NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.Ma Found 18 matches. 2023ME12 Phys.Rev. C 108, 034602 (2023) B.Mei, Y.Guan, N.Zeng, Z.Mai, J.Tu, T.Yu, S.Wang, X.Zhang, P.Ma, X.Xu, X.Tu, Y.Sun, Z.Sun, S.Tang, Y.Yu, F.Fang, D.Yan, S.Jin, Y.Zhao, S.Ma, Y.Zhang Isotopic cross sections in fragmentation reactions of 12, 14C, 14, 16N, and 16O projectiles on a carbon target
doi: 10.1103/PhysRevC.108.034602
2022JI03 Chin.Phys.C 46, 014003 (2022) S.-Y.Jin, Y.-Z.Sun, S.-T.Wang, Z.-Y.Sun, X.-H.Zhang, Z.-Q.Chen, B.Mei, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.B.Ma, X.-M.Liu, R.Han Fragmentation of stable and neutron-rich 12-16C into boron fragments at approximately 240 MeV/nucleon NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X)10Be/13B/B, E=240 MeV/nucleon; measured reaction products; deduced σ. Comparison with EPAX3, modified EPAX2, FRACS, NUCFRG2, INCL++, JQMD, and JQMD-2.0 calculations. The ETF of the Institute of Modern Physics, Chinese Academy of Sciences.
doi: 10.1088/1674-1137/ac2ed5
2022LI28 Few-Body Systems 63, 43 (2022) W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho Progress of Underground Nuclear Astrophysics Experiment JUNA in China NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.
doi: 10.1007/s00601-022-01735-3
2022ME07 Phys.Rev. C 105, 064604 (2022) B.Mei, J.Tu, X.Zhang, S.Wang, Y.Guan, Z.Mai, N.Zeng, X.Tu, Z.Sun, S.Tang, Y.Yu, F.Fang, D.Yan, S.Jin, Y.Zhao, S.Ma, Y.Zhang New experimental evidence for universal odd-even staggering in fragmentation cross sections NUCLEAR REACTIONS 27Al, 16,17,18O(78Kr, X), E=300 MeV/nucleon; measured reaction products, Bρ, time of flight, ΔE; deduced production yields, odd-even staggering (OES) in fragmentation reaction for Z=5-45 with N-Z from 1–9. Systematics of odd-even staggering magnitudes for 78Kr+Al2O3, 78Kr+Be, 84Kr+112,124Sn and 86Kr+Be/Ta. Fragmentation on Al2O3 target at RIBLL2 separator at the Heavy-Ion Research Facility in Lanzhou (HIRFL).
doi: 10.1103/PhysRevC.105.064604
2022XU12 Chin.Phys.C 46, 111001 (2022) Xi.-D.Xu, Y.-Z.Sun, S.-T.Wang, B.Mei, S.-Y.Jin, X.-H.Zhang, Z.-Y.Sun, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.-B.Ma Isotopic production cross sections of fragmentation residues produced by 18O ions on a carbon target near 260 MeV/nucleon NUCLEAR REACTIONS C(18O, X)14N/15C/12C/12B/13B/10B, E=260 MeV/nucleon; measured reaction products, TOF; deduced isotopic σ. Comparison with available data. The HIRFL facility in Lanzhou (China).
doi: 10.1088/1674-1137/ac827c
2021HU23 Phys.Rev.Lett. 127, 172701 (2021) J.Hu, H.Yamaguchi, Y.H.Lam, A.Heger, D.Kahl, A.M.Jacobs, Z.Johnston, S.W.Xu, N.T.Zhang, S.B.Ma, L.H.Ru, E.Q.Liu, T.Liu, S.Hayakawa, L.Yang, H.Shimizu, C.B.Hamill, A.St J.Murphy, J.Su, X.Fang, K.Y.Chae, M.S.Kwag, S.M.Cha, N.N.Duy, N.K.Uyen, D.H.Kim, R.G.Pizzone, M.La Cognata, S.Cherubini, S.Romano, A.Tumino, J.Liang, A.Psaltis, M.Sferrazza, D.Kim, Y.Y.Li, S.Kubono Advancement of Photospheric Radius Expansion and Clocked Type-I X-Ray Burst Models with the New 22Mg(α, p)25Al Reaction Rate Determined at the Gamow Energy NUCLEAR REACTIONS 1H(25Al, p), (25Al, p'), (25Al, X), E=142 MeV; measured reaction products, Ep, Ip, Eγ, Iγ. 26Si; deduced σ(θ), level energies, J, π, resonance parameters, astrophysical reaction rates. Comparison with available data.
doi: 10.1103/physrevlett.127.172701
2019ZH02 Nucl.Instrum.Methods Phys.Res. B438, 48 (2019) L.Zhang, S.Xu, J.He, S.Wang, H.Chen, J.Hu, S.Ma, N.Zhang, S.Hou, W.Liu Properties of fluorine targets and their application on the astrophysically important 19F(p, α)16O reaction NUCLEAR REACTIONS 19F(p, α), E < 270 keV; measured reaction products, Eγ, Iγ; deduced γ-ray yields.
doi: 10.1016/j.nimb.2018.10.024
2018LI18 Chin.Phys.C 42, 044001 (2018) E.-T.Li, Z.H.Li, S.-Q.Yan, J.Su, B.Guo, Y.-J.Li, Y.-B.Wang, G.Lian, S.Zeng, S.-Z.Chen, S.-B.Ma, X.-Q.Li, C.He, H.-B.Sun, W.-P.Liu Measurement of the 2H(7Be, 6Li)3He reaction rate and its contribution to the primordial lithium abundance NUCLEAR REACTIONS 2H(7Be, 6Li)3He, E=17.7, 30.2 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ, reaction rates. Comparison with theoretical calculations.
doi: 10.1088/1674-1137/42/4/044001
2016HE05 Phys.Rev. C 93, 055804 (2016) J.J.He, B.L.Jia, S.W.Xu, S.Z.Chen, S.B.Ma, S.Q.Hou, J.Hu, L.Y.Zhang, X.Q.Yu Direct measurement of 11B(p, γ)12C astrophysical S factors at low energies NUCLEAR REACTIONS 11B(p, γ)12C, E(cm)=130-257 keV; measured Eγ, Iγ, excitation functions, cross section at IMP-Lanzhou; deduced astrophysical S factors. Comparison with previous experimental results and with data in NACREII database.
doi: 10.1103/PhysRevC.93.055804
2016SU10 Phys.Lett. B 756, 323 (2016) J.Su, W.P.Liu, N.T.Zhang, Y.P.Shen, Y.H.Lam, N.A.Smirnova, M.MacCormick, J.S.Wang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, Z.C.Gao, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li, G.Audi Revalidation of the isobaric multiplet mass equation at A = 53, T = 3/2 RADIOACTIVITY 53Ni(EC), (ECp) [from Be(58Ni, X)53Ni, E=68.3 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced T1/2, level scheme, J, π, isobaric analog state, mass excess, explanation of unexpected deviation from the isobaric multiplet mass equation (IMME) at A=53, T=3/2.
doi: 10.1016/j.physletb.2016.03.024
2015SH16 Phys.Rev. C 91, 047304 (2015) Y.P.Shen, W.P.Liu, J.Su, N.T.Zhang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, J.S.Wang, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li Measurement of the 52Fe mass via the precise proton-decay energy of 53Com RADIOACTIVITY 53mCo(p)[from 9Be(58Ni, X), E=68.3 MeV/nucleon]; 41Ti(β+p); measured Ep, Ip, at RIBLL-HIRFL-Lanzhou facility; deduced mass excess of 52Fe and compared with AME-2012 evaluation. 51Fe, 52Co(β+); measured half-lives and compared with evaluated data in ENSDF. ATOMIC MASSES 52Fe; deduced mass excess from Q value of proton decay of 3174.1 keV, 19/2- isomer in 53Co determined from measured proton energy. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.047304
2013SU07 Phys.Rev. C 87, 024312 (2013) J.Su, W.P.Liu, N.C.Shu, S.Q.Yan, Z.H.Li, B.Guo, W.Z.Huang, S.Zeng, E.T.Li, S.J.Jin, X.Liu, Y.B.Wang, G.Lian, Y.J.Li, Y.S.Chen, X.X.Bai, J.S.Wang, Y.Y.Yang, R.F.Chen, S.W.Xu, J.Hu, S.Z.Chen, S.B.Ma, J.L.Han, P.Ma, Q.Hu, J.B.Ma, X.G.Cao, S.L.Jin, Z.Bai, K.Yang, F.D.Shi, W.Zhang, Z.Chen, L.X.Liu, Q.Y.Lin, X.S.Yan, X.H.Zhang, F.Fu, J.J.He, X.Q.Li, C.He, M.S.Smith Reexamining the β decay of 53, 54Ni, 52, 53Co, 51Fe, and 50Mn RADIOACTIVITY 50Mn, 50Cr, 51Fe, 52,53Co, 53,54Ni(β+), (EC), (β+p)[from (58Ni, X), E=68.6 MeV/nucleon]; measured β-delayed protons, (proton)γ-coin, Eγ, Iγ, T1/2 at HIRFL facility in Lanzhou. Implications for r process. Comparison with previous experimental studies.
doi: 10.1103/PhysRevC.87.024312
1994TA13 Nucl.Instrum.Methods Phys.Res. B84, 491 (1994) C.Tan, Y.Xia, X.Liu, J.Liu, S.Ma, J.Li Implanted Dopant and Associated Damage Profiles in Kiloelectronvolt 19F+ Implanted LiNbO3 NUCLEAR REACTIONS 19F(p, αγ), E ≈ resonance; measured γ yield vs E; deduced fluorine depth, associated damage profiles, implantation in LiNbO3.
doi: 10.1016/0168-583X(94)95343-0
1993CA25 Phys.Scr. 47, 751 (1993) X.Cai, Z.Y.Liu, X.M.Chen, S.X.Ma, Z.C.Chen, Q.Xu, H.P.Liu, X.W.Ma M-Subshell Ionization of Th and U by Alpha Particle Bombardment NUCLEAR REACTIONS Th, U(α, X), E=2.5-4.5 MeV; measured M X-ray production σ; deduced M-shell ionization σ, Coster-Kronig yields, M-shell fluorescence yields. ATOMIC PHYSICS Th, U(α, X), E=2.5-4.5 MeV; measured M X-ray production σ; deduced M-shell ionization σ, Coster-Kronig yields, M-shell fluorescence yields.
doi: 10.1088/0031-8949/47/6/011
1992CA35 Nucl.Instrum.Methods Phys.Res. B72, 159 (1992) X.Cai, Z.Y.Liu, X.M.Chen, S.X.Ma, Z.C.Chen, Q.Xu, H.P.Liu, X.W.Ma L-Subshell Ionisation of 71Lu, 73Ta and 79Au by 1.5-4.5 MeV Alpha Particles NUCLEAR REACTIONS Lu, Ta, 197Au(α, X), E=1.5-4.5 MeV; measured L subshell ionization σ vs E. ATOMIC PHYSICS Lu, Ta, 197Au(α, X), E=1.5-4.5 MeV; measured L subshell ionization σ vs E.
doi: 10.1016/0168-583X(92)95230-O
1991MA53 Chin.J.Nucl.Phys. 13, No 4, 347 (1991) Th and U L-Subshell Ionization by Proton Impact NUCLEAR REACTIONS Th, U(p, X), E=0.8-3.4 MeV; measured L-subshell ionization σ. ECPSSR theory. ATOMIC PHYSICS Th, U(p, X), E=0.8-3.4 MeV; measured L-subshell ionization σ. ECPSSR theory.
1989LI18 Nucl.Instrum.Methods Phys.Res. B43, 162 (1989) Z.Liu, X.Cai, S.Ma, J.Liu, J.Feng, S.Liu, Z.Zheng L-Subshell Ionization of Dy and Ho by 0.4-3.0 MeV Protons NUCLEAR REACTIONS Dy, 165Ho(p, X), E=0.4-3 MeV; measured L X-ray production σ; deduced subshell ionization σ. ATOMIC PHYSICS Dy, 165Ho(p, X), , E=0.4-3 MeV; measured L X-ray production σ; deduced subshell ionization σ.
doi: 10.1016/0168-583X(89)90031-1
1988LI16 Chin.J.Nucl.Phys. 10, 149 (1988) Liu Zhaoyuan, Ma Shuxun, Liu Shaoxiang, Zhang Zhijin, Liu Jihu, Cai Xiaohong, Feng Jiazhen K-Shell X-Ray Production Cross Sections of Al, Ti and Ni by Proton Bombardment NUCLEAR REACTIONS 27Al, Ti, Ni(p, X), E=0.25-0.43 keV; 27Al(p, X), E=0.4-3 MeV; measured K-shell X-ray production σ.
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