NSR Query Results

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NSR database version of April 27, 2024.

Search: Author = B.He

Found 29 matches.

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2023LU06      Eur.Phys.J. A 59, 125 (2023)

S.Luo, L.-J.Qi, D.-M.Zhang, B.He, P.-C.Chu, X.-H.Li

An improved empirical formula of α decay half-lives for superheavy nuclei

RADIOACTIVITY ^234,236,238Cm, ²⁴²Cm, ²⁴⁶Cm, ²³⁸Cf, ²⁴²Cf, ²⁴⁶Cf, ²⁵⁰Cf, ²⁵⁴Cf, ²⁴⁶Fm, ²⁵⁰Fm, ²⁵⁴Fm, ²⁵²No, ²⁵⁶No, ²⁵⁸Rf, ²⁶⁶Hs, ²⁷⁰Hs, ²⁸²Ds, ²⁸⁶Fl, ²⁹⁰Lv, ²⁹⁴Og(α); calculated T_1/2; deduced formula. Comparison with available data.

doi: 10.1140/epja/s10050-023-01040-5
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2023QI05      Chin.Phys.C 47, 064107 (2023)

L.-J.Qi, D.-M.Zhang, S.Luo, B.He, X.-J.Wu, X.Chen, X.-H.Li

New Geiger-Nuttall law for cluster radioactivity half-lives

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224}Ra, ²²⁶Ra, ^223,225Ac(¹⁴C), ²²⁸Th(²⁰O), ²³¹Pa(²³F), ²³⁰Th, ²³¹Pa, ^{232,233,234,235}U(²⁴Ne), ²³³U(²⁵Ne), ²³⁴U(²⁶Ne), ^234,236U, ^236,238Pu(²⁸Mg), ²³⁶U(³⁰Mg), ²³⁸Pu(³⁰Mg), (³²Si), ²⁴²Cm(³⁴Si); calculated T_1/2 from Balasubramaniam's formula and further considering the effect of the parent nucleus mass, blocking effect, and effect of reduced mass on cluster radioactivity half-lives; deduced a new Geiger-Nuttall law that is model-independent. Comparison with available data.

doi: 10.1088/1674-1137/accc78
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2023QI07      Eur.Phys.J. A 59, 255 (2023)

L.-J.Qi, D.-M.Zhang, S.Luo, X.-H.Li, B.He, P.C.Chu

Cluster radioactivity half-lives of trans-lead nuclei with a statistical physical preformation factor

RADIOACTIVITY ²²¹Fr, ^221,222,223Ra, ²²³Ac, ^224,226Ra(¹⁴C), ²²⁸Th(²⁰O), ²³⁰Th(²⁴Ne), ²³¹Pa(²³F), ²³¹Pa, ^232,233U(²⁴Ne), ²³³U(²⁵Ne), ²³⁴U(²⁴Ne), ²³⁶Pu(²⁶Ne), ²³⁸Pu(²⁸Mg); calculated T_1/2 using the cluster preformation probability in statistical physical way and Wentzel-Kramers-Brillouin (WKB) theory. Comparison with available data.

doi: 10.1140/epja/s10050-023-01162-w
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2023WA14      Phys.Rev. C 107, 064322 (2023)

T.Wang, B.-c.He, D.-k.Li, C.-x.Zhou

Prolate-oblate asymmetric shape phase transition in the interacting boson model with SU(3) higher-order interactions

NUCLEAR STRUCTURE ¹⁸⁰Hf, ^182,184,186W, ^188,190,192Os, ^194,196Pt, ^198,200Hg; calculated excitation energies for yrast band, J, π, yrast band structure, B(E2), quadrupole moment, prolate-oblate shape phase transition. Interacting boson model with SU(3) higher-order interactions (SU3-IBM). Point out that the average deformation of the prolate shape is nearly twice the one of the oblate shape. Comparison to experimental results.

doi: 10.1103/PhysRevC.107.064322
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2023ZH40      Phys.Rev. C 108, 024318 (2023)

D.-M.Zhang, L.-J.Qi, H.-F.Gui, S.Luo, B.He, X.-J.Wu, X.-H.Li

Analytic formula for the proton radioactivity spectroscopic factor

RADIOACTIVITY ^108,109I, ^111,112,113Cs, ^116,117La, ¹²¹Pr, ^130,131Eu, ¹³⁵Tb, ^140,141mHo, ^{144,145,146m,147m}Tm, ^{150,150m,151,151m}Lu, ^{155,156,156m,157}Ta, ^{159,159m,160,161,161m}Re, ^{164,165,165m,166,166m,167,167m,169m}Ir, ^{169,170,170m,171,171m,172}Au, ^176,177,177mTl, ^184,185,185mBi, ¹⁰³Sb, ¹²⁷Pm, ^159,162Re(p); calculated T_1/2, spectrosocopic factors of proton radioactivity. Deformed two-potential approach (D-TPA). Established link between the quadrupole deformation parameter of proton emitter and spectroscopic factor of proton radioactivity. Comparison to available experimental data and theoretical results obtained with universal decay law for proton radioactivity (UDLP) and the new Geiger-Nuttall law (NG-N).

doi: 10.1103/PhysRevC.108.024318
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2022HE08      Phys.Rev. C 105, 044332 (2022)

B.C.He, S.Y.Zhang, L.Li, Y.A.Luo, Y.Zhang, F.Pan, J.P.Draayer

Even-even Nd isotopes in an SD-pair shell model

NUCLEAR STRUCTURE ^{144,146,148,150,152,154,156}Nd; calculated levels, J, π, B(E2). Nucleon pair shell model truncated to SD collective pair subspace (SDPSM). Comparison to experimental data.

doi: 10.1103/PhysRevC.105.044332
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2022LI12      Int.J.Mod.Phys. E31, 2250014 (2022)

Z.W.Li, B.C.He, L.Li, Y.A.Luo, L.N.Bao, F.Pan, J.P.Draayer

Nucleon-pair shell model: Effect of non-collective pairs for odd ^123-129Sn

NUCLEAR STRUCTURE ^{123,124,125,126,127,128,129}Sn; calculated energy levels, J, π, relative angular momenta, B(E2) within the framework of nucleon-pair shell model (NPSM).

doi: 10.1142/S0218301322500148
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2022LU11      Eur.Phys.J. A 58, 244 (2022)

S.Luo, Y.-Y.Xu, D.-X.Zhu, B.He, P.-C.Chu, X.-H.Li

Improved Geiger-Nuttall law for α-decay half-lives of heavy and superheavy nuclei

RADIOACTIVITY ^{220,222,224,226,228,230,232}Th, ^{222,224,226,228,230,232,234,236,238}U, ^{230,232,234,236,238,240,242,244}Pu, ^{234,236,238,240,242,244,246,248}Cm, ^{238,240,242,244,246,248,250,252,254}Cf, ^{244,246,248,250,252,254,256}Fm, ^252,254,256No, ^256,258Rf, ²⁶⁰Sg, ^266,268,270Hs, ²⁷⁰Ds, ²⁸²Ds, ²⁸⁶Cn, ^286,288Fl, ²⁹²Lv, ²⁹⁴Og, ^{221,223,225,227,229}Th, ^{221,223,225,227,229,231}Pa, ^{223,225,227,229,231,233}U, ^233,235,237Np, ^{229,231,233,235}Pu, ^{245,247,249,251,253,255}Es, ^{241,243,245,247,249,251,253,255,257}Fm, ^{245,247,249,251,253,255,257}Md, ^{251,253,255,257,259}No, ^{224,226,228,230}Pa, ^{224,226,228,230,232,234,236}Np, ^{234,236,238,240,242}Am, ²³⁴Bk, ^{240,242,244,246}Es, ^{281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317}Ts, ^{282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318}Og, ^{284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319}119, ^{287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320}120(α); calculated T_1/2. Comparison with available data.

doi: 10.1140/epja/s10050-022-00898-1
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2022PA24      Int.J.Mod.Phys. E31, 2250051 (2022)

X.Pan, Y.-T.Zou, B.He, X.-H.Li, X.-J.Wu, Z.Zhang

Systematic study of two-proton radioactivity half-lives using two-potential approach with different Skyrme interactions

RADIOACTIVITY ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr, ¹⁵Ne, ¹⁷Na, ²²Si, ²⁴P, ²⁶S, ²⁸Cl, ^29,30Ar, ^31,32K, ^33,34Ca, ^35,37Sc, ^37,38,39Ti, ^39,40V, ^41,42Cr, ^43,44Mn, ⁴⁷Co, ⁴⁹Ni, ⁵²Cu, ⁵⁵Zn, ^56,57,58Ga, ^58,59Ge, ^60,61,62As, ^63,64Se, ^65,66Br, ⁶⁸Kr, ⁸¹Mo, ⁸⁵Ru(2p); analyzed available data; calculated T_1/2 using Skyrme energy density functional theory.

doi: 10.1142/S0218301322500513
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2022WU15      Chin.Phys.C 46, 104101 (2022)

Y.-Q.Wu, W.Teng, X.-J.Hou, G.-X.Na, Y.Zhang, B.-C.He, Y.-A.Luo

Spectral fluctuations in the interacting boson model

doi: 10.1088/1674-1137/ac76a5
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2022XU02      Phys.Rev. C 105, 014304 (2022)

H.T.Xue, X.R.Zhou, S.Y.Zhang, B.C.He, Y.A.Luo, L.Li, F.Pan, J.P.Draayer

Neutrinoless double-β decay in the nucleon-pair shell model

RADIOACTIVITY ¹³⁰Te, ^134,136Xe(2β^-); calculated nuclear matrix elements (NMEs) of g.s. to g.s. neutrinoless double-β decay (0νββ) in the nucleon pair shell-model framework, with surface-δ approximation (SDI) and the BCS approximation. Comparison with shell model (SM), quasiparticle random-phase approximation (QRPA), and IBM2 theoretical calculations.

NUCLEAR STRUCTURE ^130,134,136Xe, ¹³⁰Te, ^134,136Ba; calculated low-lying positive-parity levels p to 10+ using shell model in the surface-δ approximation (SD)-pair or the SDG-pair subspace. Comparison with experimental data taken from the ENSDF database at NNDC, BNL.

doi: 10.1103/PhysRevC.105.014304
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2022XU10      Eur.Phys.J. A 58, 163 (2022)

Y.-Y.Xu, D.-X.Zhu, X.Chen, X.-J.Wu, B.He, X.-H.Li

A unified formula for α decay half-lives

RADIOACTIVITY ¹⁰⁹I, ¹⁵¹Eu, ^149,151Tb, ¹⁵⁵Lu, ¹⁵⁷Ta, ¹⁶⁹Re, ^171,173,175Ir, ¹⁷⁵Pt, ¹⁷⁹Pt, ¹⁸⁵Hg, ¹⁷¹Hg, ¹⁷⁷Hg, ¹⁸¹Hg, ^181,183Tl, ¹⁸⁷Tl, ^{179,181,183,185,187,189}Pb, ^187,189Bi, ^209,211,213Bi, ²¹¹Po, ^187,189Po, ²⁰³Po, ^191,193,195At, ¹⁹³Rn, ²⁰⁵Rn, ^211,213Rn, ^219,221Rn, ^221,223Fr, ²¹³Ra, ^{215,217,219,221,223}Ra, ²⁰⁷Ra, ^223,225Ac, ²¹⁷Th, ^{221,223,225,227,229}Th, ²¹⁷Pa, ²²⁵Pa, ²²⁹Pa, ²¹⁹U, ^223,225,227U, ²³¹U, ^227,229,231Np, ^235,237Np, ²²⁹Pu, ²³³Pu, ²⁴¹Pu, ²²⁹Am, ^{233,235,237,239,241,243}Am, ²³⁵Cm, ^{241,243,245,247}Cm, ^245,247,249Bk, ²³⁷Cf, ²⁴³Cf, ^247,249,251Cf, ²⁴⁹Es, ^243,245,247Fm, ^251,253Fm, ²⁵⁷Fm, ^{245,247,249,251,253,255,257}Md, ^{253,255,257,259}No, ²⁵⁵Lr, ^{255,257,259,261}Rf, ^257,259Db, ²⁶³Db, ^{259,261,263,265}Sg, ²⁶¹Bh, ²⁶³Hs, ²⁶⁹Hs, ²⁰⁵Ac, ²¹⁷Ac, ²⁵⁷Lr, ¹⁵⁴Ho, ¹⁵⁶Lu, ¹⁶²Ta, ¹⁵⁸Ta, ¹⁶⁰Re, ¹⁶⁸Re, ^170,172,174Ir, ^{180,182,184,186}Au, ¹⁷⁸Tl, ^184,186Tl, ^{186,188,190,192,194}Bi, ^212,214Bi, ²⁰⁶At, ^210,212At, ²¹⁸At, ¹⁹²At, ²⁰⁰At, ¹⁹⁸Fr, ^212,214Fr, ^218,220Fr, ^214,216At, ²²⁰At, ²⁰⁸At, ^222,224,226At, ^216,218Pa, ^228,230Pa, ²²⁴Np, ^228,230Np, ²³⁶Np, ²³⁴Am, ²⁴²Am, ^{242,244,246,248}Es, ^252,254Es, ^244,246Md, ²⁵⁰Md, ^256,258Md, ^254,256Lr, ²⁵⁶Db, ^{281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317}Ts, ^{282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318}Og, ^{284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319}119, ^{287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320}120, ²⁵⁴No, ^256,258Rf(α); calculated T_1/2; deduced formula. Comparison with NUBASE2020 values.

doi: 10.1140/epja/s10050-022-00812-9
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2022XU13      Chin.Phys.C 46, 114103 (2022)

Y.-Y.Xu, D.-X.Zhu, Y.-T.Zou, X.-J.Wu, B.He, X.-H.Li

Systematic study on α-decay half-lives of uranium isotopes with a screened electrostatic barrier

RADIOACTIVITY ^216,217,218U, ²²¹U, ^{222,223,224,225,226,227,228}U, ²²⁹U, ^230,231,232U, ²³³U, ^{234,235,236,237,238,239,240,241,242,243}U(α); calculated T_1/2 using the Gamow model with a screened electrostatic barrier. Comparison with available data.

doi: 10.1088/1674-1137/ac7fe8
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2021CH57      Eur.Phys.J. A 57, 305 (2021)

J.-L.Chen, X.-H.Li, X.-J.Wu, P.-C.Chu, B.He

Systematic study on proton radioactivity of spherical proton emitters within two-potential approach

RADIOACTIVITY ^{144,145,146,147}Tm, ^150,151Lu, ^155,156,157Ta, ^159,160,161Re, ^{164,165,166,167}Ir, ^170,171Au, ^176,177Tl(p); calculated T_1/2. Comparison with available data.

doi: 10.1140/epja/s10050-021-00618-1
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2021DO07      J.Phys.(London) G48, 045103 (2021)

W.-T.Dong, Y.Zhang, B.-C.He, F.Pan, Y.-A.Luo, J.P.Draayer, S.Karampagia

Statistical analysis of the excited-state quantum phase transitions in the interacting boson model

doi: 10.1088/1361-6471/abdd8c
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2021LI16      Chin.Phys.C 45, 024108 (2021)

H.-M.Liu, Y.-T.Zou, X.Pan, J.-L.Chen, B.He, X.-H.Li

New Geiger-Nuttall law for two-proton radioactivity

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr, ²²Si, ²⁶S, ³⁴Ca, ³⁶Sc, ^38,39Ti, ⁴⁰V, ⁴²Cr, ⁴⁷Co, ⁴⁹Ni, ⁵⁶Ga, ^58,59,60Ge, ⁶¹As, ¹⁰N, ²⁸Cl, ³²K, ⁵⁷Ga, ⁶²As, ⁵²Cu, ⁶⁰As(2p); calculated T_1/2 using GLDM, ELDM, the four-parameter empirical formula. Comparison with experimental data.

doi: 10.1088/1674-1137/abd01e
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2021LI45      Int.J.Mod.Phys. E30, 2150074 (2021)

H.-M.Liu, Y.-T.Zou, X.Pan, B.He, X.-H.Li

Systematic study of two-proton radioactivity half-lives based on a modified Gamow-like model

RADIOACTIVITY ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr, ²²Si, ²⁶S, ³⁴Ca, ³⁶Sc, ^38,39Ti, ⁴⁰V, ⁴²Cr, ⁴⁷Co, ⁴⁹Ni, ⁵⁸Ga, ^58,59Ge, ⁶¹As, ¹⁰N, ²⁸Cl, ³²K, ⁵⁷Ga, ⁶²As, ⁵²Cu, ⁶⁰As(2p); calculated T_1/2; deduced T_1/2 and Q-values reaction. Comparison with available data.

doi: 10.1142/S0218301321500749
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2021LI67      Phys.Scr. 96, 12522 (2021)

H.-M.Liu, Y.-T.Zou, X.Pan, X.-H.Li, X.-J.Wu, B.He

Systematic study of cluster radioactivity half-lives based on a modified Gamow-like model

RADIOACTIVITY ^222,224,226Ra(¹⁴C), ^230,232,234U(²⁴Ne), ^234,236U, ^236,238Pu(²⁸Mg), ²²¹Fr, ^221,223Ra, ²²⁵Ac(¹⁴C), ²³¹Pa, ^233,235U(²⁴Ne), ^233,235U(²⁵Ne); calculated T_1/2. Comparison with available data.

doi: 10.1088/1402-4896/ac3dbc
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2021ZO01      Chin.Phys.C 45, 104101 (2021)

Y.-T.Zou, X.Pan, X.-H.Li, H.-M.Liu, X.-J.Wu, B.He

Systematic study of two-proton radioactivity with a screened electrostatic barrier

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); analyzed available data; calculated T_1/2 using five different theoretical models and/or formulas.

doi: 10.1088/1674-1137/ac1b96
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2021ZO02      Phys.Scr. 96, 075301 (2021)

Y.-T.Zou, X.Pan, H.-M.Liu, X.-J.Wu, B.He, X.-H.Li

Systematic studies on a decay half-lives of neptunium isotopes

RADIOACTIVITY ^{219,223,224,225,233,221,222,229,231,235,237,239,220,226,227,228,232,236}Np(α); calculated T_1/2. Comparison with available data.

doi: 10.1088/1402-4896/abf795
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2020HE01      Phys.Rev. C 101, 014324 (2020)

B.C.He, H.T.Xue, L.Li, Y.A.Luo, Y.Zhang, F.Pan, J.P.Draayer

Noncollective nucleon pairs in even-even ^124-128Sn

NUCLEAR STRUCTURE ^124,126,128Sn; calculated positive-parity yrast levels up to 20+, Eγ versus spin, level energy versus spin, and E-GOS versus spin distributions, B(E2) ratios, number of noncollective pairs as function of spin. Collective S- and D-pair shell model (SDPSM) calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.101.014324
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2020HE20      Phys.Rev. C 102, 024304 (2020)

B.C.He, L.Li, Y.A.Luo, Y.Zhang, F.Pan, J.P.Draayer

Nucleon pair shell model in M scheme

NUCLEAR STRUCTURE ¹⁵⁰Nd; calculated levels, J, π, B(E2) using nucleon pair shell model (NPSM) cast into M scheme for the cases with isospin symmetry and without isospin symmetry, with the odd system and even system treated on the same footing. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.024304
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2020HE29      Int.J.Mod.Phys. E29, 2050088 (2020)

B.C.He, Y.Zhang, L.Li, Y.A.Luo, F.Pan, J.P.Draayer

SD-pair shell model: Vibrational and rotational limits in the interacting boson-fermion model for like-nucleon system

doi: 10.1142/S0218301320500883
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2019CH45      Eur.Phys.J. A 55, 214 (2019)

J.-L.Chen, J.-Y.Xu, J.-G.Deng, X.-H.Li, B.He, P.-C.Chu

New Geiger-Nuttall law for proton radioactivity

doi: 10.1140/epja/i2019-12927-7
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2019HE14      Eur.Phys.J. A 55, 143 (2019)

B.-C.He, S.-Y.Zhang, Y.Zhang, Y.-A.Luo, F.Pan, J.P.Draayer

Understanding nuclear dynamics in the SD-pair shell model: From pre-vibration to collective rotation

doi: 10.1140/epja/i2019-12835-x
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2019LI58      Int.J.Mod.Phys. E28, 1950089 (2019)

H.-M.Liu, J.-Y.Xu, J.-G.Deng, B.He, X.-H.Li

Predictions of α decay half-lives for even-even superheavy nuclei with 104≤ Z ≤ 128 based on two-potential approach within cluster-formation model

RADIOACTIVITY ¹⁴⁴Nd, ^146,148Sm, ^148,150,152Gd, ^150,152,154Dy, ^152,154,156Er, ^154,156,158Yb, ^{156,158,160,162,164,166,168,170,172,174}Hf, ^{158,160,162,164,166,168}W, ¹⁸⁰W, ^{162,164,166,168,170,172,174}Os, ¹⁸⁶Os, ^{166,168,170,172,174,176,178,180,182,184,186,188,190}Pt, ^{172,174,176,178,180,182,184,186,188}Hg, ¹⁸⁰Pb, ^{184,186,188,190,192,194}Pb, ²¹⁰Pb, ¹⁹⁰Po, ^{194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^194,196Rn, ^{200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^202,204Ra, ²⁰⁸Ra, ^{214,216,218,220,222,224,226}Ra, ^{212,214,216,218,220,222,224,226,228,230,232}Th, ^{216,218,220,222,224,226,228,230,232,234,236,238}U, ^{228,230,232,234,236,238,240,242,244}Pu, ^{234,236,238,240,242,244,246,248,250}Cm, ^{238,240,242,244,246,248,250,252,254,256}Cf, ²⁴⁴Fm, ²⁴⁸Fm, ^252,254,256Fm, ^254,256,258No, ^256,258,260Rf, ²⁶⁰Sg, ²⁶⁴Hs, ^268,270Hs, ²⁷⁰Ds, ^286,288Fl, ^290,292Lv, ²⁹⁴Og(α); calculated T_1/2. Comparison with available data.

doi: 10.1142/S0218301319500897
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2014SU12      Phys.Rev. C 89, 068201 (2014)

D.Suenaga, B.R.He, Y.-Li.Ma, M.Harada

D and D^* meson mixing in spin-isospin correlated cold nuclear matter

doi: 10.1103/PhysRevC.89.068201
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2003HE04      Phys.Rev. D 67, 014022 (2003)

B.He, H.Li, C.M.Shakin, Q.Sun

Calculation of the pseudoscalar-isoscalar hadronic current correlation functions of the quark-gluon plasma

doi: 10.1103/PhysRevD.67.014022
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2003HE09      Phys.Rev. C 67, 065203 (2003)

B.He, H.Li, C.M.Shakin, Q.Sun

Comparison of temperature-dependent hadronic current correlation functions calculated in lattice simulations of QCD and with a chiral Lagrangian model

doi: 10.1103/PhysRevC.67.065203
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Note: The following list of authors and aliases matches the search parameter B.He: , B.C.HE, B.R.HE