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NSR database version of May 3, 2024.

Search: Author = X.Su

Found 22 matches.

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2024XU04      Chin.Phys.C 48, 024106 (2024)

Y.-L.Xu, X.-W.Su, Zh.-H.Sun, Y.-L.Han, X.-J.Sun, D.-H.Zhang, Ch.-H.Cai

Description of elastic scattering for ⁷Li-induced reactions on 1p-shell nuclei

NUCLEAR REACTIONS ⁹Be, ^10,11B, ^12,13C, ¹⁵N, ¹⁶O(⁷Li, ⁷Li), E=4.5-131.8 MeV; analyzed available data; deduced σ(θ), the global phenomenological optical potentials (GPOPs), the contribution of elastic transfer by the distorted wave Born approximation (DWBA) method.

doi: 10.1088/1674-1137/ad1924
Citations: PlumX Metrics

2023HU23      Eur.Phys.J. A 59, 265 (2023)

D.Y.Huo, Z.Wei, K.Wu, C.Han, Y.X.Wang, Y.N.Han, Z.E.Yao, Y.Zhang, J.R.Wang, X.D.Su

Evaluation of pre-neutron-emission mass distributions in induced fission of typical actinides based on Monte Carlo dropout neural network

NUCLEAR REACTIONS ²³²Th, ^235,238U, ²³⁷Np, ²³⁹Pu(n, F), E<45 MeV; analyzed available data; deduced pre-neutron-emission mass distribution wi th the Monte Carlo dropout neural network (MC-Dropout NN) method.

doi: 10.1140/epja/s10050-023-01189-z
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2022SU13      Nucl.Sci.Eng. 196, 1031 (2022)

X.Su, Y.Xu, Y.Han

Theoretical Analysis of Cross Sections for n+^{46, 47, 49, 50, nat.}Ti Reactions

NUCLEAR REACTIONS ^46,47,49,50Ti, Ti(n, X), E<20 MeV; calculated σ, σ(θ), σ(E), σ(θ, E) using the optical model the unified Hauser-Feshbach theory, the exciton model, which includes the improved Iwamoto-Harada model, and the distorted wave Born approximation theory. Comparison with ENDF/B-VIII, JENDL-4, and JEFF33.

doi: 10.1080/00295639.2022.2049990
Citations: PlumX Metrics

2022XU14      Int.J.Mod.Phys. E31, 2250093 (2022)

Y.Xu, X.Su, Y.Han, X.Sun, D.Zhang, C.Cai

Optical potential for the elastic scattering of ⁶Li projectile on 1p-shell nuclei

NUCLEAR REACTIONS ^6,7Li, ⁹Be, ^10,11B, ^12,13,14C, ¹⁵N, ^16,18O(⁶Li, ⁶Li), E=2-210 MeV; analyzed available data; deduced σ(θ), a set of global optical potential parameters by fitting the experimental data of elastic scattering angular distributions.

doi: 10.1142/S0218301322500938
Citations: PlumX Metrics

2021SU05      Nucl.Sci.Eng. 195, 239 (2021)

X.Su, Y.Xu, Y.Han

Calculations and Evaluations of the n + ⁴⁸Ti Reaction Below 200 MeV

NUCLEAR REACTIONS ⁴⁸Ti(n, X), (n, n), (n, n'), E<200 MeV; analyzed available data; calculated σ, σ(θ). Comparison with the EXFOR library.

doi: 10.1080/00295639.2020.1808388
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2021XU07      Chin.Phys.C 45, 114103 (2021)

Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai

Description of elastic scattering induced by the unstable nuclei ^{9, 10, 11, 13, 14}C

NUCLEAR REACTIONS ²⁰⁸Pb(⁹C, ⁹C), (¹¹C, ¹¹C), E=222-227 MeV; ²⁷Al, ⁵⁸Ni, ²⁰⁸Pb(¹⁰C, ¹⁰C), E=29.1-256 MeV; ²⁸Si, ²⁰⁸Pb(⁹C, ⁹C), E<500 MeV; ²⁸Si, ²⁰⁸Pb(¹¹C, ¹¹C), E<500 MeV; ²⁸Si(¹³C, ¹³C), E=25-60 MeV; ⁴⁰Ca, ⁵⁶Fe, ⁶⁰Ni, ⁶⁶Zn, ⁸⁸Sr(¹⁴C, ¹⁴C), E=51 MeV; ^92,100Mo(¹⁴C, ¹⁴C), E=71 MeV; ²⁸Si(¹⁴C, ¹⁴C), E<500 MeV; analyzed available data; deduced σ, σ(θ), global optical model potentials.

doi: 10.1088/1674-1137/ac1fe1
Citations: PlumX Metrics

2020XU10      Chin.Phys.C 44, 124103 (2020)

Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai

Global optical model potential describing ¹²C-nucleus elastic scattering

NUCLEAR REACTIONS ²⁴Mg, ²⁸Si, ³²S, ³⁹K, ^40,42,48Ca, ⁵⁰Cr, ⁵⁶Fe, Fe, ^58,64Ni, Ni, ^{90,91,92,94,96}Zr, ⁹²Mo, ^{116,117,118,119,120,122,124}Sn, ^194,198Pt, ²⁰⁸Pb, ²⁰⁹Bi(¹²C, ¹²C), E<200 MeV; analyzed available data; deduced a new global optical model potential parameters.

doi: 10.1088/1674-1137/abb4d0
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2019LI22      Chin.Phys.C 43, 064001 (2019)

C.-Q.Liu, Z.Wei, C.Han, C.Huang, Z.-W.Huang, Z.-W.Ma, S.-J.Zhang, S.-Hu.Peng, W.-M.Li, X.-H.Bai, J.-R.Wang, X.-L.Lu, Y.Zhang, D.-P.Xu, X.-D.Su, Z.-E.Yao

Monte Carlo simulation of fast neutron-induced fission of ²³⁷Np

NUCLEAR REACTIONS ²³⁷Np, ²³²Th, ^235,238U, ²³⁹Pu(n, F), E=0.50, 2, 4, 5, 59.9, 5.04, 160, 4.48 MeV; calculated pre-neutron emission fission-fragment mass distribution using GEANT4. Comparison with experimental data.

doi: 10.1088/1674-1137/43/6/064001
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2019SU12      Nucl.Sci.Eng. 193, 760 (2019)

X.Su, Z.Zhang, Y.Han

Calculations and Evaluations of n + ^{113, 115, nat.}In Reactions up to 200 MeV

NUCLEAR REACTIONS ^113,115In, In(n, X), (n, n), (n, n'), E<200 MeV; calculated σ, σ(E), σ(θ, E). Comparison with JENDL-4, ENDF/B-VIII libraries.

doi: 10.13182/NSE15-1
Citations: PlumX Metrics

2019WA30      Chin.Phys.C 43, 114101 (2019)

Y.-Z.Wang, X.-D.Su, C.Qi, J.-Z.Gu

Tensor force effect on the exotic structure of neutron-rich Ca isotopes*

NUCLEAR STRUCTURE ^{56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74}Ca; calculated two neutron separation energy, radii, neutron density distributions using spherical Skyrme-Hartree-Fock-Bogoliubov (SHFB) approach.

doi: 10.1088/1674-1137/43/11/114101
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2019WE13      Eur.Phys.J. A 55, 162 (2019)

Z.Wei, C.Han, S.H.Peng, X.H.Bai, C.Q.Liu, Z.W.Ma, Z.W.Huang, S.J.Zhang, W.M.Li, Y.Yang, Z.E.Yao, W.S.Wu, Y.Zhang, X.L.Lu, J.R.Wang, X.D.Su, D.P.Xu

Physical design and evaluation of a high-intensity accelerator-based D-D/D-T fusion neutron source

doi: 10.1140/epja/i2019-12848-5
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2017SU16      Phys.Rev. C 95, 054606 (2017)

X.W.Su, Y.L.Han, H.Y.Liang, Z.D.Wu, H.R.Guo, C.H.Cai

Global phenomenological optical model potential for ⁸Li projectile

NUCLEAR REACTIONS ⁹Be(⁸Li, ⁸Li), E=14, 19.6, 27 MeV; ¹²C(⁸Li, ⁸Li), E=14, 23.9 MeV; ¹³C, ¹⁴N, ²⁷Al, ¹⁹⁷Au(⁸Li, ⁸Li), E=14 MeV; ⁵¹V(⁸Li, ⁸Li), E=18.5, 26 MeV; ⁵⁸Ni(⁸Li, ⁸Li), E=14, 19.6, 20.2, 22 MeV; ²⁰⁸Pb(⁸Li, ⁸Li), E=24.4, 27.9, 28.9, 30.6, 33.1 MeV; calculated σ(θ, E) by optical potential model, and compared with experimental data; deduced global phenomenological optical model parameters (OMPs) for ⁸Li. ⁹Be(⁸Li, X), E=19.6 MeV; ¹²C(⁸Li, X), E=14 MeV; ⁵¹V(⁸Li, X), E=18.5, 26.0 MeV; ²⁰⁸Pb(⁸Li, X), E=24.4, 27.6, 28.89, 30.57, 33.13 MeV; calculated total σ(E), and compared with experimental data.

doi: 10.1103/PhysRevC.95.054606
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2016SU02      Ann.Nucl.Energy 90, 123 (2016)

X.Su, Y.Han, C.Cai

Neutron-induced reaction on ²³³U

NUCLEAR REACTIONS ²³³U(n, X), (n, n), (n, n'), (n, γ), (n, F), E<200 MeV; calculated σ, σ(E), σ(θ, E). Comparison with experimental data, ENDF/B-VII and JENDL-4 evaluated nuclear libraries.

doi: 10.1016/j.anucene.2015.12.003
Citations: PlumX Metrics

2016SU13      Int.J.Mod.Phys. E25, 1650033 (2016)

X.-W.Su, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai

Global ⁶He optical model potential

NUCLEAR REACTIONS ^6,7Li, ⁹Be, ¹²C, ²⁷Al, ²⁸Si, ⁵¹V, ⁴⁸Ti, ⁵⁸Ni, ^63,65Cu, ⁶⁴Zn, ¹²⁰Sn, ¹⁹⁷Au, ^206,208Pb, ²⁰⁹Bi(⁶He, X), (⁶He, ⁶He), E<300 MeV; analyzed available data; deduced optical potential; calculated σ, σ(θ).

doi: 10.1142/S0218301316500336
Citations: PlumX Metrics

2015SU11      Nucl.Sci.Eng. 181, 272 (2015)

X.Su, Z.Zhang, Y.Han

Calculations and Evaluations of n + ^{113, 115, nat.}In Reactions up to 200 MeV

NUCLEAR REACTIONS ^113,115In, In(n, X), E<200 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Comparison with ENDF/B-VII, JENDL-4 and TENDL-2012 libraries.

doi: 10.13182/NSE15-1
Citations: PlumX Metrics

2015SU14      Int.J.Mod.Phys. E24, 1550092 (2015)

X.-W.Su, Y.-L.Han

Global optical model potential for alpha projectile

NUCLEAR REACTIONS ⁹Be, ¹²C, ¹⁶O, ^40,48Ca, ^58,60Ni, ^{112,116,120,124}Sn, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th(α, α), E<200 MeV; calculated σ; deduced optical model parameters.

doi: 10.1142/S0218301315500925
Citations: PlumX Metrics

2014SU19      Ann.Nucl.Energy 76, 469 (2014)

X.Su, Y.Han, C.Cai

Theoretical calculations of n+²³²Th reaction for energies up to 150 MeV

NUCLEAR REACTIONS ²³²Th(n, γ), (n, F), (n, 2n), (n, xn), E<150 MeV; calculated σ, σ(θ, E), σ(E). Comparison with ENDF/B-VII, JENDL-3.3 libraries, experimental data.

doi: 10.1016/j.anucene.2014.10.021
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2010SU14      Ann.Nucl.Energy 37, 1513 (2010)

X.Su, Y.Han

Calculation and analysis of n+^{90, 91, 92, 94, 96, nat}Zr reactions in the E_n ≤ 250 MeV

NUCLEAR REACTIONS ^{90,91,92,94,96}Zr, Zr(n, n), (n, n'), (n, γ), (n, 2n), (n, p), (n, α), (n, xn), (n, xp), (n, xα), (n, xd), E=0.1-250 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). The optical, Hauser-Feshbach, Iwamoto-Harada models. Comparison with ENDF/B-VII.0, ENDF/B-VI.8, JENDL-3.3 libraries.

doi: 10.1016/j.anucene.2010.06.011
Citations: PlumX Metrics

2010SU15      Nucl.Instrum.Methods Phys.Res. B268, 2585 (2010)

X.Su, H.Liang, Y.Han, C.Cai, Q.Shen

The theoretical calculation of p+²³²Th reaction for energies up to 250 MeV

NUCLEAR REACTIONS ²³²Th(p, n), (p, 2n), (p, 3n), (p, 6n), (p, xn), (p, xα), (p, xt), (p, F), (p, X), E<250 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Optical and Iwamoto-Harada models.

doi: 10.1016/j.nimb.2010.07.003
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2009DO21      Chin.Phys.C 33, 633 (2009)

J.-M.Dong, H.-F.Zhang, Y-Z.Wang, W.Zuo, X.-N.Su, J.-Q.Li

α-decay half-lives of superheavy nuclei and general predictions

NUCLEAR STRUCTURE Z=105-118; calculated α-decay T_1/2. Generalized liquid drop model (GLDM).

doi: 10.1088/1674-1137/33/8/007
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2009WA08      Chin.Phys.Lett. 26, 062101 (2009)

Y-Z.Wang, H.-F.Zhang, J.-M.Dong, X.-N.Su, W.Zuo, J.-Q.Li

Branching Ratios of α Decay for Nuclei near Deformed Shell Closures

RADIOACTIVITY ²⁷⁰Hs(α); Z=102-112; Calculated α-branching. Generalized Liquid Drop Model (GLDM).

doi: 10.1088/0256-307X/26/6/062101
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2009ZH18      Chin.Phys.Lett. 26, 072301 (2009)

H.-F.Zhang, J.-M.Dong, Y.-Z.Wang, X.-N.Su, Y.-J.Wang, L.-Z.Cai, T.-B.Zhu, B.-T.Hu, W.Zuo, J.-Q.Li

Theoretical Analysis and New Formulae for Half-Lives of Proton Emission

NUCLEAR STRUCTURE ¹⁰⁵Sb, ^145,147Tm, ^150,151Lu, ^155,156,157Ta, ^159,160,161Re, ^{164,165,166,167}Ir, ¹⁷¹Au, ¹⁷⁷Tl, ¹⁸⁵Bi; calculated proton radioactivity T_1/2; deduced formulae for T_1/2. comparison with experiment.

doi: 10.1088/0256-307X/26/7/072301
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Note: The following list of authors and aliases matches the search parameter X.Su: , X.D.SU, X.N.SU, X.W.SU