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NSR database version of May 10, 2024.

Search: Author = Yan Shiwei

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2024XI06      Phys.Rev. C 109, 035804 (2024)

W.Xian, S.Chen, S.Nikas, M.Rosenbusch, M.Wada, H.Ishiyama, D.Hou, S.Iimura, S.Nishimura, P.Schury, A.Takamine, S.Yan, F.Browne, P.Doornenbal, F.Flavigny, Y.Hirayama, Y.Ito, S.Kimura, T.M.Kojima, J.Lee, J.Liu, H.Miyatake, S.Michimasa, J.Y.Moon, S.Naimi, T.Niwase, T.Sonoda, D.Suzuki, Y.X.Watanabe, V.Werner, K.Wimmer, H.Wollnik

Mass measurements of neutron-rich A ≈ 90 nuclei constrain element abundances

doi: 10.1103/PhysRevC.109.035804
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2023II01      Phys.Rev.Lett. 130, 012501 (2023)

S.Iimura, M.Rosenbusch, A.Takamine, Y.Tsunoda, M.Wada, S.Chen, D.S.Hou, W.Xian, H.Ishiyama, S.Yan, P.Schury, H.Crawford, P.Doornenbal, Y.Hirayama, Y.Ito, S.Kimura, T.Koiwai, T.M.Kojima, H.Koura, J.Lee, J.Liu, S.Michimasa, H.Miyatake, J.Y.Moon, S.Naimi, S.Nishimura, T.Niwase, A.Odahara, T.Otsuka, S.Paschalis, M.Petri, N.Shimizu, T.Sonoda, D.Suzuki, Y.X.Watanabe, K.Wimmer, H.Wollnik

Study of the N=32 and N=34 Shell Gap for Ti and V by the First High-Precision Multireflection Time-of-Flight Mass Measurements at BigRIPS-SLOWRI

ATOMIC MASSES 55Sc, 56,58Ti, 56,57,58,59V; measured TOF; deduced masses, nonexistence of the N=34 empirical two-neutron shell gaps for Ti and V, and the enhanced energy gap in Ca. Comparison with new Monte Carlo shell model calculations. RIKEN's Radioactive Isotope Beam Factory (RIBF).

doi: 10.1103/PhysRevLett.130.012501
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2023SH06      Astrophys.J. 945, 41 (2023)

Y.Shen, B.Guo, R.J.deBoer, E.Li, Z.Li, Y.Li, X.Tang, D.Pang, S.Adhikari, C.Basu, J.Su, S.Yan, Q.Fan, J.Liu, C.Chen, Z.Han, X.Li, G.Lian, T.Ma, W.Nan, W.Nan, Y.Wang, S.Zeng, H.Zhang, W.Liu

New Determination of the 12C(α, γ)16O Reaction Rate and Its Impact on the Black-hole Mass Gap

NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; measured reaction products. 16O; deduced σ(θ), the asymptotic normalization coefficient (ANC) for the 16O ground state (GS), astrophysical S-factor and the stellar rate. The HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE) in Beijing, China.

doi: 10.3847/1538-4357/acb7de
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2023TO03      Phys.Rev. C 107, 054615 (2023)

L.Tong, S.Yan

Roles of pairing dynamics in fusion enhancement or suppression in 124Sn + 40, 48Ca and 132Sn + 58Ni reactions at sub-barrier energies

NUCLEAR REACTIONS 40,48Ca(124Sn, X), (132Sn, X), E(cm)=105-135 MeV; 58Ni(132Sn, X), E(cm)=150-200 MeV; calculated nucleus-nucleus interaction potentials, collective kinetic energies, real-space particle density distributions, reduced friction coefficients, internal excitation energies, reduced pairing energies, fusion σ(E). Real space density-constrained time-dependent Hartree-Fock-Bogoliubov (rDC-TDHFB) method. Comparison to experimental and other theoretical results.

doi: 10.1103/PhysRevC.107.054615
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2022TO01      Phys.Rev. C 105, 014613 (2022)

L.Tong, S.Yan

Real space density-constrained time-dependent Hartree-Fock-Bogoliubov method and pairing effects in the fusion of calcium isotopes

NUCLEAR REACTIONS 40,44,48Ca(40Ca, X), E(cm)=55 MeV; 44Ca(44Ca, X), E(cm)=53 MeV; calculated nucleus-nucleus interaction potentials for head-on collisions and fusion σ(E) using a real space density-constrained time-dependent Hartree-Fock-Bogoliubov (rDC-TDHFB) method with Gogny interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.105.014613
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2022TO10      Phys.Rev. C 106, 044611 (2022)

L.Tong, S.Yan

Microscopic investigations into fission dynamics beyond the saddle point

RADIOACTIVITY 240Pu(SF); calculated adiabatic and dynamical potentials for symmetric and asymmetric fission pathways along the quadrupole deformation Q20, the octupole Q30 and hexadecapole Q40 deformations before scission, proton and neutron number distribution in fragments, total pairing energies, the numbers of nucleon-transferring of asymmetric fission, proton and neutron pairing energies, proton and neutron spin-orbit energies, total kinetic energies TKE, collective accelerations of fission dynamics, internal excitation energies and deformation energies of fragments, total excitation energies. Real space density-constrained time-dependent Hartree-Fock-Bogoliubov (rDC-TDHFB) method with Gogny D1S interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.106.044611
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2021TO13      Phys.Rev. C 104, 064617 (2021)

L.Tong, R.He, S.Yan

Prediction of neutron-induced fission product yields by a straightforward k-nearest-neighbor algorithm

NUCLEAR REACTIONS 233,234,236,237,238U, 237,238Np, 238,239,240,241,242Pu, 241,243Am, 242,244,246,248Cm(n, F), E=0.4-2.0 MeV; analyzed mass distributions of fast neutron-induced fission products, and compared with evaluated experimental data in JENDL library. 232U(n, F), E=fast; predicted mass distributions of fast neutron-induced fission and compared with the recommended data of ENDF/B-VII.1 library. Machine learning algorithm for known fission product yields (FPYs) and predicted unknowns using k-nearest-neighbor algorithm (KNN) combined with a general description of the fission observable (GEF) method.

doi: 10.1103/PhysRevC.104.064617
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2018WA34      Yuan.Wul.Ping. 35, 445 (2018); Nucl.Phys.Rev. 35, 445 (2018)

Y.Wang, J.Su, Z.Han, B.Tang, B.Cui, T.Ge, Y.Lu, Z.Chen, B.Guo, X.Li, Y.Li, Z.Li, G.Lian, T.Ma, Y.Ma, Y.Shen, Y.Su, C.Wang, H.Wu, S.Yan, S.Zeng, Y.Zheng, C.Zhou, Y.Dang, G.Fu, Y.He, F.Liu, D.Wu, T.Zhang, W.Liu, for the BRIF collaboration

Study of the Exotic Decay Mode of 20Na with an Intense ISOL Beam

RADIOACTIVITY 20Na(β+α) [from 24Mg(p, nα), E<100 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced γ-ray energies and intensities, exotic β-γ-α decay mode.

doi: 10.11804/NuclPhysRev.35.04.445
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2017GU03      Phys.Rev. A 95, 022705 (2017)

D.L.Guo, X.Ma, S.F.Zhang, X.L.Zhu, W.T.Feng, R.T.Zhang, Y.Gao, B.Hai, M.Zhang, D.B.Qian, S.Yan, and P.Zhang

Dynamics of transfer ionization in p-He collisions at intermediate energies

NUCLEAR REACTIONS He(p, X), E=50-100 keV; measured reaction products, Eβ, Iβ; deduced that electron momentum distribution projected onto the scattering plane is consistent with the prediction of an independent two-step mechanism involving a binary encounter. Comparison with theoretical calculations.

doi: 10.1103/PhysRevA.95.022705
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2017ZH45      Nucl.Instrum.Methods Phys.Res. B412, 81 (2017)

J.P.Zhu, X.Xiao, S.Yan, Y.Gao, J.M.Xue, Y.G.Wang

Measurement of differential cross section of D(3He, p)4He from 0.8 MeV to 3.6 MeV

NUCLEAR REACTIONS 2H(3He, p), E=0.8-3.6 MeV; measured reaction products; deduced σ(θ). Comparison with available data.

doi: 10.1016/j.nimb.2017.07.020
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0089.


2015NI09      Phys.Lett. B 748, 89 (2015)

K.Nishio, A.N.Andreyev, R.Chapman, X.Derkx, Ch.E.Dullmann, L.Ghys, F.P.Hessberger, K.Hirose, H.Ikezoe, J.Khuyagbaatar, B.Kindler, B.Lommel, H.Makii, I.Nishinaka, T.Ohtsuki, S.D.Pain, R.Sagaidak, I.Tsekhanovich, M.Venhart, Y.Wakabayashi, S.Yan

Excitation energy dependence of fragment-mass distributions from fission of 180, 190Hg formed in fusion reactions of 36Ar + 144, 154Sm

NUCLEAR REACTIONS 144,154Sm(36Ar, X)180Hg/190Hg, E=148-198 MeV; measured reaction products; deduced fission fragment mass and total kinetic-energy distributions. Comparison with available data.

doi: 10.1016/j.physletb.2015.06.068
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2015WE11      J.Radioanal.Nucl.Chem. 305, 455 (2015)

Z.Wei, Z.Yao, C.Lan, J.Chen, Y.Yan, Y.Shi, S.Yan, J.Wang, J.Wang

Monte Carlo simulation of fission yields, kinetic energy, fission neutron spectrum and decay γ-ray spectrum for 232Th(n, f) reaction induced by 3H(d, n) 4He neutron source

NUCLEAR REACTIONS 232Th(n, F), E<20 MeV; calculated fission neutron yields, average kinetic energy, fission neutron and γ-ray spectra. Comparison with ENDF/B-VII.1 evaluated nuclear library, available data.

doi: 10.1007/s10967-014-3910-7
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2014JI07      Phys.Rev. C 90, 024612 (2014)

X.Jiang, S.Yan

Effects of large mass transfer and statistical decay on ternary breakup in the reaction 238U + 197Au at 15A MeV

NUCLEAR REACTIONS 197Au(238U, F), E=15 MeV/nucleon; calculated fragment multiplicity, fragment mass and charge, binary, ternary, quaternary and quinary breakup probabilities as a function of impact parameter, total kinetic energy. Hybrid model combining the improved quantum molecular dynamics (ImQMD) model with statistical code GEMINI++. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.024612
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2014JI17      Phys.Rev. C 90, 064618 (2014)

X.Jiang, J.A.Maruhn, S.Yan

Microscopic study of noncentral effects in heavy-ion fusion reactions with spherical nuclei

NUCLEAR REACTIONS 16O(16O, X), E(cm)=12, 20 MeV; 40Ca(40Ca, X), E(cm)=56, 58, 60, 70, 100, 48-75 MeV; 90Zr(40Ca, X), E(cm)=100, 110, 120, 180, 300 MeV; calculated time evolution of the moment of inertia for 16O+16O reaction, time evolution of the quadrupole moments, penetration probability as a function of impact parameter, and fusion σ(E) for 40Ca+40Ca reaction, N-N potentials and collective kinetic energies, effective mass parameters for head-on collisions and for various impact parameters. Three dimensional time-dependent Hartree-Fock approach (TDHF) with and without density constraint. Comparison with available experimental data.

doi: 10.1103/PhysRevC.90.064618
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2013HE08      Phys.Rev. C 87, 034320 (2013), Erratum Phys.Rev. C 102, 029903 (2020)

C.He, S.Shen, S.Wen, L.Zhu, X.Wu, G.Li, Y.Zhao, Y.Yan, Z.Bai, Y.Wu, Y.Li, G.Li, S.Yan, M.Oshima, Y.Toh, A.Osa, M.Koizumi, Y.Hatsukawa, M.Matsuda, T.Hagakawa

Signature splitting inversion and backbending in 80Rb

NUCLEAR REACTIONS 65Cu(19F, 3np), E=75 MeV; 66Zn(18O, 3np), E=76 MeV; 68Zn(16O, 3np), E=80 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at CIAE and JAERI facilities. 80Rb; deduced high-spin levels, J, π, bands, alignments, signature splitting and inversion. Comparison with structures of 78Rb and 82Y nuclei. Calculated total Routhian surface (TRS) plots. Projected shell-model calculations.

doi: 10.1103/PhysRevC.87.034320
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013JI17      Phys.Rev. C 88, 044611 (2013)

X.Jiang, S.Yan, J.A.Maruhn

Dynamics of energy dissipation in heavy-ion fusion reactions

NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=55, 100 MeV; 64Ni(64Ni, X), E(cm)=95, 190 MeV; 90Zr(90Zr, X), E(cm)=195, 300 MeV; 120Sn(120Sn, X), E(cm)=300, 500 MeV; calculated relative distance, quadrupole moment, nuclear stopping power as function of time, dynamic interaction potentials, dynamic reduced mass parameters, friction coefficients, relative distance dependence of the nucleons transferred, energies dissipated. Role of nucleon-nucleon two-body collisions in energy dissipation. Improved quantum molecular dynamics (ImQMD) model.

doi: 10.1103/PhysRevC.88.044611
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2013LI16      Nucl.Phys. A902, 1 (2013)

Y.Li, S.Yan, X.Jiang, L.Wang

Dynamical effects in heavy-ion induced ternary breakup

NUCLEAR REACTIONS 40Ca(40Ca, X), 58Ni(58Ni, X), 100Mo(100Mo, X), 120Sn(120Sn, X), 197Au(197Au, X), 238U(238U, X), E≈15 MeV/nucleon; calculated fragments σ, ternary fission fragments σ using ImQMD model; deduced probability of cascade and direct ternary fission vs impact parameter, momentum anisotropy ratio. 100Mo+100Mo deduced nucleon number asymmetry vs impact parameter and vs incident energy, Comparison with available data and momentum anisotropy also with Jain calculation.

doi: 10.1016/j.nuclphysa.2013.02.015
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2013WA26      Nucl.Phys. A920, 1 (2013)

L.Wang, S.Yan, Y.Li, X.Jiang

Odd-even and nonequilibrium effects in multifragmentation of 56Fe on C, Al targets at 471 A MeV

NUCLEAR REACTIONS C, Al(56Fe, X), E=471 MeV/nucleon; calculated fragment σ, charge and mass distribution, σ(θ), time development of density distribution using ImQMD (Improved QMD) with statistical GEMINI model.Compared to data.

doi: 10.1016/j.nuclphysa.2013.10.007
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2012KH11      Phys.Rev. C 86, 064602 (2012)

J.Khuyagbaatar, K.Nishio, S.Hofmann, D.Ackermann, M.Block, S.Heinz, F.P.Hessberger, K.Hirose, H.Ikezoe, B.Kinlder, B.Lommel, H.Makii, S.Mitsuoka, I.Nishinaka, T.Ohtsuki, Y.Wakabayashi, S.Yan

Evidence for hindrance in fusion between sulfur and lead nuclei

NUCLEAR REACTIONS 204,206,208Pb(34S, F), (36S, F), E=160-200 MeV; measured fission fragments, fission and ER σ at JAEA facility. Comparison with coupled-channel (HIVAP) calculations. Influence of coupling to the vibrational states in 34S.

doi: 10.1103/PhysRevC.86.064602
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2413.


2012WA22      Acta Phys.Pol. B43, 1769 (2012)

L.-C.Wang, D.-H.Zhang, S.Yan, Y.-J.Li, J.-X.Cheng, J.-S.Li, S.Kodaira, N.Yasuda

Fragmentation Cross Sections of 56Fe at 471 A MeV on Al, C and CH2 Targets

NUCLEAR REACTIONS Al, C(56Fe, X), E=471 MeV/nucleon; measured reaction products; deduced fragmentation total and partial charge-changing σ. Comparison with available data.

doi: 10.5506/APhysPolB.43.1769
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2010TI01      Int.J.Mod.Phys. E19, 307 (2010)

J.Tian, X.Li, S.Yan, Z.Wu, Z.Li

Kinematic correlation of the ternary fission for the system 197Au + 197Au

NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; measured reaction fragments; deduced mass number distributions, dynamical modes of ternary fission.

doi: 10.1142/S0218301310014777
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2010TI07      Phys.Rev. C 82, 054608 (2010)

J.Tian, X.Wu, Z.Li, K.Zhao, Y.Zhang, X.Li, S.Yan

Mechanism of ternary breakup in the reaction 197Au+197Au at 15A MeV

doi: 10.1103/PhysRevC.82.054608
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2007RA22      Eur.Phys.J. A 32, 51 (2007)

F.Raiola, T.Spillane, B.Limata, B.Wang, S.Yan, M.Aliotta, H.W.Becker, J.Cruz, M.Fonseca, L.Gialanella, A.P.Jesus, K.U.Kettner, R.Kunze, H.Luis, J.P.Ribeiro, C.Rolfs, M.Romano, D.Schurmann, F.Strieder

First hint on a change of the 210Po alpha-decay half-life in the metal Cu

RADIOACTIVITY 210Po(α); measured Eα, Iα, T1/2 as a function of temperature by implanting Po ions in cooled metallic copper.

doi: 10.1140/epja/i2007-10012-8
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2006LI34      Eur.Phys.J. A 28, 251 (2006)

B.Limata, F.Raiola, B.Wang, S.Yan, H.W.Becker, A.D'Onofrio, L.Gialanella, V.Roca, C.Rolfs, M.Romano, D.Schurmann, F.Strieder, F.Terrasi

First hints on a change of the 22Na β+-decay half-life in the metal Pd

RADIOACTIVITY 22Na(β+) [from 19F(α, n)]; measured T1/2 for source implanted in Pd metal; deduced shorter T1/2 due to environmental effects.

doi: 10.1140/epja/i2006-10057-1
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2006WA21      Eur.Phys.J. A 28, 375 (2006)

B.Wang, S.Yan, B.Limata, F.Raiola, M.Aliotta, H.W.Becker, J.Cruz, N.De Cesare, A.D'Onofrio, Z.Fulop, L.Gialanella, G.Gyurky, G.Imbriani, A.Jesus, J.P.Ribeiro, V.Roca, D.Rogalla, C.Rolfs, M.Romano, D.Schurmann, E.Somorjai, F.Strieder, F.Terrasi

Change of the 7Be electron capture half-life in metallic environments

RADIOACTIVITY 7Be(EC) [7Li(p, n)]; measured T1/2 for source implanted in Pd, In metals and Li2O insulator; deduced longer T1/2 due to environmental effects in the metals, no change in the insulator.

doi: 10.1140/epja/i2006-10068-x
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2005LI40      Nucl.Phys. A758, 110c (2005)

W.Liu, Z.Li, X.Bai, G.Lian, B.Guo, S.Zeng, S.Yan, B.Wang, N.Shu, K.Wu, Y.Chen

Nuclear Astrophysics Experiments at CIAE

NUCLEAR REACTIONS 2H(7Be, n), (11C, n), (8Li, p), E ≈ 5.8-9.8 MeV; measured σ(θ), total σ; deduced astrophysical S-factors.

doi: 10.1016/j.nuclphysa.2005.05.164
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2003LI51      Nucl.Phys. A728, 275 (2003)

W.Liu, Z.Li, X.Bai, B.Guo, S.Zeng, Y.Chen, S.Yan, B.Wang, G.Lian, Y.Lu, K.Wu, N.Shu

Determination of 11C(p, γ) 12N astrophysical S-factor via measurement of 11C(d, n)12N reaction

NUCLEAR REACTIONS 2H(11C, 12N), E(cm)=9.8 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 11C(p, γ), E=low; deduced astrophysical S-factor, reaction mechanism features. DWBA analysis.

doi: 10.1016/j.nuclphysa.2003.08.017
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0053.


1996DU11      Nucl.Instrum.Methods Phys.Res. A369, 424 (1996)

H.Du, Y.Liu, J.Li, S.Yan, G.Li, Y.Zhu, L.Yao

Progress in Preparation 4πβ Quantitative Sources

RADIOACTIVITY 60Co(β-); measured βγ-coin; deduced detector plateau-characteristics.

doi: 10.1016/S0168-9002(96)80023-4
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1993ZH01      Z.Phys. A344, 251 (1993)

J.Zhang, S.Yan, C.Wang

The Pick-Up Mechanism in Composite Particle Emission Processes

NUCLEAR REACTIONS 27Al, 51V, 59Co, 93Nb, 115In, 139La, 181Ta, 209Bi(n, t), E ≈ 15-20 MeV; calculated reaction σ(E). Exciton model with nucleon-pickup mechanism.


1992WA21      Chin.J.Nucl.Phys. 14, No 1, 87 (1992)

S.Wang, S.Yan, C.Wang, Z.Su

Sensitivity of Nuclear Level Density Parameters

NUCLEAR REACTIONS 197Au(n, γ), E ≤ 10 MeV; 197Au(n, n'), (n, 2n), E ≤ 20 MeV; calculated σ(E); deduced level density parameter dependence. Statistical, preequilibrium models.


1992ZH39      Chin.J.Nucl.Phys. 14, No 4, 345 (1992)

J.Zhang, S.Yan, C.Wang

The Pick-Up Mechanism in Composite Particle Emission Processes

NUCLEAR REACTIONS 27Al, 51V, 59Co, 93Nb, 115In, 139La, 181Ta, 209Bi(n, t), E ≈ 15-20 MeV; calculated σ(E). Exciton model.


1987SH07      Chin.J.Nucl.Phys. 9, 16 (1987)

Shi Xiangjun, Yan Shiwei, Zhang Jingshang

Statistical Theoretical Calculation of the Double Differential Cross Sections and Secondary Neutron Energy Spectra for 238U(n, n') Reaction

NUCLEAR REACTIONS 238U(n, n'), E=14.2 MeV; calculated σ(En', θn'). Preequilibrium statistical theory, evaporation model.


1986WE10      Z.Phys. A324, 325 (1986)

Wen Yuanqi, Shi Xiangjun, Yan Shiwei, Zhuo Yizhong, Han Huiyi

A Semi-Classical Model of Multi-Step Direct and Compound Nuclear Reactions

NUCLEAR REACTIONS 197Au, 120Sn(p, p'), E=62 MeV; 93Nb(n, n'), E=14.6 MeV; calculated σ(θ, Ep), σ(θ, En). Semi-classical model, multi-step direct, compound nuclear reactions.


1986WE14      Chin.J.Nucl.Phys. 8, 9 (1986)

Wen Yuanqi, Han Huiyi, Shi Xiangjun, Yan Shiwei, Zhuo Yizhong

The Multi-Step Energy Correlation of Exciton Model and the Calculation of Double Differential Cross Section

NUCLEAR REACTIONS 93Nb(n, n'), E=15 MeV; 120Sn, 197Au(p, p'), E=62 MeV; calculated σ(θn, En), σ(θp, Ep). Exciton model, multi-step energy correlation.


1980LI23      J.Nucl.Radiochem. 2, 1 (1980)

Z.Li, S.Yan

The absolute determination of cumulative yield of several nuclides from thermal neutron and fission spectrum neutron induced fission of 235U

NUCLEAR REACTIONS 235U(n, F)95Zr/99Mo/144Ce, E thermal; measured reaction products by radiochemical technique; deduced cumulative fission yields.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32633.


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