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NSR database version of April 27, 2024.

Search: Author = H.J.Schulze

Found 86 matches.

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2024XU03      Phys.Rev. C 109, 024324 (2024)

H.-T.Xue, Q.B.Chen, J.-W.Cui, C.-F.Chen, H.-J.Schulze, X.-R.Zhou

Structure of low-lying states of ¹²C and ¹³_ΛC in a beyond-mean-field approach

doi: 10.1103/PhysRevC.109.024324
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2023LI59      Phys.Rev. C 108, 064312 (2023)

Y.-X.Liu, C.F.Chen, Q.B.Chen, H.-T.Xue, H.-J.Schulze, X.-R.Zhou

Deformed charmed hypernuclei

doi: 10.1103/PhysRevC.108.064312
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2023XU03      Phys.Rev. C 107, 044317 (2023)

H.-T.Xue, Y.-F.Chen, Q.B.Chen, Y.A.Luo, H.-J.Schulze, X.-R.Zhou

Deformation and spin-orbit splitting of Λ hypernuclei in the Skyrme-Hartree-Fock approach

NUCLEAR STRUCTURE ^12,13C, ¹⁶O, ²⁸Si, ³²S, ⁴⁰Ca, ⁵¹V, ⁸⁹Y, ¹³⁹La, ²⁰⁸Pb; calculated Λ separation energy for hypernuclei, two-dimensional density distributions of Λ orbits, potential energy surfaces, quadrupole deformations of core nucleus and Λ orbitals, Λ spin-orbit slitting. Deformed Skyrme-Hartree-Fock (DSHF) approach with SLy4 NN and SLL4 ΛN interactions. Discussed spin symmetry in the hyperon spectrum. Comparison to available experimental data.

doi: 10.1103/PhysRevC.107.044317
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2022CH36      Chin.Phys.C 46, 064109 (2022)

C.F.Chen, Q.B.Chen, X.-R.Zhou, Y.Y.Chen, J-W.Cui, H.-J.Schulze

Effects of Λ hyperons on the deformations of even-even nuclei

NUCLEAR STRUCTURE ⁸Be, ¹²C, ¹⁶O, ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ³⁶Ar, ⁴⁰Ca, ^22,24,26,28Ne, ^30,32,34,36Si, ^42,44,46,48Ca; calculated potential energy surfaces as functions of quadrupole deformation, hyperon s.p. energy levels as function of quadrupole deformation, density distributions for the occupied s.p. orbits using the deformed Skyrme-Hartree-Fock approach.

doi: 10.1088/1674-1137/ac5b58
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2022GU03      Phys.Rev. C 105, 034322 (2022)

J.Guo, C.F.Chen, X.-R.Zhou, Q.B.Chen, H.-J.Schulze

ΛΛ pairing effects in spherical and deformed multi-Λ hyperisotopes

NUCLEAR STRUCTURE ⁶He, ^10,11,12Be, ^12,13B, ⁴⁰Ca, ¹³²Sn, ²⁰⁸Pb, ²⁴Mg, ⁵⁶Fe, ¹⁰⁴Zr; calculated ΛΛ separation energies (S(2Λ)) double-Λ hypernuclei. ^40,46Ca, ^132,160Sn, ^208,272Pb, ²⁴Mg, ⁵⁶Fe, ¹⁰⁴Zr; calculated pairing gaps, pairing energies of hypernuclei. ¹³⁰Zr; calculated deformation dependence of single-particle level energies, pairing gap and occupation probabilities of hypernuclei. ²⁷⁸Pb; calculated Λ hyperon potentil; single-particle levels. Skyrme-Hartree-Fock approach with Skyrme force SLy5 for the NN interaction, the Nijmegen interaction NSC97f for the ΛN interaction, and the empirical prescription EmpC for the ΛΛ interaction. Comparison to available experimental data.

doi: 10.1103/PhysRevC.105.034322
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2022GU11      Chin.Phys.C 46, 064106 (2022)

J.Guo, D.H.Chen, X.-R.Zhou, Q.B.Chen, H.-J.Schulze

Effects of a kaonic meson on the ground-state properties of nuclei

NUCLEAR STRUCTURE ^{5,6,7,8,9,10,11,12,13,14,15,16,17,18}Be, ^{11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28}O, ^{15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34}Ne; calculated energies of the highest-occupied nucleon s.p. levels, partial neutron and proton s.p. levels within an axially-deformed Skyrme-Hartree-Fock approach combined with a Skyrme-type kaon-nucleon interaction.

doi: 10.1088/1674-1137/ac5601
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2022LI46      Phys.Rev. C 106, 025801 (2022)

H.-M.Liu, J.Zhang, Z.-H.Li, J.-B.Wei, G.F.Burgio, H.-J.Schulze

Microscopic nuclear equation of state at finite temperature and stellar stability

doi: 10.1103/PhysRevC.106.025801
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2022XU11      Phys.Rev. C 106, 044306 (2022)

H.-T.Xue, Q.B.Chen, X.-R.Zhou, Y.Y.Cheng, H.-J.Schulze

Deformation and hyperon halo in hypernuclei

NUCLEAR STRUCTURE ^{11,13,15,17,19,21,23}C, ¹⁰Li, ¹¹Be, ¹²B, ¹⁴N, ¹⁵O, ¹⁶F, ¹⁷Ne; calculated potential energy surface, deformation parameters for hypernucleus and Λ hyperon, Λ removal energy, density distributions of spherical and deformed Λ 1p states, rms radii. Deformed Skyrme-Hartree-Fock approach with combinations of the NN interactions SIII, SGII, SkI4 and the ΛN interactions LY1 and SLL4.

doi: 10.1103/PhysRevC.106.044306
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2021BU11      Prog.Part.Nucl.Phys. 120, 103879 (2021)

G.F.Burgio, H.-J.Schulze, I.Vidana, J.-B.Wei

Neutron stars and the nuclear equation of state

doi: 10.1016/j.ppnp.2021.103879
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2021GU28      Phys.Rev. C 104, L061307 (2021)

J.Guo, X.-R.Zhou, H.-J.Schulze

Skyrme force for all known Ξ^- hypernuclei

NUCLEAR STRUCTURE ¹²Be, ¹³B, ¹⁵C; analyzed experimental results for Ξ^- hypernuclei within a Skyrme-Hartree-Fock approach, with optimal Skyrme parameters determined for a consistent description of experimental data from KISO, IBUKI, KINKA, BNL-E885, BNL-E906, KEK-E224, and KEK-E176 facilities for these nuclei; calculated removal energies for the 1s and 1p states of ¹³B and ¹²Be Ξ^- hypernuclei. Discussed role of deformation for ¹³B Ξ^- hypernucleus.

doi: 10.1103/PhysRevC.104.L061307
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2021LI11      Phys.Rev. C 103, 024307 (2021)

F.Li, J.-J.Lu, Z.-H.Li, C.-Y.Chen, G.F.Burgio, H.-J.Schulze

Accurate nuclear symmetry energy at finite temperature within a Brueckner-Hartree-Fock approach

doi: 10.1103/PhysRevC.103.024307
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2021WE15      Phys.Rev. C 104, 065806 (2021)

J.-B.Wei, G.F.Burgio, Ad.R.Raduta, H.-J.Schulze

Hot neutron stars and their equation of state

doi: 10.1103/PhysRevC.104.065806
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2020GU08      Chin.Phys.C 44, 054110 (2020)

W.Guo, M.Colonna, V.Greco, U.Lombardo, H.-J.Schulze

The spin-isospin decomposition of the nuclear symmetry energy from low to high density

doi: 10.1088/1674-1137/44/5/054110
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2020JI05      Eur.Phys.J. A 56, 135 (2020)

Y.Jin, X.R.Zhou, Y.-Y.Cheng, H.-J.Schulze

Study of Ξ^- hypernuclei in the Skyrme-Hartree-Fock approach

doi: 10.1140/epja/s10050-020-00143-7
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2020SH12      Phys.Rev. C 101, 065801 (2020)

X.L.Shang, A.Li, Z.Q.Miao, G.F.Burgio, H.-J.Schulze

Nucleon effective mass in hot dense matter

doi: 10.1103/PhysRevC.101.065801
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2020WE05      Eur.Phys.J. A 56, 63 (2020)

J.-B.Wei, J.-J.Lu, G.F.Burgio, Z.-H.Li, H.-J.Schulze

Are nuclear matter properties correlated to neutron star observables?

doi: 10.1140/epja/s10050-020-00058-3
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2019JI10      Prog.Theor.Exp.Phys. 2019, 123D03 (2019)

Y.Jin, C.F.Chen, X.-R.Zhou, Y.-Y.Cheng, H.-J.Schulze

Deformed K- nuclei in the Skyrme-Hartree-Fock approach

NUCLEAR STRUCTURE ⁸Be, ¹⁶O, ²⁰Ne, ⁴⁰Ca, ²⁰⁸Pb; calculated hypernuclei central kaon potential, kaon removal energies using a two-dimensional Skyrme–Hartree–Fock model with a KN Skyrme force.

doi: 10.1093/ptep/ptz141
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2019LU14      Phys.Rev. C 100, 054335 (2019)

J.-J.Lu, Z.-H.Li, G.F.Burgio, A.Figura, H.-J.Schulze

Hot neutron stars with microscopic equations of state

doi: 10.1103/PhysRevC.100.054335
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2019WE02      J.Phys.(London) G46, 034001 (2019)

J.-B.Wei, A.Figura, G.F.Burgio, H.Chen, H.-J.Schulze

Neutron star universal relations with microscopic equations of state

doi: 10.1088/1361-6471/aaf95c
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2018LU17      Phys.Rev. C 98, 064322 (2018)

J.-J.Lu, Z.-H.Li, C.-Y.Chen, M.Baldo, H.-J.Schulze

Neutron matter in the hole-line expansion

doi: 10.1103/PhysRevC.98.064322
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2017CU01      Phys.Rev. C 95, 024323 (2017)

J.-W.Cui, X.-R.Zhou, L.-X.Guo, H.-J.Schulze

Investigation of single- and double-Λ hypernuclei using a beyond-mean-field approach

NUCLEAR STRUCTURE ^13,14C, ^21,22Ne; calculated levels, J, π of single- and double-hypernuclei with ¹²C and ²⁰Ne as core nuclei, potential-energy surfaces as functions of deformation parameter β, core B(E2), rms charge radii. Beyond-mean-field approach with angular momentum projection (AMP) techniques and generator coordinate method (GCM) based on Skyrme-Hartree-Fock (SHF). Comparison with experimental data.

doi: 10.1103/PhysRevC.95.024323
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2017LU08      Phys.Rev. C 96, 044309 (2017)

J.-J.Lu, Z.-H.Li, C.-Y.Chen, M.Baldo, H.-J.Schulze

Convergence of the hole-line expansion with modern nucleon-nucleon potentials

doi: 10.1103/PhysRevC.96.044309
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2016BL02      Eur.Phys.J. A 52, 71 (2016)

D.Blaschke, J.Schaffner-Bielich, H.-J.Schulze

Topical issue on exotic matter in neutron stars

doi: 10.1140/epja/i2016-16071-8
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2016BU07      Chin.Phys.Lett. 33, 032101 (2016)

Q.-Y.Bu, Z.-H.Li, H.-J.Schulze

The Brueckner-Hartree-Fock Equation of State for Nuclear Matter and Neutron Skin

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ^114,132Sn, ²⁰⁸Pb; calculated charge radii, neutron skin, binding energies, drop model volume, surface, and Coulomb energy parameter. Comparison with experimental data.

doi: 10.1088/0256-307X/33/3/032101
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2016CH42      Eur.Phys.J. A 52, 291 (2016)

H.Chen, J.-B.Wei, H.-J.Schulze

Strange quark matter and quark stars with the Dyson-Schwinger quark model

doi: 10.1140/epja/i2016-16291-x
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2016LI39      Phys.Rev. C 94, 024322 (2016)

Z.-H.Li, H.-J.Schulze

Correlation strength with modern nucleon-nucleon potentials in the Brueckner-Hartree-Fock approach

doi: 10.1103/PhysRevC.94.024322
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2016RI01      Eur.Phys.J. A 52, 21 (2016)

Th.A.Rijken, H.-J.Schulze

Hyperon-hyperon interactions with the Nijmegen ESC08 model

doi: 10.1140/epja/i2016-16021-6
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2016SU27      Phys.Rev. C 94, 064319 (2016)

T.T.Sun, E.Hiyama, H.Sagawa, H.-J.Schulze, J.Meng

Mean-field approaches for Ξ^- hypernuclei and current experimental data

NUCLEAR STRUCTURE ¹⁵C, ¹²Be; calculated binding energies of hypernuclei with Ξ^- hyperon and the core nuclei of ¹⁴N and ¹¹B; reproduced results for observed 2015 Kiso event for ¹⁵C at the KEK-E373 experiment. Relativistic-mean-field and Skyrme-Hartree-Fock models.

doi: 10.1103/PhysRevC.94.064319
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2015CU01      Phys.Rev. C 91, 054306 (2015)

J.-W.Cui, X.-R.Zhou, H.-J.Schulze

Shape and energy spectra of Λ hypernuclei from a Skyrme-Hartree-Fock model and a beyond-mean-field calculation

NUCLEAR STRUCTURE ^12,13C, ^20,21Ne, ^24,25,26,27Mg, ^26,27,28,29Si; calculated levels, J, π, B(E2), potential energy surface (PES) contours in (β, γ) plane, root-mean-square (rms) radii and deformation β of core nuclei ¹²C, ²⁰Ne, ^24,26Mg, ^26,28Si, and hypernuclei ¹³C, ²¹Ne, ^25,27Mg, ^27,29Si. Triaxial shape-constrained Skyrme-Hartree-Fock mean-field model with a density-dependent pairing interaction and NSC89NΛ interaction. Comparison with available experimental data.

doi: 10.1103/PhysRevC.91.054306
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2015FU13      Phys.Rev. C 92, 065802 (2015)

K.Fukukawa, M.Baldo, G.F.Burgio, L.Lo Monaco, H.-J.Schulze

Nuclear matter equation of state from a quark-model nucleon-nucleon interaction

doi: 10.1103/PhysRevC.92.065802
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2014BA13      Phys.Rev. C 89, 048801 (2014)

M.Baldo, G.F.Burgio, H.-J.Schulze, G.Taranto

Nucleon effective masses within the Brueckner-Hartree-Fock theory: Impact on stellar neutrino emission

doi: 10.1103/PhysRevC.89.048801
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2014SC21      Phys.Rev. C 90, 047301 (2014)

H.-J.Schulze, E.Hiyama

Skyrme force for light and heavy hypernuclei

NUCLEAR STRUCTURE ^5,6,7,8He, ^7,8,9Li, ⁹Be, ^9,10,11,12B, ^12,13,14C, ^15,16N, ¹⁶O, ²⁸Si, ⁸⁹Y, ¹³⁹La, ²⁰⁸Pb; analyzed binding energies of hypernuclei; deduced a new parameter set for a standard NΛ Skyrme force. Skyrme-Hartree-Fock (SHF) approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.047301
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2013SC15      Phys.Rev. C 88, 024322 (2013)

H.-J.Schulze, T.Rijken

Hypernuclear structure with the Nijmegen ESC08 potentials

NUCLEAR STRUCTURE ^12,13,16C, ²⁸Si, ³²S, ⁴⁰Ca, ⁵¹V, ⁸⁹Y, ¹³⁹La, ²⁰⁸Pb; calculated single particle energies in single-hypernuclei. ⁶He, ¹⁰Be, ¹⁴C, ¹⁸O, ³⁰Si, ⁴²Ca, ⁹²Zr, ¹⁴²Ce, ²⁴⁰Pb; calculated bond energies of double-hypernuclei. Brueckner-Hartree-Fock calculations of hypernuclear matter using several potentials. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.024322
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2013ZH30      Int.J.Mod.Phys. E22, 1350038 (2013)

X.-R.Zhou, H.-J.Schulze

Kaonic Nuclei in the Skyrme-Hartree-Fock Approach

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ²⁰⁸Pb; calculated hypernuclei, kaon chemical potential, kaon and nucleon densities. Skyrme-Hartree-Fock nuclear structure approach.

doi: 10.1142/S0218301313500389
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2013ZH40      Nucl.Phys. A914, 332c (2013)

X.-R.Zhou, H.-J.Schulze

Kaonic nuclei in the Skyrme-Hartree-Fock approach

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ²⁰⁸Pb; calculated K^- hypernuclei chemical potential, ¹⁶O K^- hypernucleus calculated neutron, proton, kaon density distribution, radius using combination of standard SHF (Skyrme HF) model with chiral model for kaon-nucleon interaction.

doi: 10.1016/j.nuclphysa.2012.12.121
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2012BA57      Phys.Rev. C 86, 064001 (2012)

M.Baldo, A.Polls, A.Rios, H.-J.Schulze, I.Vidana

Comparative study of neutron and nuclear matter with simplified Argonne nucleon-nucleon potentials

doi: 10.1103/PhysRevC.86.064001
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2012LI06      Chin.Phys.Lett. 29, 012101 (2012)

Z-H.Li, D.-P.Zhang, H.-J.Schulze, W.Zuo

Second-Order Contribution of the Incompressibility in Asymmetric Nuclear Matter

doi: 10.1088/0256-307X/29/1/012101
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2012LI26      Phys.Rev. C 85, 064002 (2012)

Z.H.Li, H.-J.Schulze

Nuclear matter with chiral forces in Brueckner-Hartree-Fock approximation

doi: 10.1103/PhysRevC.85.064002
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2011BU01      Phys.Rev. C 83, 025804 (2011)

G.F.Burgio, H.-J.Schulze, A.Li

Hyperon stars at finite temperature in the Brueckner theory

doi: 10.1103/PhysRevC.83.025804
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2011SC24      Phys.Rev. C 84, 035801 (2011)

H.-J.Schulze, T.Rijken

Maximum mass of hyperon stars with the Nijmegen ESC08 model

doi: 10.1103/PhysRevC.84.035801
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2010LI06      Phys.Rev. C 81, 025806 (2010)

A.Li, X.R.Zhou, G.F.Burgio, H.-J.Schulze

Protoneutron stars in the Brueckner-Hartree-Fock approach and finite-temperature kaon condensation

doi: 10.1103/PhysRevC.81.025806
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2010SC04      Prog.Theor.Phys.(Kyoto) 123, 569 (2010)

H.-J.Schulze, M.T.Win, K.Hagino, H.Sagawa

Hyperons as a Probe of Nuclear Deformation

NUCLEAR STRUCTURE ³⁰Si, ^30,32S; calculated nuclear deformation; deduced large deformation differences between the core nucleus and hypernucleus in ³⁰Si and ³⁰S.

doi: 10.1143/PTP.123.569
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2010SC25      Nucl.Phys. A835, 19c (2010)

H.-J.Schulze

Hypernuclei with a Microscopic Lambda-Nucleon Force

NUCLEAR STRUCTURE ^12,13C, ¹⁶O, ²⁸Si, ³²S, ⁴⁰Ca, ⁵¹V, ⁹⁹Y, ¹³⁹La, ²⁰⁸Pb; calculated hypernuclei single-particle energies. ^{8,9,10,13,14,15,16,17,18,19,20}Be, ^31,32Si; calculated hypernuclei energy, deformation. Bruckner HF, Skyrme HF, soft-core potential.

doi: 10.1016/j.nuclphysa.2010.01.170
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2010SC29      Int.J.Mod.Phys. E19, 2523 (2010)

H.-J.Schulze, H.Sagawa

Hypernuclei with a microscopic lambda-nucleon force

NUCLEAR STRUCTURE ^7,8,9,10Be, ¹⁴C, ¹⁸O, ³⁰Si, ⁴²Ca, ⁹²Zr, ¹⁴²Ce, ²¹⁰Pb; calculated hypernuclei bond energies, energy surfaces, single-particle energies. Skyrme-Hartree-Fock model, comparison with experimental data.

doi: 10.1142/S0218301310017034
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2008CU02      Chinese Physics B 17, 3289 (2008)

C.-X.Cui, W.Zuo, H.J.Schulze

³PF₂ neutron superfluidity in neutron stars and three-body force effect

2008LI11      Phys.Rev. C 77, 034316 (2008)

Z.H.Li, U.Lombardo, H.-J.Schulze, W.Zuo

Consistent nucleon-nucleon potentials and three-body forces

doi: 10.1103/PhysRevC.77.034316
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2008LI37      Phys.Rev. C 78, 028801 (2008)

Z.H.Li, H.-J.Schulze

Neutron star structure with modern nucleonic three-body forces

doi: 10.1103/PhysRevC.78.028801
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2008ZH25      Phys.Rev. C 78, 054306 (2008)

X.-R.Zhou, A.Polls, H.-J.Schulze, I.Vidana

Λ hyperons and the neutron drip line

NUCLEAR STRUCTURE ^{6,7,8,9,10,11,12,13,14,15,16,17,18,19,20}Be, ^{22,23,24,25,26,27,28}O; calculated neutron single-particle levels, binding energies, quadrupole deformations. Hypernuclei. Skyrme Hartree-Fock calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.78.054306
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2008ZH30      Int.J.Mod.Phys. E17, Supplement 1, 192 (2008)

X.-R.Zhou, H.-J.Schulze, H.Sagawa

Properties of nuclei and hypernuclei with the deformed Skyrme Hartree-Fock Model

NUCLEAR STRUCTURE ^7,9Be, ^8,9,10B, ^11,12C, ²⁷Si, ⁵⁰V; calculated deformations, radii. Deformed HF calculations.

doi: 10.1142/S0218301308011859
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2008ZU01      Phys.Rev. C 78, 015805 (2008)

W.Zuo, C.X.Cui, U.Lombardo, H.-J.Schulze

Three-body force effect on ³P F₂ neutron superfluidity in neutron matter, neutron star matter, and neutron stars

doi: 10.1103/PhysRevC.78.015805
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2007BA09      Phys.Rev. C 75, 025802 (2007)

M.Baldo, H.-J.Schulze

Proton pairing in neutron stars

doi: 10.1103/PhysRevC.75.025802
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2007ZH35      Phys.Rev. C 76, 034312 (2007)

X.-R.Zhou, H.-J.Schulze, H.Sagawa, C.-X.Wu, E.-G.Zhao

Hypernuclei in the deformed Skyrme-Hartree-Fock approach

NUCLEAR STRUCTURE ^7,8,9,10Be, ^8,9,10,11B, ^11,12,13C, ^27,28Si, ^50,51V, ^88,89Y, ^207,208Pb; calculated binding energies and deformation parameters using a deformed Hartree-Fock approach for Λ hypernuclei.

doi: 10.1103/PhysRevC.76.034312
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2006LI52      Phys.Rev. C 74, 047304 (2006)

Z.H.Li, U.Lombardo, H.-J.Schulze, W.Zuo, L.W.Chen, H.R.Ma

Nuclear matter saturation point and symmetry energy with modern nucleon-nucleon potentials

doi: 10.1103/PhysRevC.74.047304
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2006SC14      Phys.Rev. C 73, 058801 (2006)

H.-J.Schulze, A.Polls, A.Ramos, I.Vidana

Maximum mass of neutron stars

doi: 10.1103/PhysRevC.73.058801
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2006ZU01      Phys.Rev. C 73, 035208 (2006)

W.Zuo, Z.H.Li, U.Lombardo, G.C.Lu, H.-J.Schulze

Temperature dependence of single-particle properties in nuclear matter

doi: 10.1103/PhysRevC.73.035208
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2006ZU03      Phys.Rev. C 74, 014317 (2006)

W.Zuo, U.Lombardo, H.-J.Schulze, Z.H.Li

Three-body force rearrangement effect on single particle properties in neutron-rich nuclear matter

doi: 10.1103/PhysRevC.74.014317
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2005LO07      Int.J.Mod.Phys. E14, 513 (2005)

U.Lombardo, C.Shen, H.-J.Schulze, W.Zuo

Superfluid states of nuclear matter beyond the BCS approximation

doi: 10.1142/S0218301305003375
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2005ZH23      Phys.Rev.Lett. 95, 051101 (2005)

X.-R.Zhou, H.-J.Schulze, F.Pan, J.P.Draayer

Strong Hyperon-Nucleon Pairing in Neutron Stars

doi: 10.1103/PhysRevLett.95.051101
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2004SC20      Part. and Nucl., Lett. 119, 27 (2004)

H.-J.Schulze, D.Blaschke

Pion broadening and low-mass dilepton production

NUCLEAR REACTIONS ¹⁹⁷Au(Pb, X), E=158 GeV/nucleon; analyzed dilepton mass and transverse momentum spectra; deduced medium effects.

2004ZH06      Phys.Rev. C 69, 018801 (2004)

X.R.Zhou, G.F.Burgio, U.Lombardo, H.-J.Schulze, W.Zuo

Three-body forces and neutron star structure

doi: 10.1103/PhysRevC.69.018801
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2004ZH36      Phys.Rev. C 70, 048802 (2004)

X.-R.Zhou, H.-J.Schulze, E.-G.Zhao, F.Pan, J.P.Draayer

Pairing gaps in neutron stars

doi: 10.1103/PhysRevC.70.048802
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2002BA96      Phys.Rev. C 66, 054304 (2002)

M.Baldo, U.Lombardo, H.-J.Schulze, Z.Wei

Self-energy effects on isospin singlet pairing in nuclear matter

doi: 10.1103/PhysRevC.66.054304
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2002BU22      Phys.Rev. C66, 025802 (2002)

G.F.Burgio, M.Baldo, P.K.Sahu, H.J.Schulze

Hadron-quark phase transition in dense matter and neutron stars

doi: 10.1103/PhysRevC.66.025802
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2002ZU05      Phys.Rev. C66, 037303 (2002)

W.Zuo, U.Lombardo, H.-J.Schulze, C.W.Shen

Short-Range Effects on Nuclear Pairing

doi: 10.1103/PhysRevC.66.037303
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2001GA14      Phys.Rev. C63, 037304 (2001)

E.Garrido, P.Sarriguren, E.Moya de Guerra, U.Lombardo, P.Schuck, H.J.Schulze

Nuclear Pairing in the T = 0 Channel Reexamined

doi: 10.1103/PhysRevC.63.037304
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2001LO27      Phys.Rev. C64, 064314 (2001)

U.Lombardo, P.Nozieres, P.Schuck, H.-J.Schulze, A.Sedrakian

Transition from BCS Pairing to Bose-Einstein Condensation in Low-Density Asymmetric Nuclear Matter

doi: 10.1103/PhysRevC.64.064314
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2001SC17      Phys.Rev. C63, 044310 (2001)

H.-J.Schulze, A.Polls, A.Ramos

Pairing with Polarization Effects in Low-Density Neutron Matter

doi: 10.1103/PhysRevC.63.044310
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2001VI10      Phys.Rev. C64, 044301 (2001)

I.Vidana, A.Polls, A.Ramos, H.-J.Schulze

Hypernuclear Structure with the New Nijmegen Potentials

NUCLEAR STRUCTURE ¹³C, ¹⁷O, ²⁹Si, ⁴¹Ca, ⁹¹Zr, ¹⁴¹Ce, ²⁰⁹Pb; calculated hypernucleus Λ single-particle levels. ¹⁰Be, ¹⁴C, ¹⁸O, ³⁰Si, ⁴²Ca, ⁹²Zr, ¹⁴²Ce, ²¹⁰Pb; calculated two-Λ hypernucleus bond energies. Comparisons with data.

doi: 10.1103/PhysRevC.64.044301
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2000BA41      Phys.Rev. C61, 055801 (2000)

M.Baldo, G.F.Burgio, H.-J.Schulze

Hyperon Stars in the Brueckner-Bethe-Goldstone Theory

doi: 10.1103/PhysRevC.61.055801
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2000CU05      Phys.Rev. C62, 064308 (2000)

J.Cugnon, A.Lejeune, H.-J.Schulze

Hypernuclei in the Skyrme-Hartree-Fock Formalism with a Microscopic Hyperon-Nucleon Force

NUCLEAR STRUCTURE ¹³C, ¹⁷O, ²⁹Si, ⁴¹Ca, ⁹¹Zr, ¹⁴¹Ce, ²⁰⁹Pb; calculated Λ hypernucleus single-particle levels. ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated multi-Λ hypernuclei density profiles, radii, binding energies. Skyrme-Hartree-Fock model.

doi: 10.1103/PhysRevC.62.064308
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1999LO06      Phys.Rev. C59, 2927 (1999)

U.Lombardo, H.-J.Schulze, W.Zuo

Superfluidity and Single-Particle Energies in Nuclear Matter

doi: 10.1103/PhysRevC.59.2927
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1998BA79      Phys.Rev. C58, 1921 (1998)

M.Baldo, O.Elgaroy, L.Engvik, M.Hjorth-Jensen, H.-J.Schulze

³P₂-³F₂ Pairing in Neutron Matter with Modern Nucleon-Nucleon Potentials

doi: 10.1103/PhysRevC.58.1921
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1998BB01      Phys.Rev. C58, 3688 (1998)

M.Baldo, G.F.Burgio, H.-J.Schulze

Onset of Hyperon Formation in Neutron Star Matter from Brueckner Theory

doi: 10.1103/PhysRevC.58.3688
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1998BL02      Phys.Rev. C57, 438 (1998)

D.Blaschke, Yu.L.Kalinovsky, S.Schmidt, H.-J.Schulze

Scalar Correlations in a Quark Plasma and Low Mass Dilepton Production

doi: 10.1103/PhysRevC.57.438
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1998SC01      Phys.Rev. C57, 704 (1998)

H.-J.Schulze, M.Baldo, U.Lombardo, J.Cugnon, A.Lejeune

Hyperonic Nuclear Matter in Brueckner Theory

doi: 10.1103/PhysRevC.57.704
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1998SC02      Phys.Rev. C57, 806 (1998)

A.Schnell, G.Ropke, U.Lombardo, H.-J.Schulze

Elastic Nucleon-Nucleon Cross Section in Nuclear Matter at Finite Temperature

doi: 10.1103/PhysRevC.57.806
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1998ZU01      Phys.Lett. 421B, 1 (1998)

W.Zuo, G.Giansiracusa, U.Lombardo, N.Sandulescu, H.-J.Schulze

Single-Particle Properties in Neutron Matter from Extended Brueckner Theory

doi: 10.1016/S0370-2693(97)01600-6
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1998ZU02      Phys.Lett. 432B, 241 (1998)

W.Zuo, U.Lombardo, H.-J.Schulze

Mean Free Path in Nuclear Matter from Extended Brueckner Theory

doi: 10.1016/S0370-2693(98)00656-X
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1997DE31      Phys.Rev. C56, 2332 (1997)

F.V.De Blasio, M.Hjorth-Jensen, O.Elgaroy, L.Engvik, G.Lazzari, M.Baldo, H.-J.Schulze

Coherence Length of Neutron Superfluids

doi: 10.1103/PhysRevC.56.2332
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1997SC11      Phys.Rev. C55, 3006 (1997)

H.-J.Schulze, A.Schnell, G.Ropke, U.Lombardo

Nucleon-Nucleon Cross Sections in Nuclear Matter

NUCLEAR REACTIONS ¹n, ¹H(n, n), E < 400 MeV; calculated σ(E); deduced density dependence. Brueckner-Hartree-Fock approximation scheme with Paris potential.

doi: 10.1103/PhysRevC.55.3006
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1996SC10      Phys.Lett. 375B, 1 (1996)

H.-J.Schulze, J.Cugnon, A.Lejeune, M.Baldo, U.Lombardo

Medium Polarization Effects on Neutron Matter Superfluidity

doi: 10.1016/0370-2693(96)00213-4
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1995SC18      J.Phys.(London) G21, 185 (1995)

H.-J.Schulze

Pion-Pion Scattering Lengths in the SU(2) Nambu-Jona-Lasinio Model

doi: 10.1088/0954-3899/21/2/006
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1995SC41      Phys.Rev. C52, 2785 (1995)

H.-J.Schulze, J.Cugnon, A.Lejeune, M.Baldo, U.Lombardo

Status of the Brueckner-Hartree-Fock Approximation to the Nuclear Matter Binding Energy with the Paris Potential

doi: 10.1103/PhysRevC.52.2785
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1995SC43      Phys.Lett. 355B, 21 (1995)

H.-J.Schulze, A.Lejeune, J.Cugnon, M.Baldo, U.Lombardo

Hypernuclear Matter in the Brueckner-Hartree-Fock Approximation

doi: 10.1016/0370-2693(95)00665-8
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1994SC08      J.Phys.(London) G20, 531 (1994)

H.-J.Schulze

The Pion Form Factor at Zero and Finite Temperature in the Nambu-Jona-Lasinio Model

doi: 10.1088/0954-3899/20/4/002
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1994SC23      J.Phys.(London) G20, 1283 (1994)

H.J.Schulze

Two-Rho Exchange Contribution to the Pion-Nucleon Scattering Lengths

doi: 10.1088/0954-3899/20/8/018
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