NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Bao Found 50 matches. 2024CH17 Eur.Phys.J. A 60, (2024) Y.Chen, Y.Qiu, Q.Li, Sh.Tang, Y.Yang, Zh.Ren, W.Jiang, R.Fan, H.Yi, R.Liu, J.Tang, H.Jing, Ch.Lan, Y.Li, Zh.Tan, Q.An, J.Bai, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Zh.Chen, Z.Cui, Ch.Feng, K.Gao, X.Gao, M.Gu, Ch.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, H.Huang, X.Huang, H.Jiang, Zh.Jiang, L.Kang, B.Li, Ch.Li, J.Li, X.Li, J.Liu, Sh.Liu, X.Liu, Z.Long, G.Luan, Ch.Ning, M.Niu, B.Qi, J.Ren, X.Ruan, Zh.Song, K.Sun, Zh.Sun, X.Tang, B.Tian, L.Wang, P.Wang, Zh.Wang, Zh.Wen, X.Wu, X.Wu, L.Xie, X.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Zh.Zhang, L.Zhou, Zh.Zhou, K.Zhu Measurement of the neutron flux of CSNS Back-n ES#1 under small collimators from 0.5 eV to 300 MeV NUCLEAR REACTIONS 235U(n, F), 6Li(n, X), E=0.0000005-300 MeV; measured reaction products, En, In, TOF; deduced σ, neutron flux and uncertainties. China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-024-01272-z
2023QI03 Phys.Rev. C 107, 024606 (2023) Y.Qiu, C.Lan, Y.Chen, L.Jiang, J.Bao, Y.Yang, Z.Wen, R.Liu, X.Ruan, J.Tang, J.Ren, H.Jing, G.Luan, R.Fan, Y.Nie, X.Yang, X.Li, H.Yi, W.Jiang, T.Ye, Y.Yang, S.Liu, J.Wang Measurement of the 239Pu(n, f) cross section from 4 keV to 100 MeV using the white neutron source at the CSNS Back-n facility NUCLEAR REACTIONS 235U, 239Pu(n, F), E=0.004-100 MeV; measured neutron ToF, En, fission fragments; deduced fission σ(E) for 239Pu(n, F) relative to known σ(e) for 235U(n, F) reaction. Comparison to CENDL-3.2, ENDF/B-VIII.0, JENDL-4.0/HE, JEFF-3.3 and BROND-3.1 evaluations, other experimental data and TALYS-1.95 calculations. Fast fission ionization chamber for the fission cross section measurement (FIXM). Neutrons from 1.6 GeV proton beam impinging on thick W-target at the China Spallation Neutron Source (CSNS).
2023WA35 Eur.Phys.J. A 59, 224 (2023) J.Wang, J.Ren, W.Jiang, X.Ruan, Q.Sun, J.Hu, B.Jiang, J.Bao, Q.Zhang, G.Luan, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, J.Bai, P.Cao, Q.Chen, Y.Chen, Z.Chen, Z.Cui, A.Fan, R.Fan, C.Feng, F.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, W.Jia, H.Jiang, Z.Jiang, Z.Jin, L.Kang, B.Li, C.Li, G.Li, J.Li, Q.Li, Y.Li, J.Liu, R.Liu, S.Liu, C.Ning, B.Qi, Z.Ren, Z.Song, K.Sun, Z.Tan, J.Tang, S.Tang, L.Wang, P.Wang, Z.Wang, Z.Wen, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, Y.Yu, G.Zhang, L.Zhang, M.Zhang, X.Zhang, Y.Zhang, Y.Zhang, Z.Zhang, M.Zhao, L.Zhou, K.Zhu, J.Zhang Determination of the 232Th(n, γ) cross section from 10 to 200 keV at the Back-n facility at CSNS NUCLEAR REACTIONS 232Th, 197Au(n, γ), E=10-200 keV; measured reaction products, En, In, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, CENDL-3.2, JENDL-5 libraries and TALYS 1.96 calculations. The back-streaming white neutron beam-line (Back-n) of China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-023-01126-0
2022ZH04 Phys.Rev. C 105, 014604 (2022) D.Zhang, Y.Li, J.Bao, C.Fu, M.Guan, Y.He, X.Ji, H.Jia, Y.Li, J.Liu, J.Xia, W.Xiong, J.You, C.Yuan, N.Zhou 83Rb/83mKr production and cross-section measurement with 3.4 MeV and 20 MeV proton beams NUCLEAR REACTIONS Kr(p, n)83Rb/84Rb/86Rb, E=3.4 MeV beam from China Institute of Atomic Energy; Kr(p, n), E=20 MeV beam from Institute of Modern Physics; measured Eγ, Iγ, total generated radioactivities and thick-target yields for rubidium isotope. 83mKr/83Rb; measured production rate of 83mKr from 83Rb decay; produced 83mKr yielded enough statistics for detector calibration injected into the PandaX-II liquid xenon detector for dark matter studies. Relevance to calibration source such as short half-life 83mKr for liquid xenon or liquid argon detectors in experiments dealing with search for dark matter.
doi: 10.1103/PhysRevC.105.014604
2021LI35 Eur.Phys.J. A 57, 232 (2021); Erratum Eur.Phys.J. A 57, 252 (2021) X.Liu, Y.Yang, R.Liu, Z.Wen, J.Wen, Z.Han, Y.Chen, H.Jing, H.Yi, J.Bao, Z.Ren, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS NUCLEAR REACTIONS 27Al(n, X), E<20 MeV; measured reaction products, En, In; deduced neutron transmission, total σ and uncertainties. Comparison withENDF/B-VIII.0, JEFF-3.3 and CENDL-3.2 library evaluations, EXFOR compilations. Spallation Neutron Source Science Center.
doi: 10.1140/epja/s10050-021-00513-9
2021RE01 Nucl.Instrum.Methods Phys.Res. A985, 164703 (2021) J.Ren, X.Ruan, W.Jiang, J.Bao, G.Luan, Q.Zhang, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, Z.Cui, R.Fan, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, Q.Mu, C.Ning, B.Qi, Z.Ren, Y.Song, Z.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Background study for (n, γ) cross section measurements with C6D6 detectors at CSNS Back-n NUCLEAR REACTIONS 197Au, Pb, C, 181Ta, 59Co(n, γ), E<400 MeV; measured reaction products, Eγ, Iγ; deduced σ.
doi: 10.1016/j.nima.2020.164703
2020BA03 Chin.Phys.C 44, 014003 (2020) H.Bai, R.Fan, H.Jiang, Z.Cui, Y.Hu, G.Zhang, Z.Chen, W.Jiang, H.Yi, J.Tang, L.Zhou, Q.An, J.Bao, P.Cao, Q.Chen, Y.Chen, P.Cheng, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the differential cross sections and angle-integrated cross sections of the 6Li(n, t)4He reaction from 1.0 eV to 3.0 MeV at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), E=0.000001-3 MeV; measured reaction products; deduced σ. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries, experimental data.
doi: 10.1088/1674-1137/44/1/014003
2020JI06 Nucl.Instrum.Methods Phys.Res. A973, 164126 (2020) W.Jiang, H.Bai, H.Jiang, H.Yi, R.Fan, G.Zhang, J.Tang, Z.Sun, C.Ning, K.Sun, K.Gao, Z.Cui, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Y.Song, Z.Song, H.Sun, X.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Application of a silicon detector array in (n, lcp) reaction cross-section measurements at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), 10B(n, α), E<1 MeV; measured reaction products, En, In; deduced σ. Comparison with experimental data, ENDF/B-VIII.0, JEFF-3.3, ROSFOND evaluated libraries.
doi: 10.1016/j.nima.2020.164126
2020LI33 Nucl.Instrum.Methods Phys.Res. A980, 164506 (2020) Q.Li, H.Jing, B.Zhou, C.Ning, J.Tang, J.Ren, H.Yi, X.Zhu, L.Zhang, W.Jiang, R.Fan, J.Bao, C.Feng, X.Ruan, Y.Chen, L.Zhou, Y.Li, Z.Tan, Y.Chen, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, L.Kang, M.Kang, B.Li, L.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, B.Qi, Z.Song, H.Sun, X.Sun, Z.Sun, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron and γ background measurements of the experimental halls at the CSNS back-streaming white neutron source
doi: 10.1016/j.nima.2020.164506
2020RE11 Phys.Rev. C 102, 034604 (2020) Z.Ren, Y.Yang, J.Wen, H.Guo, Z.Wen, R.Liu, Z.Han, W.Sun, X.Liu, Q.Chen, T.Ye, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the 236U(n, f) cross section for neutron energies from 0.4 MeV to 40 MeV from the back-streaming white neutron beam at the China Spallation Neutron Source NUCLEAR REACTIONS 235,236U(n, F), E AP 0.4-40 MeV beam from the China Spallation Neutron Source (CSNS)-Back-streaming white neutron source (WNS); measured fission fragments, energy spectra, time-of-flight using Fast Ionization Chamber Spectrometer; deduced 236U(n, F)/235U(n, F) cross section ratios. Comparison with theoretical calculation using the UNF code, and with evaluated data in JENDL-4.0, CENDL-3.1, and ENDF/B-VIII.0 libraries.
doi: 10.1103/PhysRevC.102.034604
2020WE04 Ann.Nucl.Energy 140, 107301 (2020) J.Wen, Y.Yang, Z.Wen, R.Liu, X.Liu, Z.Han, Q.Chen, Z.Ren, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the U-238/U-235 fission cross section ratio at CSNS - Back-in WNS NUCLEAR REACTIONS 235,238U(n, F), E=1-20 MeV; measured reaction products, fission fragments, Eγ, Iγ; deduced neutron resonances, σ. Comparison with ENDF/B-VIII.0 library evaluations.
doi: 10.1016/j.anucene.2019.107301
2019CH37 Eur.Phys.J. A 55, 115 (2019), Erratum Eur.Phys.J. A 55, 145 (2019) Y.Chen, G.Luan, J.Bao, H.Jing, L.Zhang, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, Ch.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron energy spectrum measurement of the Back-n white neutron source at CSNS
doi: 10.1140/epja/i2019-12808-1
2019JI07 Chin.Phys.C 43, 124002 (2019) H.Jiang, W.Jiang, H.Bai, Z.Cui, G.Zhang, R.Fan, H.Yi, C.Ning, L.Zhou, J.Tang, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Z.Song, Y.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurements of differential and angle-integrated cross sections for the 10B(n, α)7Li reaction in the neutron energy range from 1.0 eV to 2.5 MeV NUCLEAR REACTIONS 10B(n, α), E=0.000001-2.5 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ and uncertainties. Comparison with ENDF/B-VIII.0, JEFF-3.3, CENDL-3.1 and JENDL 4.0 libraries.
doi: 10.1088/1674-1137/43/12/124002
2017ZH48 Phys.Rev. C 96, 055801 (2017) X.Zhang, J.Zhao, D.Yuan, C.Fu, J.Bao, L.Chen, J.He, L.Hou, L.Li, Y.Li, Y.Li, G.Liao, Y.Rhee, Y.Sun, S.Xu, G.Zhao, B.Zhu, J.Zhu, Z.Zhang, J.Zhang Deuteron-deuteron fusion in laser-driven counter-streaming collisionless plasmas NUCLEAR REACTIONS 2H(d, n)3He, E(cm)<45 keV; measured E(n), I(n), time-of-flight spectra using scintillation detectors, and head-on-head collision of plasma streams driven by nanosecond pulse lasers at the National Laboratory on High Power Lasers and Physics, Shanghai; deduced neutron yield. Implications for reactions in plasma environments in astrophysical conditions.
doi: 10.1103/PhysRevC.96.055801
2016LA09 Nucl.Instrum.Methods Phys.Res. B375, 8 (2016) C.Lan, X.Ruan, G.Chen, Y.Nie, H.Huang, J.Bao, Z.Zhou, H.Tang, X.Kong, M.Peng Measurement of secondary neutron emission double-differential cross sections for 9Be induced by 21.65 ± 0.07 MeV neutrons NUCLEAR REACTIONS 9Be(n, xn), E=21.65 MeV; measured reaction products, En, In; deduced σ, σ(θ, E). Comparison with statistical Hauser-Feshbach model and the angular momentum dependent exciton model calculations.
doi: 10.1016/j.nimb.2016.03.027
2015HA09 Nucl.Phys. A936, 17 (2015) R.Han, R.Wada, Z.Chen, Y.Nie, X.Liu, S.Zhang, P.Ren, B.Jia, G.Tian, F.Luo, W.Lin, J.Liu, F.Shi, M.Huang, X.Ruan, J.Ren, Z.Zhou, H.Huang, J.Bao, K.Zhang, B.Hu Fast neutron scattering on Gallium target at 14.8 MeV NUCLEAR REACTIONS 69,71Ga(n, n), (n, n'), E≈14.8 MeV; measured En, In(θ); deduced σ, σ(θ). 69,71Ga(n, n), (n, n'), (n, 2n), (n, np), (n, nα), E=0-15 MeV; calculated σ, σ(θ), using TALYS and MCNP. Compared with experimental data and databases.
doi: 10.1016/j.nuclphysa.2015.01.004
2014LI04 Phys.Rev. C 89, 024604 (2014) Neutron emission in the fusion process and its effect on the formation of superheavy nuclei NUCLEAR REACTIONS 238U(48Ca, 3n), (48Ca, 4n)E(cm)=185-215 MeV; 249Cf(50Ti, 3n), (50Ti, 4n), E(cm)=238 MeV; calculated precompound neutron multiplicity, fusion probabilities as function of excitation energy and angular momentum, σ(Ex), σ for evaporation residues. Superheavy elements. Fusion dynamics treated with Langevin equations coupled with neutron emission process.
doi: 10.1103/PhysRevC.89.024604
2013LI15 Phys.Rev. C 87, 034616 (2013) Possibility to produce element 120 in the 54Cr+248Cm hot fusion reaction NUCLEAR REACTIONS 249Cf(50Ti, 3n)120296, 248Cm(54Cr, 4n)120298, E*=20-60 MeV; calculated fusion and survival probabilities, evaporation residue cross sections, hot fusion reaction. Modified fusion by diffusion model, two-dimensional coupled Langevin equations. Comparison with earlier studies on the same and other fusion reactions.
doi: 10.1103/PhysRevC.87.034616
2012LI23 Phys.Rev. C 85, 057603 (2012) Cold fusion reaction of 58Fe + 208Pb analyzed by a generalized model of fusion by diffusion NUCLEAR REACTIONS 208Pb(58Fe, n)265Hs, E=212-228 MeV; calculated fusion probability distribution, σ(E). Fusion by Diffusion (FBD) model, coupled Langevin equations. Formation of superheavy nuclei in cold fusion reactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.057603
2011LI10 Phys.Rev. C 83, 044613 (2011) Role of the coupling between neck and radial degrees of freedom in evolution from dinucleus to mononucleus NUCLEAR REACTIONS 249Cf(50Ti, 3n)296120, (50Ti, 4n)295120, E=235, 245 MeV; calculated radial momentum distribution, transition time distribution, deterministic velocities of neck growth, probability distribution of sin, and σ(ER) using coupled Langevin equations in two-dimensional collective space. Dynamics of neck growth, and the evolution from dinucleus to mononucleus.
doi: 10.1103/PhysRevC.83.044613
2011LI37 Phys.Rev. C 84, 031602 (2011) Calculation of the evaporation residue cross sections for the synthesis of the superheavy element Z = 119 via the 50Ti+ 249Bk hot fusion reaction NUCLEAR REACTIONS 249Bk(50Ti, 3n)296119, (50Ti, 4n)295119, E=225, 230 MeV; calculated evaporation residue cross sections. Fusion-by-diffusion model. Discussed possibilities of identification of Z=119 element.
doi: 10.1103/PhysRevC.84.031602
2011RU13 J.Korean Phys.Soc. 59, 1729s (2011) X.C.Ruan, G.C.Chen, H.X.Huang, X.Li, Y.B.Nie, B.Zhou, Z.Y.Ma, J.Bao, Q.P.Zhong, Z.Y.Zhou, H.Q.Tang, J.S.Zhang, C.L.Lan, Y.L.Zhang, Y.M.Li Measurement of the Secondary Neutron Emission Differential and Double-Differential Cross Sections between 20 and 30 MeV NUCLEAR REACTIONS 9Be(n, n), (n, xn), E=21.65 MeV; measured In, En using TOF and BC501A; deduced σ, σ(θ), σ(E, θ); calculated TOF neutron spectra using Monte Carlo code STREUER, σ by LUNF code. Compared with other data.
doi: 10.3938/jkps.59.1729
2010LI12 Phys.Rev. C 81, 044606 (2010) Systematical calculations of the 136Xe(136Xe, xn)272-xHs reaction: Effects of quasifission in the early stage of the fusion process NUCLEAR REACTIONS 136Xe(136Xe, xn)268Hs/269Hs/270Hs/271Hs/, E=310, 330 MeV; calculated radial potential, capture probability, radial momentum distributions, fusion probability, σ, and quasifission probability using fusion-by-diffusion model.
doi: 10.1103/PhysRevC.81.044606
2010NI11 Ann.Nucl.Energy 37, 1456 (2010) Y.Nie, J.Bao, X.Ruan, H.Huang, X.Li, Q.Zhong, B.Zhou, Z.Ma, Y.Zhang, Z.Zhou Benchmarking of evaluated nuclear data for uranium by a 14.8 MeV neutron leakage spectra experiment with slab sample
doi: 10.1016/j.anucene.2010.06.018
2009CH39 Nucl.Sci.Eng. 163, 272 (2009) G.Chen, X.Ruan, Z.Zhou, J.Zhang, B.Qi, X.Li, H.Huang, H.Tang, Q.Zhong, J.Jiang, B.Xin, J.Bao, L.Chen Double-Differential Neutron Emission Cross-Section Measurements of 6Li and 7Li at Incident Neutron Energies of 8.17 and 10.27 MeV NUCLEAR REACTIONS 6,7Li(n, xn), (n, n), (n, n'), E = 8.17, 10.27 MeV; measured En, In using TOF; deduced σ(θ, E). Comparison with Monte Carlo simulation.
doi: 10.13182/NSE163-272
2009LI37 Phys.Rev. C 80, 034601 (2009) Optimal reaction for synthesis of superheavy element 117 NUCLEAR REACTIONS 249Bk(48Ca, 3n)294Ts, E(cm)=200-220 MeV; 250Bk(48Ca, 4n)294Ts, E=200-220 MeV; 245,246,247,248Bk(48Ca, X)293Ts/294Ts/295Ts/296Ts/297Ts/298Ts, E not given; 243Am(50Ti, X), E not given; 238U(55Mn, X), E not given; calculated σ and compound nucleus formation probability using diffusion process and Smoluchowski partial differential equations.
doi: 10.1103/PhysRevC.80.034601
2009LI52 Phys.Rev. C 80, 054608 (2009) Synthesis of superheavy element 120 via 50Ti+ACf hot fusion reactions NUCLEAR REACTIONS 249,250,251,252Cf(50Ti, 3n), (50Ti, 4n), E not given; calculated capture and fusion σ, and survival probability for evaporation residues (ER) using fusion-by-diffusion model. 302120; estimated fusion probability for the formation of superheavy nucleus.
doi: 10.1103/PhysRevC.80.054608
2008WA05 Phys.Rev. C 77, 024603 (2008) Optimal path of diffusion over the saddle point and fusion of massive nuclei
doi: 10.1103/PhysRevC.77.024603
2007JI06 Phys.Rev. C 75, 034601 (2007) Calculations of the anisotropy of the fission fragment angular distribution and neutron emission multiplicities prescission from Langevin dynamics NUCLEAR REACTIONS 208Pb, 232Th, 238U(16O, nF), E ≈ 80-300 MeV; 209Bi(20Ne, nF), E ≈ 140-220 MeV; calculated pre-scission neutron multiplicities, fission fragment anisotropies. Two-dimensional realistic coupled Langevin equations.
doi: 10.1103/PhysRevC.75.034601
2007LI03 Chin.Phys.Lett. 24, 393 (2007) Origin of Unexpected Isotopic Trends in Synthesis of Superheavy Nuclei NUCLEAR REACTIONS 208Pb(64Zn, n), (66Zn, n), (67Zn, n), (68Zn, n), (72Ge, n), (73Ge, n), (74Ge, n), (58Ni, xn), (60Ni, xn), (62Ni, xn), (64Ni, xn), 207,208Pb(70Zn, n), (76Ge, n), E* ≈ 8-20 MeV; calculated evaporation residue σ; deduced dependence on neutron excess. Comparison with data.
doi: 10.1088/0256-307X/24/2/025
2007LI53 Phys.Rev. C 76, 034604 (2007) Isotopic dependence of the evaporation residue cross section in the synthesis of superheavy nuclei
doi: 10.1103/PhysRevC.76.034604
2007RU11 Phys.Rev. C 75, 057001 (2007) X.C.Ruan, Z.Y.Zhou, X.Li, J.Jiang, H.X.Huang, Q.P.Zhong, H.Q.Tang, B.J.Qi, J.Bao, B.Xin, W.von Witsch, H.Witala Experimental study of neutron-neutron quasifree scattering in the nd breakup reaction at 25 MeV NUCLEAR REACTIONS 2H(n, X), E=25 MeV; measured yields and neutron-neutron quasi free scattering cross section. Compared results to model calculations.
doi: 10.1103/PhysRevC.75.057001
2006BA72 Int.J.Mod.Phys. E15, 1625 (2006) Neck formation in fusion dynamics of massive nuclei NUCLEAR REACTIONS 100Mo, 110Pd(100Mo, X), 123Sb(86Kr, X), 124Sn(96Zr, X), E(cm) ≈ 180-280 MeV; calculated fusion probability, role of neck formation.
doi: 10.1142/S0218301306004910
2006LI20 Chin.Phys.Lett. 23, 1437 (2006) Isotope Dependence of Superheavy Nucleus Formation Cross Section NUCLEAR REACTIONS 204Pb(54Fe, X), 206Pb(56Fe, X), 208Pb(58Fe, X), E(cm)=210-230 MeV; calculated compound nucleus formation σ, evaporation residue σ; deduced isotope dependence features. Two-dimensional Smoluchowski equation.
doi: 10.1088/0256-307X/23/6/022
2006LI56 Phys.Rev. C 74, 057602 (2006) Q-value effects on the production of superheavy nuclei NUCLEAR REACTIONS 248Cm(26Mg, 4n), 244Pu(30Si, 4n), 238U(36S, 4n), 226Ra(48Ca, 4n), E* ≈ 30-60 MeV; calculated compound nucleus formation probability, evaporation residue σ. Two-parameter Smoluchowski equation.
doi: 10.1103/PhysRevC.74.057602
2005BA75 Chin.Phys.Lett. 22, 1880 (2005) Oscillation of Hot Fissioning Nuclei around a Saddle Point
doi: 10.1088/0256-307X/22/8/016
2005LI51 Chin.Phys.Lett. 22, 3044 (2005) Effects of Isospin Equilibrium on Cold Fusion of Superheavy Nuclei NUCLEAR REACTIONS 208Pb(58Fe, n), E(cm)=210-230 MeV; calculated excitation function, effects of isospin equilibrium.
doi: 10.1088/0256-307X/22/12/016
2004BA09 Phys.Rev. C 69, 027602 (2004) Determination of fission rate by mean last passage time
doi: 10.1103/PhysRevC.69.027602
2004LI26 Chin.Phys.Lett. 21, 457 (2004) P-Wave Nuclear Halos in 8B and 11Be NUCLEAR STRUCTURE 8B, 11Be; analyzed asymptotic normalization coefficients; deduced valence particle wave functions, halo features.
doi: 10.1088/0256-307X/21/3/011
2004LI52 Chin.Phys.Lett. 21, 1491 (2004) Effects of Target Deformation on the Synthesis of Superheavy Nucleus 283112 NUCLEAR REACTIONS 238U(48Ca, 3n), E(cm)=180-210 MeV; calculated σ, target deformation effects.
doi: 10.1088/0256-307X/21/8/021
2003BA50 Phys.Rev. C 67, 064606 (2003) Investigation on anomalous diffusion for nuclear fusion reactions
doi: 10.1103/PhysRevC.67.064606
2003BO42 Eur.Phys.J. A 18, 627 (2003) Inverse Kramers formula and fusion dynamics of heavy ions
doi: 10.1140/epja/i2003-10088-0
2002AB28 Prog.Theor.Phys.(Kyoto), Suppl. 146, 104 (2002) Y.Abe, D.Boilley, G.Kosenko, J.D.Bao, C.W.Shen, B.Giraud, T.Wada Fusion Dynamics of Massive Heavy-Ion Systems NUCLEAR REACTIONS 244Pu(48Ca, X), E ≈ threshold; calculated fusion probability, related features. Two-step model.
doi: 10.1143/PTPS.146.104
2002BA76 Nucl.Phys. A707, 47 (2002) Quantum Propagator Approach to Heavy-Ion Fusion NUCLEAR REACTIONS 100Mo(100Mo, X), 123Sb(86Kr, X), 124Sn(96Zr, X), E(cm) ≈ 190-270 MeV; calculated fusion probability. Quantum propagator approach, comparison with data.
doi: 10.1016/S0375-9474(02)00751-0
1996BA36 Z.Phys. A354, 293 (1996) Quantum Decay Rate of a Nonlinear Dissipative System with Fission-Like Potential Near T(c)
doi: 10.1007/s002180050048
1995BA47 Z.Phys. A352, 321 (1995) Systematic Studies of Fission Fragment Kinetic Energy Distributrions by Langevin Simulations NUCLEAR STRUCTURE 233Pu, 234Th, 218Pa, 256,254Fm, 239Es; calculated fission fragment kinetic energy, variances; deduced scission condition finite neck radius. Langevin Monte Carlo simulation of fission fluctuation-Dissipation dynamics.
doi: 10.1007/BF01289505
1995BB07 Chin.J.Nucl.Phys. 17, No 3, 260 (1995) Covariant Form of Non-Markovian Langevin Equation in Phase Space
1994BA18 Z.Phys. A347, 217 (1994) Kramers Rate Formula with Coordinate-Dependent Mass NUCLEAR STRUCTURE 248Cf; calculated stationary, time-dependent fission rates vs temperature. 230Th; calculated symmetric fission rate. Kramers rate formula, coordinate-dependent mass.
doi: 10.1007/BF01292379
1994BA34 Phys.Lett. 327B, 1 (1994) Path-Integral Monte Carlo Approach to the Quantum Decay Rate of a Metastable State with Coordinate-Dependent Inertia and Friction
doi: 10.1016/0370-2693(94)91519-9
1990BA05 Z.Phys. A335, 213 (1990) The Realistic Calculation and Analyses of the Multidimensional Fission Width in the Quasi-Stationary Approximation NUCLEAR STRUCTURE 200Tl, 206Bi, 212At, 226Ra, 236U, 240Pu, 244Cm, 254Fm; calculated two-dimensional fission Γ. Quasistationary approximation.
Back to query form Note: The following list of authors and aliases matches the search parameter J.Bao: , J.D.BAO |