thomas

Strangeness Production from πN Collisions in Nuclear Matter

doi: 10.1103/PhysRevC.62.064904
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1999KR08      Nucl.Phys. A650, 313 (1999)

G.Krein, A.W.Thomas, K.Tsushima

Fock Terms in the Quark-Meson Coupling Model

doi: 10.1016/S0375-9474(99)00117-7
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1999LU11      Phys.Rev. C60, 068201 (1999)

D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito

Electromagnetic Form Factors of the Bound Nucleon

NUCLEAR STRUCTURE 4He, 16O, 40Ca, 208Pb; calculated bound proton electric, magnetic form factors.

doi: 10.1103/PhysRevC.60.068201
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1999SA03      Phys.Rev. C59, 1203 (1999)

K.Saito, K.Tsushima, D.H.Lu, A.W.Thomas

ω-Nucleus Bound States in the Walecka Model

NUCLEAR STRUCTURE 6He, 11Be, 16O, 26Mg, 40Ca, 90Zr, 208Pb; calculated ω-meson bound state energies. Walecka model, comparison with quark-meson coupling model.

doi: 10.1103/PhysRevC.59.1203
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1999SA30      Phys.Lett. 460B, 17 (1999)

K.Saito, K.Tsushima, A.W.Thomas

Spectral Change of σ and ω Mesons in a Dense Nuclear Medium

doi: 10.1016/S0370-2693(99)00775-3
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1999SA49      Phys.Lett. 465B, 27 (1999)

K.Saito, K.Tsushima, A.W.Thomas

Effect of Nucleon Structure Variation on the Longitudinal Response Function

doi: 10.1016/S0370-2693(99)01087-4
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1999SI01      Nucl.Phys. A646, 427 (1999)

A.Sibirtsev, K.Tsushima, W.Cassing, A.W.Thomas

The Role of the P11(1710) in the NN → NΣK Reaction

NUCLEAR REACTIONS 1H(p, pX), (n, pX), E < 3 GeV; analyzed kaon, sigma production associated σ, related data; deduced role of baryonic resonances, meson exchange contributions.

doi: 10.1016/S0375-9474(98)00646-0
Citations: PlumX Metrics


1999SI19      Eur.Phys.J. A 6, 351 (1999)

A.Sibirtsev, K.Tsushima, A.W.Thomas

On Studying Charm in Nuclei Through Antiproton Annihilation

NUCLEAR REACTIONS 12C, 197Au(p-bar, X), E=4-8 GeV; calculated D-meson production σ, missing mass distributions, momentum spectra.

doi: 10.1007/s100500050353
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1999ST05      Phys.Lett. 447B, 233 (1999)

F.M.Steffens, K.Tsushima, A.W.Thomas, K.Saito

Spin Dependence Parton Distributions in a Bound Nucleon

NUCLEAR STRUCTURE 1n, 1H; calculated spin structure functions; deduced nuclear medium effects.

doi: 10.1016/S0370-2693(98)01591-3
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1999TS01      Phys.Rev. C59, 369 (1999); Erratum Phys.Rev. C61, 029903 (2000)

K.Tsushima, A.Sibirtsev, A.W.Thomas, G.Q.Li

Resonance Model Study of Kaon Production in Baryon-Baryon Reactions for Heavy-Ion Collisions

NUCLEAR REACTIONS 1H(p, K+X), (p, K0X), (n, K+X), (n, K0X), E=high; calculated kaon production σ(E) for several channels. 197Au(197Au, X), Ni(Ni, X), E=high; calculated kaon yields. Resonance model, delta-nucleon interactions considered.

doi: 10.1103/PhysRevC.59.369
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1999TS03      Phys.Rev. C59, 2824 (1999)

K.Tsushima, D.H.Lu, A.W.Thomas, K.Saito, R.H.Landau

Charmed Mesic Nuclei: Bound D and D(bar) States with 208Pb

NUCLEAR STRUCTURE 208Pb; calculated bound D-meson states energies, densities, wavefunctions.

doi: 10.1103/PhysRevC.59.2824
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1999TS06      Phys.Lett. 465B, 36 (1999)

K.Tsushima, K.Saito, A.W.Thomas

Charge Symmetry Breaking in Mirror Nuclei from Quarks

NUCLEAR STRUCTURE 15,17O, 15,17F, 39,41Ca, 39K, 41Sc; calculated single-particle energies in mirror nuclei; deduced charge symmetry breaking effects. Quark-meson coupling model.

doi: 10.1016/S0370-2693(99)01049-7
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1998LU01      Phys.Lett. 417B, 217 (1998)

D.H.Lu, A.W.Thomas, K.Tsushima, A.G.Williams, K.Saito

In-Medium Electron-Nucleon Scattering

doi: 10.1016/S0370-2693(97)01385-3
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1998LU06      Nucl.Phys. A634, 443 (1998)

D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito

Medium Dependence of the Bag Constant in the Quark-Meson Coupling Model

doi: 10.1016/S0375-9474(98)00181-X
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1998LU16      Phys.Lett. 441B, 27 (1998)

D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito

The Neutron Charge Form Factor in Helium-3

NUCLEAR STRUCTURE 1n, 3He; calculated neutron charge form factor; deduced medium effects.

doi: 10.1016/S0370-2693(98)01196-4
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1998SA27      Phys.Lett. 433B, 243 (1998)

K.Saito, K.Tsushima, A.W.Thomas, A.G.Williams

σ and ω Meson Propagation in a Dense Nuclear Medium

doi: 10.1016/S0370-2693(98)00702-3
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1998SI07      Phys.Lett. 421B, 59 (1998)

A.Sibirtsev, K.Tsushima, A.W.Thomas

A Clue to the Mechanism of the ΛK+ Production in pp-Reactions

NUCLEAR REACTIONS 1H(p, pX), E not given; analyzed ΛK+ channel total σ; calculated invariant mass spectra; deduced resonance excitation role.

doi: 10.1016/S0370-2693(98)00025-2
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1998TS03      Nucl.Phys. A630, 691 (1998)

K.Tsushima, K.Saito, J.Haidenbauer, A.W.Thomas

The Quark-Meson Coupling Model for Λ, Σ and Ξ Hypernuclei

NUCLEAR STRUCTURE 17O, 41Ca, 49Ca, 91Zr, 209Pb; calculated hypernuclei single-particle energies. 41Ca, 209Pb; calculated hypernuclei binding energies, charge radii. Quark-meson coupling model.

doi: 10.1016/S0375-9474(97)00806-3
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1998TS07      Phys.Lett. 429B, 239 (1998); Erratum Phys.Lett. 436B, 453 (1998)

K.Tsushima, K.Saito, A.W.Thomas, S.V.Wright

In-Medium Kaon and Antikaon Properties in the Quark-Meson Coupling Model

doi: 10.1016/S0370-2693(98)00488-2
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1998TS14      Phys.Lett. 443B, 26 (1998)

K.Tsushima, D.H.Lu, A.W.Thomas, K.Saito

Are η- and ω-Nuclear States Bound ?

NUCLEAR STRUCTURE 6He, 11B, 16O, 26Mg, 40Ca, 90Zr, 208Pb; calculated η, ω meson single-particle energies, widths; deduced bound states.

doi: 10.1016/S0370-2693(98)01336-7
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1997SA21      Phys.Rev. C55, 2637 (1997)

K.Saito, K.Tsushima, A.W.Thomas

Variation of Hadron Masses in Finite Nuclei

NUCLEAR STRUCTURE 16O, 48Ca, 90Zr; calculated binding energy per nucleon, rms charge radius, nucleon radii differences. 40Ca, 208Pb; calculated binding energy per nucleon, rms charge radius, nucleon radii differences, charge density distribution, hadron mass variation. Quark-meson coupling model.

doi: 10.1103/PhysRevC.55.2637
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1997SA28      Phys.Rev. C56, 566 (1997)

K.Saito, K.Tsushima, A.W.Thomas

ρ-Meson Mass in Light Nuclei

NUCLEAR STRUCTURE 3,4He, 12C; calculated ρ-meson mass, density distribution. Quark-meson coupling model.

doi: 10.1103/PhysRevC.56.566
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1997SA35      Phys.Lett. 406B, 287 (1997)

K.Saito, K.Tsushima, A.W.Thomas

Naturalness in the Quark-Meson Coupling Model

doi: 10.1016/S0370-2693(97)00693-X
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1997TS01      Phys.Lett. 390B, 29 (1997)

K.Tsushima, A.Sibirtsev, A.W.Thomas

Resonance Model Study of Strangeness Production in pp Collisions

NUCLEAR REACTIONS 1H(p, X), E=high; calculated pΛK+-production σ vs (g(ρNN)), cut-off parameters. Extended version of resonance model.

doi: 10.1016/S0370-2693(96)01391-3
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1997TS05      Phys.Lett. 411B, 9 (1997); Erratum Phys.Lett. 421B, 413 (1998)

K.Tsushima, K.Saito, A.W.Thomas

Self-Consistent Description of Λ Hypernuclei in the Quark-Meson Coupling Model

NUCLEAR STRUCTURE 16,17O, 40,41,49Ca, 89Y, 91Zr, 208,209Pb; calculated hypernuclei Λ single particle energies, binding energies, radii; deduced spin-orbit force. Quark-meson coupling model.

doi: 10.1016/S0370-2693(97)00944-1
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1997TS08      Aust.J.Phys. 50, 35 (1997)

K.Tsushima, S.W.Huang, A.Faessler

A Study of the πB → YK Reactions for Kaon Production in Heavy Ion Collisions

NUCLEAR REACTIONS 1H(π+, K+X), (π-, K+X), (π-, K0X), E=high; 1n(π+, K+X), (π0, K+X), E=high; analyzed Λ, Σ production associated σ; deduced parameters. Microscopic transport models.

doi: 10.1071/P96052
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1996FA19      Yad.Fiz. 59, No 10, 1903 (1996); Phys.Atomic Nuclei 59, 1839 (1996)

A.Faessler, A.Sibirtsev, K.Tsushima

Δ Production in (p-bar)d Annihilation at Rest

NUCLEAR REACTIONS 2H(p-bar, X), E at rest; analyzed π+p-, π-p-systems invariant mass distributions; deduced Δ0-, background contributions related features. Statistical model based annihilation, resonance model based πN amplitudes.


1996SA31      Nucl.Phys. A609, 339 (1996)

K.Saito, K.Tsushima, A.W.Thomas

Self-Consistent Description of Finite Nuclei Based on a Relativistic Quark Model

NUCLEAR STRUCTURE 40Ca, 208Pb, 16O, 90Zr; calculated charge density distribution, binding energy per nucleon, rms charge radius. 40,48Ca; calculated isotope shift. 40Ca, 208Pb; calculated single particle energies. Relativistic quark model.

doi: 10.1016/S0375-9474(96)00263-1
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1996SI02      Z.Phys. A354, 215 (1996)

A.Sibirtsev, K.Tsushima, A.Faessler

Delta Excitation in Antiproton-Deuteron Annihilation

NUCLEAR REACTIONS 2H(p-bar, X), E at rest; analyzed π+p-, π-p-system invariant mass spectra, other aspects following (p-bar)d annihilation; deduced Δ-excitation role.

doi: 10.1007/s002180050034
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1995TS01      J.Phys.(London) G21, 33 (1995)

K.Tsushima, S.W.Huang, A.Faessler

Resonance Model of πΔ → YK for Kaon Production in Heavy-Ion Collisions

doi: 10.1088/0954-3899/21/1/005
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1994TS01      Phys.Lett. 333B, 17 (1994)

K.Tsushima, D.O.Riska

The πσ-Axial Exchange Current

doi: 10.1016/0370-2693(94)91001-4
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1994TS02      Phys.Lett. 337B, 245 (1994)

K.Tsushima, S.W.Huang, A.Faessler

The Role of the Δ(1920) Resonance for Kaon Production in Heavy Ion Collisions

NUCLEAR REACTIONS 1n, 1H(π+, X), (π-, X), (π0, X), E=high; calculated σ(E) for (ΣK) production; deduced Δ(1920) resonance role.

doi: 10.1016/0370-2693(94)90971-7
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1989YA12      Nucl.Phys. A500, 429 (1989)

T.Yamaguchi, K.Tsushima, Y.Kohyama, K.Kubodera

Semi-Leptonic Beta-Decay Form Factors and Magnetic Moments of Octet Baryons: Recoil effects and center-of-mass corrections in the cloudy bag model including gluonic effects

RADIOACTIVITY 1n; calculated semi-leptonic β-decay form factors. Cloudy bag model.

NUCLEAR STRUCTURE 1n, 1H; calculated μ. Cloudy bag model.

doi: 10.1016/0375-9474(89)90222-4
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1988TS05      Nucl.Phys. A489, 557 (1988)

K.Tsushima, T.Yamaguchi, Y.Kohyama, K.Kubodera

Weak Interaction Form Factors and Magnetic Moments of Octet Baryons: Chiral bag model with gluonic effects

NUCLEAR STRUCTURE 1n, 1H; calculated μ, weak interaction form factors.

doi: 10.1016/0375-9474(88)90111-X
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1987KO10      Phys.Lett. 186B, 255 (1987)

Y.Kohyama, K.Oikawa, K.Tsushima, K.Kubodera

Weak-Current Form Factors of Octet Baryons in the Volume-Type Cloudy Bag Model

RADIOACTIVITY 1n(β-); calculated vector, axial current form factors. MIT, cloudy bag, SU(3) model.

doi: 10.1016/0370-2693(87)90290-5
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