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NSR database version of May 2, 2024.

Search: Author = B.A.Bian

Found 11 matches.

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2014BI02      Phys.Rev. C 89, 014317 (2014)

B.-A.Bian, Y.Sun, Y.-C.Yang

Projected shell model description for rotational bands in the proton emitter ¹⁴¹Ho

NUCLEAR STRUCTURE ¹⁴¹Ho; calculated levels, J, π, rotational band drawings and configurations, B(M1), signature splitting, dynamical moments of inertia, bandhead energies for proton-decaying nucleus. Projected shell model with the deformed Nilsson single-particle states. Discussed role of hexadecapole deformation. Comparisons with experimental data.

doi: 10.1103/PhysRevC.89.014317
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2011SU02      Phys.Rev. C 83, 014608 (2011)

J.Su, F.Zhang, B.A.Bian

Odd-even effect in heavy-ion collisions at intermediate energies

NUCLEAR REACTIONS ²⁷Al(²⁰Ne, X), E=600 MeV/nucleon; ²⁷Al(²⁸Ne, X), (²⁹Na, X), (³⁰Mg, X), (³¹Al, X), (³²Si, X), (³³P, X), (³⁴S, X), (³⁴Ar, X), (³⁵Cl, X), (³⁷K, X), (³⁸Ca, X), (³⁸Ar, X), (⁴²Ar, X), (⁴⁴Ar, X), E=650 MeV/nucleon; ²⁷Al(³⁶Ar, X), (⁴⁰Ar, X), E=400, 650 MeV/nucleon; ²⁷Al(⁴⁸Ti, X), E=1000 MeV/nucleon; ²⁷Al(⁵⁶Fe, X), E=1050 MeV/nucleon; calculated σ as function of neutron and proton number of the fragments, excitation energy distribution as a function of prefragment charge, projectile-isospin-dependent odd-even effect, pairing effects, V(Z) and V(N) for the products from the decays of ^40,50,55V, ^42,48,53Ti. isospin-dependent quantum molecular dynamics (IQMD) and IQMD + GEMINI models. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.014608
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2010BI05      Eur.Phys.J. A 43, 67 (2010)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Effect of shell structure in the fusion reactions

NUCLEAR REACTIONS ^134,138Ba(⁸²Se, X), ^176,180Hf(⁴⁰Ar, X), ^92,96Zr(¹²⁴Sn, X), E(cm)≈125-270 MeV; calculated fusion probabilities, barrier height, related features using the improved isospin dependent quantum molecular dynamics and Bass models. Comparison with data.

doi: 10.1140/epja/i2009-10889-y
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2009BI10      Nucl.Phys. A829, 1 (2009)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fusion enhancement in the reactions of neutron-rich nuclei

NUCLEAR REACTIONS ¹⁹⁷Au(²⁷Al, X), (³¹Al, X), ¹⁸¹Ta, ²⁰⁸Pb(³²S, X), (³⁸S, X), ⁶⁴Ni(¹²⁴Sn, X), (¹³²Sn, X), E(cm)≈100-270 MeV; calculated fusion barrier height, σ, related features using the improved isospin dependent quantum molecular dynamics and Bass models. Comparison with data.

doi: 10.1016/j.nuclphysa.2009.08.003
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2008BI02      Chin.Phys.Lett. 25, 451 (2008)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fragmentation Cross Sections of ¹²C on Different Targets at Beam Energies from 50 to 100MeV/Nucleon

NUCLEAR REACTIONS ²H, ¹²C, ¹⁴N, ¹⁶O(¹²C, X), E=50-100 MeV/nucleon; calculated fragmentation cross sections using the isospin-dependent Boltzman-Langevin equation model.

doi: 10.1088/0256-307X/25/2/027
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2008BI11      Nucl.Phys. A807, 71 (2008)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fragmentation cross sections of ²⁰Ne collisions with different targets at 600 MeV/nucleon

NUCLEAR REACTIONS ¹²C, ²⁷Al, ⁶³Cu, ¹²⁰Sn, ¹⁸¹Ta, ²⁰⁸Pb(²⁰Ne, X), E=600 MeV/nucleon; calculated Z=2-9 fragment production σ using an isospin-dependent Boltzmann?Langevin model. Comparison with data and other models.

doi: 10.1016/j.nuclphysa.2008.03.014
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2008BI18      Int.J.Mod.Phys. E17, 1927 (2008)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fragmentation cross sections in heavy ion collisions

NUCLEAR REACTIONS C, Al, Cu, Sn, Ta, Pb(Ne, X), E=600 MeV/nucleon; ²H, ¹²C, ¹⁴N, ¹⁶O(¹²C, X), E=50-150 MeV/nucleon; calculated fragmentation cross sections.

doi: 10.1142/S0218301308010908
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2008BI20      Int.J.Mod.Phys. E17, Supplement 1, 80 (2008)

B.-A.Bian, F.-S.Zhang, S.-S.Du

Shell correction energy and the entrance channel effect on the formation of superheavy nuclei

NUCLEAR STRUCTURE ⁶²Zn, ⁷⁶Kr, ²⁰²Pb; calculated reaction systems forming compound nuclei, fusion σ.

doi: 10.1142/S021830130801177X
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2008DU20      Int.J.Mod.Phys. E17, 1979 (2008)

S.-S.Du, B.-A.Bian, F.-S.Zhang

Shell effect in synthesis of superheavy nuclei

NUCLEAR REACTIONS ¹⁵⁴Sm(⁴⁸Ca, X), E(cm) < 160 MeV; ²⁰⁸Pb(³²S, X), E(cm) < 260 MeV; calculated fusion cross sections.

doi: 10.1142/S0218301308010957
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2007BI02      Phys.Rev. C 75, 014312 (2007)

B.-A.Bian, Y.-M.Di, G.-Lu.Long, Y.Sun, J.Zhang, J.A.Sheikh

Systematics of g factors of 2⁺₁ states in even-even nuclei from Gd to Pt: A microscopic description by the projected shell model

NUCLEAR STRUCTURE ^{152,154,156,158,160}Gd, ^{154,156,158,160,162,164}Dy, ^{156,158,160,162,164,166,168,170}Er, ^{164,166,168,170,172,174,176}Yb, ^{166,168,170,172,174,176,178,180}Hf, ^{168,170,172,174,176,178,180,182,184,186}W, ^{178,180,182,184,186,188,190,192}Os, ^{182,184,186,188,190,192,194,196,198}Pt; calculated quadrupole deformation parameters, B(E2), g factors. Projected shell model approach, comparison with data.

doi: 10.1103/PhysRevC.75.014312
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2007BI19      Chin.Phys.Lett. 24, 1529 (2007)

B.-A.Bian, G.-S.Zhang, H.-Y.Zhou

Isospin Effects of Threshold Energy of Radial Flow in Heavy Ion Collisions

doi: 10.1088/0256-307X/24/6/027
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