NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = Liu Manqing Found 78 matches. 2023CH23 Phys.Rev. C 107, 054306 (2023) J.Chen, M.Liu, C.Yuan, S.Chen, N.Shimizu, X.Sun, R.Xu, Y.Tian Shell-model-based investigation on level density of Xe and Ba isotopes NUCLEAR STRUCTURE 131,132,133,134Sn, 132,133,134,135Sb, 133,134,135,136Te, 134,135,136,137I, 135,136,137,138Xe, 136,137,138,139Cs, 137,138,139,140Ba; calculated one-neutron separation energy S(n). 132,133,134Sn, 132,133,134,135Sb, 134,135,136Te, 135,136,137I, 136,137,138Xe, 137,138,139Cs, 138,139,140Ba; calculated two-neutron separation energies S(2n). 134, ,136,138Xe, 134,136,138,140Ba, 128,129,130,134,135,136Sn, 131,135Sb, 132,134,136Te, 133,135,137I, 135,137,139Cs, 139La; calculated levels, J, π. 133,134,135,136,137Xe, 134,135,136,137,138,139Ba; calculated nuclear level densities (NLD), cumulative number of levels spin distributions. 134Te, 135I, 136Xe, 137Cs, 138Ba, 139La; calculated effective single particle energy for proton and neutron orbits with and without the consideration of tensor part in two-body matrix elements. 133,134,135,136,137Xe; calculated spin distribution , parity ratios, spin cut-off parameter. Configuration-interaction shell model with a unified effective nuclear force. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.054306
2023CH42 At.Data Nucl.Data Tables 154, 101587 (2023) Y.Chen, H.Yao, M.Liu, J.Tian, P.Wen, N.Wang Systematic study of fusion barriers with energy dependent barrier radius NUCLEAR STRUCTURE Z<92; analyzed available data; deduced fusion barriers, a modified Siwek-Wilczynski (MSW) fusion σ formula.
doi: 10.1016/j.adt.2023.101587
2023LI06 Phys.Rev. C 107, 014320 (2023) Z.Li, J.Zhu, T.Wang, M.Liu, J.Wang, Y.Yang, C.Lin, J.Ma, P.Ma, Z.Bai, Y.Yu, X.Zhang, X.Liu, F.Duan, C.G.Lu, H.Yang, X.Wei, J.Zhang, S.Jin, Z.Gao, Y.Hu, Y.Yao, J.Wang, S.Guo, W.Jiang, B.Yang, J.He Cluster structure of 11C investigated with a breakup reaction NUCLEAR REACTIONS 12C(11C, α)7Be, E=25 MeV/nucleon; measured reaction products, Eα, Iα, Eγ, Iγ, αγ-coin, (particle)α-coin; deduced invariant-mass spectra, exclusive σ, excitation functions. 11C; deduced resonances, J, π, rotational bands, rotational parameter. Provided evidence for 2α+3He structure. DSSD-CsI(Tl) telescopes and scintillator detectors (LaBr:Ce3 and NaI(Tl)) at heavy ion research facility in Lanzhou (HIRFL-RIBLL1).
doi: 10.1103/PhysRevC.107.014320
2023LI63 Int.J.Mod.Phys. E32, 2330003 (2023) Recent progress in configuration–interaction shell model NUCLEAR STRUCTURE 56Ni, 78Ni, 110Ni, 110Sn, 132Sn, 176Sn, 164Pb, 208Pb; analyzed available data; deduced the model spaces, parameters. The configuration–interaction shell model (CISM), performed in truncated model space with the inclusion of the residual interaction, is one widely-used nuclear structure model.
doi: 10.1142/S0218301323300035
2022MA31 Astrophys.J.Suppl.Ser. 260, 56 (2022) H.Ma, M.Liu, Y.Geng, T.Wang, Z.Yu, H.Zheng, S.Gamrath, P.Quinet, Z.Dai Experimental and Theoretical Radiative Parameters of Highly Excited Odd-parity Levels in Ir II ATOMIC PHYSICS Ir; measured frequencies; deduced the radiative lifetimes for 15 odd-parity levels. The time-resolved laser-induced fluorescence technique. The pseudorelativistic Hartree-Fock including core-polarization corrections method.
doi: 10.3847/1538-4365/ac721a
2022YU06 Phys.Rev. C 106, 044314 (2022) C.Yuan, M.Liu, N.Shimizu, Z.Podolyak, T.Suzuki, T.Otsuka, Z.Liu Shell-model study on spectroscopic properties in the region "south" of 208Pb NUCLEAR STRUCTURE 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Tl, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217Pb, 198,199,200,201,202,203,204,205,206,207,208,209,210,211Hg, 198,199,200,201,202,203,204,205,206,207,208,209Au, 198,199,200,201,202,203,204,205,206,207Pt, 198,199,200,201,202,203,204Ir, 198,199,200,201,202,203Os, 198,199,200,201,202Re, 197,198,199,200,201W; calculated levels J, π, configurations, T1/2, effective single-particle energies, B(E2), binding energies, S(n), proton and neutron E2 transition matrix elements, electric quadrupole moments, magnetic dipole moments. Large-scale shell-model calculations with combined KHHE (with adjustment of its proton-proton part) and KHPE Hamiltonians and the monopole-based universal interaction. Comparison to experimental results and AME2020 data.
doi: 10.1103/PhysRevC.106.044314
2021CR01 Phys.Lett. B 816, 136210 (2021) F.C.L.Crespi, A.Bracco, E.G.Lanza, A.Tamii, N.Blasi, F.Camera, O.Wieland, N.Aoi, D.L.Balabanski, S.Bassauer, A.S.Brown, M.P.Carpenter, J.J.Carroll, M.Ciemala, A.Czeszumska, P.J.Davies, V.Derya, L.M.Donaldson, Y.D.Fang, H.Fujita, G.Gey, H.T.Ha, M.N.Harakeh, T.Hashimoto, N.Ichige, E.Ideguchi, A.Inoue, J.Isaak, C.Iwamoto, D.G.Jenkins, T.Klaus, N.Kobayashi, T.Koike, M.Krzysiek, M.K.Raju, M.Liu, A.Maj, L.Morris, P.von Neumann-Cosel, S.Noji, H.J.Ong, S.G.Pickstone, N.Pietralla, D.Savran, J.M.Schmitt, M.Spieker, G.Steinhilber, C.Sullivan, B.Wasilewska, M.Weinert, V.Werner, Y.Yamamoto, T.Yamamoto, R.G.T.Zegers, X.Zhou, S.Zhu, A.Zilges The structure of low-lying 1- states in 90, 94Zr from (α, α'γ) and (p, p'γ) reactions NUCLEAR REACTIONS 90,94Zr(p, p'γ), E=80 MeV; 90,94Zr(α, α'γ), E=130 MeV; measured reaction products, Eγ, Iγ; deduced ratio of the measured yields, dipole states σ, transition densities, low-lying dipole strength. The array CAGRA with HPGe detectors.
doi: 10.1016/j.physletb.2021.136210
2021JI16 Symmetry 13, 2278 (2021) H.Jian, Y.Gao, F.Dai, J.Liu, X.Xu, C.Yuan, K.Kaneko, Y.Sun, P.Liang, G.Shi, L.Sun, L.Xayavong, C.Lin, J.Lee, Z.Li, Y.Yang, P.Li, R.Fan, S.Zha, H.Zhu, J.Li, Q.Gao, Z.Zhang, R.Chen, J.Wang, D.Wang, H.Wu, K.Wang, Y.Lam, F.Duan, P.Ma, Z.Gao, Q.Hu, Z.Bai, J.Ma, J.Wang, F.Zhong, C.Wu, D.Luo, Y.Jiang, Y.Liu, D.Hou, R.Li, N.Ma, W.Ma, G.Yu, D.Patel, S.Jin, Y.Wang, Y.Yu, Q.Zhou, P.Wang, L.Hu, X.Wang, H.L.Zang, Q.Zhao, L.Yang, P.Wen, F.Yang, H.Jia, G.Zhang, M.Pan, X.Wang, H.Sun, M.Wang, Z.Hu, X.Zhou, Y.Zhang, H.Xu, M.Liu, H.-J.Ong, W.Yang β-Delayed γ Emissions of 26P and Its Mirror Asymmetry RADIOACTIVITY 26P(β+), (EC) [from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation using RIBBL1 at HRIBF, Lanzhou facility]; measured Eγ, Iγ, βγ-coin, T1/2 of 26P decay. 26Si; deduced levels, J, π, β++ϵ feedings, logft, mirror asymmetry parameter from comparison with the ϵ decay of mirror nucleus 26Na to 26Mg, mirror-energy differences (MEDs), and halo structure in 26P. Comparison with shell-model calculations. NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P/27S, E=80.6 MeV/nucleon; measured reaction products, particle-identification (PID) plot of ΔE vs TOF for the ions separated using RIBBL1 separator at HRIBF, Lanzhou facility.
doi: 10.3390/sym13122278
2021ZA06 Phys.Rev. C 104, 014607 (2021) J.C.Zamora, C.Sullivan, R.G.T.Zegers, N.Aoi, L.Batail, D.Bazin, M.Carpenter, J.J.Carroll, Y.D.Fang, H.Fujita, U.Garg, G.Gey, C.J.Guess, M.N.Harakeh, T.H.Hoang, E.Hudson, N.Ichige, E.Ideguchi, A.Inoue, J.Isaak, C.Iwamoto, C.Kacir, N.Kobayashi, T.Koike, M.Kumar Raju, S.Lipschutz, M.Liu, P.von Neumann-Cosel, S.Noji, H.J.Ong, S.Peru, J.Pereira, J.Schmitt, A.Tamii, R.Titus, V.Werner, Y.Yamamoto, X.Zhou, S.Zhu Investigation of the isoscalar response of 24Mg to 6Li scattering NUCLEAR REACTIONS 24Mg(6Li, 6Li'), E=100 MeV/nucleon; measured scattered 6Li particles, σ(θ) using Grand Raiden spectrometer and two position-sensitive multiwire drift chambers (MWDCs) and three plastic scintillators for particle identification and reconstructing their trajectories at RCNP-Osaka University; deduced differential σ(E, Q), angular momentum transfers by fitting with multipole-decomposition analysis (MDA) using DWBA calculations for angular-momentum transfers. 24Mg; deduced energies, widths, EWSR, isoscaler giant monopole resonance (ISGMR), isoscaler giant monopole resonance (ISGDR), isoscaler giant quadrupole resonance (ISGQR) strength functions from Lorentzian fits to data. Comparison with antisymmetrized molecular dynamics (AMD) calculations, and with previous experimental data.
doi: 10.1103/PhysRevC.104.014607
2020ZA05 Phys.Rev. C 101, 064609 (2020) J.C.Zamora, C.Sullivan, R.G.T.Zegers, N.Aoi, L.Batail, D.Bazin, M.Carpenter, J.J.Carroll, I.Deloncle, Y.D.Fang, H.Fujita, U.Garg, G.Gey, C.J.Guess, M.N.Harakeh, T.H.Hoang, E.Hudson, N.Ichige, E.Ideguchi, A.Inoue, J.Isaak, C.Iwamoto, C.Kacir, N.Kobayashi, T.Koike, M.Kumar Raju, S.Lipschutz, M.Liu, P.von Neumann-Cosel, S.Noji, H.J.Ong, S.Peru, J.Pereira, J.Schmitt, A.Tamii, R.Titus, V.Werner, Y.Yamamoto, X.Zhou, S.Zhu Reexamination of isoscalar giant resonances in 12C and 93Nb through 6Li scattering NUCLEAR REACTIONS 12C, 93Nb(6Li, 6Li'), E=100 MeV/nucleon; measured 6Li spectra, double-differential σ, and angular distributions for the isoscalar giant monopole resonances (ISGMRs) using the high-resolution Grand Raiden magnetic spectrometer at the RCNP-Osaka facility; deduced contribution of different angular momentum transfers to differential σ, energies, widths and E0 strength distribution of GMRs, EWSR, influence on GMRs due to nuclear structure. Angular distribution data fitted using multipole-decomposition analysis (MDA) and DWBA methods. Comparison with antisymmetrized molecular dynamics (AMD) calculations, and with previous experimental data.
doi: 10.1103/PhysRevC.101.064609
2020ZH08 Phys.Rev. C 101, 034303 (2020) Y.Zhang, M.Liu, C.-J.Xia, Z.Li, S.K.Biswal Constraints on the symmetry energy and its associated parameters from nuclei to neutron stars NUCLEAR REACTIONS 112,124Sn(124Sn, X), (112Sn, X), E=35, 50 MeV/nucleon; analyzed symmetry energy and related set of 22 nuclear matter parameters by comparing the isospin diffusion data to transport model calculations in five-dimensional parameter space. 208Pb; calculated neutron skin of 208Pb using the deduced nuclear matter parameter set and the restricted density variational (RDV) method. Calculated properties of a neutron star, such as the tidal deformability and maximum mass, and compared with the current constraints.
doi: 10.1103/PhysRevC.101.034303
2019LI12 Nucl.Instrum.Methods Phys.Res. B445, 13 (2019) Experimental thick target bremsstrahlung spectra produced by 5-25 keV electrons for 6 ≤ Z ≤ 82 and comparison with Monte Carlo PENELOPE simulations NUCLEAR REACTIONS C, Ti, Zr, Nb, W, Pb(E, γ), E=5-25 keV; measured reaction products, X-rays; deduced thick target yields, bremsstrahlung spectra. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2019.02.025
2018HA06 Nucl.Instrum.Methods Phys.Res. B418, 68 (2018) J.Han, Z.An, G.Zheng, F.Bai, Z.Li, P.Wang, X.Liao, M.Liu, S.Chen, M.Song, J.Zhang An ion beam facility based on a 3 MV tandetron accelerator in Sichuan University, China NUCLEAR REACTIONS 55Mn(p, X), E=2 MeV; measured reaction products, Eγ, Iγ, X-rays; deduced X-ray production yields for PIXE. High-precision ion implantation.
doi: 10.1016/j.nimb.2018.01.002
2018LI51 Chin.Phys.C 42, 114101 (2018) Statistical errors in Weizsacker-Skyrme mass model NUCLEAR STRUCTURE 132Sn, 208Pb, Ca, Zr, Sb, Rn; calculated atomic masses; deduced statistical uncertainties of 13 model parameters. Comparison with AME2016.
doi: 10.1088/1674-1137/41/11/114101
2018SU14 Phys.Rev. C 98, 015804 (2018) C.Sullivan, R.G.T.Zegers, S.Noji, SamM.Austin, J.Schmitt, N.Aoi, D.Bazin, M.Carpenter, J.J.Carroll, H.Fujita, U.Garg, G.Gey, C.J.Guess, T.H.Hoang, M.N.Harakeh, E.Hudson, N.Ichige, E.Ideguchi, A.Inoue, J.Isaak, C.Iwamoto, C.Kacir, T.Koike, N.Kobayashi, S.Lipschutz, M.Liu, P.von Neumann-Cosel, H.J.Ong, J.Pereira, M.Kumar Raju, A.Tamii, R.Titus, V.Werner, Y.Yamamoto, Y.D.Fang, J.C.Zamora, S.Zhu, X.Zhou The (6Li, 6Li* [3.56 MeV]) reaction at 100 MeV/u as a probe of Gamow-Teller transition strengths in the inelastic scattering channel NUCLEAR REACTIONS 12C(6Li, 6Li'), E=100 MeV/nucleon; measured Eγ, Iγ, 6Li scattered particles, (6Li)γ-coin, double differential σ(θ, Eex) using CAGRA detector array for γ detection, and Grand Raiden magnetic spectrometer for analysis of charged particles at RCNP-Osaka; deduced Doppler-corrected (6Li)γ-coin spectrum, Gamow-Teller strengths, and isovector spin-transfer response in inelastic reaction channel by tagging the reaction with the 3.56-MeV γ-ray from the excited state of 6Li. 24Mg, 93Nb(6Li, 6Li'), E=100 MeV/nucleon; reactions used for calibration, also it was not possible to isolate the isovector spin transfer excitations in the inelastic channel.
doi: 10.1103/PhysRevC.98.015804
2017AS03 Eur.Phys.J. A 53, 71 (2017) E.-C.Aschenauer, I.Balitsky, L.Bland, S.J. Brodsky, M.Burkardt, V.Burkert, J.-P.Chen, A.Deshpande, M.Diehl, L.Gamberg, M.Grosse Perdekamp, J.Huang, C.Hyde, X.Ji, X.Jiang, Z.-B.Kang, V.Kubarovsky, J.Lajoie, K.-F.Liu, M.Liu, S.Liuti, W.Melnitchouk, P.Mulders, A.Prokudin, A.Tarasov, J.-W.Qiu, A.Radyushkin, D.Richards, E.Sichtermann, M.Stratmann, W.Vogelsang, F.Yuan Pre-Town Meeting on spin physics at an Electron-Ion Collider
doi: 10.1140/epja/i2017-12251-4
2017LI42 Chin.Phys.C 41, 114101 (2017) Statistical errors in Weizsacker-Skyrme mass model NUCLEAR STRUCTURE 132Sn, 208Pb, Ca, Zr, Sb, Rn; calculated masses. Comparison with AME2003 and AME2016 evaluations.
doi: 10.1088/1674-1137/41/11/114101
2016WA02 Phys.Rev. C 93, 014302 (2016) Correlations between neutrons and protons near the Fermi surface and Qαof superheavy nuclei NUCLEAR STRUCTURE Z=14, N=10-40; Z=28, N=20-70; calculated S(n), S(2n) and compared to experimental values. 46Si, 60Ca, 78Ni, 132Sn, 208Pb, 252Fm, 270Hs, 296Og, 298120, 308124; N=30-130 along the shell stability line; calculated scaled shell gaps, shell correction energies and quadrupole deformation β2. 284,285,286,287,288,289Fl, 288,289,290,291,292,293Lv, 292,293,294,295,296,297Og, 296,297,298,299,300,301120, 300,301,302,303,304,305122, 304,305,306,307,308,309124, 308,309,310,311,312,313126; calculated shell correction energies, deformation energies, Q(α). Weizsacker-Skyrme (WS4)mass model. Comparison with other theoretical calculations, and with available experimental values.
doi: 10.1103/PhysRevC.93.014302
2015OU02 Phys.Rev.Lett. 115, 212501 (2015) L.Ou, Z.Xiao, H.Yi, N.Wang, M.liu, J.Tian Dynamic Isovector Reorientation of Deuteron as a Probe to Nuclear Symmetry Energy NUCLEAR REACTIONS 124Sn(polarized d, X), E=100 MeV/nucleon; calculated breakup reaction σ(θ). Comparison with available data.
doi: 10.1103/PhysRevLett.115.212501
2015WA14 Phys.Rev. C 91, 044308 (2015) N.Wang, M.Liu, H.Jiang, J.L.Tian, Y.M.Zhao Mass dependence of symmetry energy coefficients in the Skyrme force ATOMIC MASSES A=160; A=20-300; A=20-106; analyzed properties of nuclear symmetry energy as function of mass using the extended Thomas-Fermi (ETF2) approximation and 36 different Skyrme forces. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.91.044308
2015WE01 Nucl.Phys. A933, 114 (2015) D.Wei, L.Mao, N.Wang, M.Liu, L.Ou Further study on mechanism of production of light complex particles in nucleon-induced reactions NUCLEAR REACTIONS 27Al(p, d), (p, t), (p, 3He), (p, α), E=62 MeV;56Fe(n, d), (n, 3H), (n, 3He), (n, α), E=62, 175 MeV;58Ni(p, d), (p, t), (p, 3He), (p, α), E=1200 MeV;58Ni(p, p'), (p, n), (p, d), (p, t), (p, 3He), (p, α), E=175 MeV;63Cu(n, d), (n, 3H), E=317, 383, 477, 542 MeV;197Au(p, d), (p, t), (p, 3He), (p, α), E=1200 MeV; calculated σ(θ, Eout) using transport model and statistical model. Compared with available data.
doi: 10.1016/j.nuclphysa.2014.10.020
2014MO23 Phys.Rev. C 90, 024320 (2014) Systematic study of shell gaps in nuclei NUCLEAR STRUCTURE Z>8, N>8; analyzed S(2n), optimal values of the 18 independent model parameters, shell gaps using eight global nuclear mass models (FRDM, HFB17, HFB27, DZ28, WS, WS*, WS3, WS4), Weizsacker-Skyrme (WS4) mass formula based on measured and evaluated nuclear masses of 2353 nuclei in AME-2012. Magicity of N=184 from S(2n) and shell gaps, and shell closures in 208Pb and 270Hs. Magic numbers at Z=82 and 114. and subshell closures at Z=64, 92, 100, 120. No subshell closure at N=132 in Ra isotopes.
doi: 10.1103/PhysRevC.90.024320
2014OU01 Phys.Rev. C 89, 011001 (2014) Sensitive dependence of isotope and isobar distributions of limiting temperatures on the symmetry energy NUCLEAR STRUCTURE A=25-250; Z=50, A=100-170; Z=38, A=75-120; Z=26-46, A=93; calculated density dependence of symmetry energy, mass and isotope distributions of limiting temperatures for β-stable nuclei, correlation between distribution width and symmetry energy. Thermodynamical approach with the Skyrme energy density functional using different Skyrme interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.011001
2013WA09 Phys.Rev. C 87, 034327 (2013) Nuclear symmetry energy from the Fermi-energy difference in nuclei NUCLEAR STRUCTURE 16,22O, 22,42Si, 40,48,60Ca, 42Ti, 56,68,78Ni, 130Cd, 100,132,134Sn, 134Te, 144Sm, 182,208Pb; calculated neutron-proton Fermi-energy difference, nuclear symmetry energy, neutron-skin thickness. Skyrme energy density functionals and nuclear masses, with 54 Skyrme parameter sets. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.034327
2012JI07 Phys.Rev. C 85, 054303 (2012) H.Jiang, G.J.Fu, B.Sun, M.Liu, N.Wang, M.Wang, Y.G.Ma, C.J.Lin, Y.M.Zhao, Y.H.Zhang, Z.Ren, A.Arima Predictions of unknown masses and their applications ATOMIC MASSES Z=1-184, N=1-184; analyzed masses for 1566 nuclei using extrapolation approach and shell correction term, S(n), S(2n), S(p), and S(2p); one-neutron and one-proton drip nuclei, R-process nucleosynthesis and astrophysical implications. Comparison with AME-2011 interim mass evaluation, and with Duflo-Zuker model. 85Mo, 87,88,89Tc, 123Ag, 140I, 222Po, 226,227,228Rn, 233,234Ra, 235Ac; compared predicted masses with measured values. RADIOACTIVITY 248,249,250,251,252,253,254,255,256,257No, 251,252,253,254,255,256,257,258,259Lr, 253,254,255,256,257,258,259,260,261Rf, 255,256,257,258,259,260,261,262Db, 256,257,258,259,260,261,262,263Sg(α); calculated Q(α), half-life. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054303
2012KE02 Nucl.Instrum.Methods Phys.Res. B280, 1 (2012) Deuteron induced secondary electron emission from titanium deuteride surface NUCLEAR REACTIONS Ti, 2H(d, e), E=80-254 keV; measured reaction products, Ee, Ie; deduced electron yields. SRIM calculation, comparison with available data.
doi: 10.1016/j.nimb.2012.02.033
2011LI31 Phys.Rev. C 84, 014333 (2011) Further improvements on a global nuclear mass model ATOMIC MASSES A=1-240; analyzed deviations of calculated nuclear masses total g.s. energies, and S(n) from the experimental data, b coefficients of nuclei in the IMME as a function of mass number. A=260-320; calculated Q(α). Global nuclear mass models. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.014333
2011LI33 Chin.Phys.C 35, 629 (2011) M.Liu, Z.-X.Li, N.Wang, F.-S.Zhang Exploring nuclear symmetry energy with isospin dependence in neutron skin thickness of nuclei
doi: 10.1088/1674-1137/35/7/006
2011WA38 Phys.Rev. C 84, 051303 (2011) Nuclear mass predictions with a radial basis function approach ATOMIC MASSES A=16-264; analyzed masses, rms deviation from recommended values for 2149 nuclei, S(n) values. Radial basis function (RBF) and the Garvey-Kelson relation with global nuclear mass models. The AME95-03 and AME03-Border tests.
doi: 10.1103/PhysRevC.84.051303
2010LI45 Phys.Rev. C 82, 064306 (2010) M.Liu, N.Wang, Z.-X.Li, F.-S.Zhang Nuclear symmetry energy at subnormal densities from measured nuclear masses NUCLEAR STRUCTURE A=20-250; analyzed nuclear symmetry energy coefficients for more that 2000 previously measured masses using liquid drop formula with the contribution of the Wigner term. Comparison with other methods.
doi: 10.1103/PhysRevC.82.064306
2010WA09 Phys.Rev. C 81, 044322 (2010), Publishers Note Phys.Rev. C 81, 059902 (2010) Modification of nuclear mass formula by considering isospin effects NUCLEAR STRUCTURE 16O, 48Ca, 208Pb; calculated energies, β2 and β4 deformation parameters. 82Sr; calculated potential energy surface as function of β2 and β4 deformation parameters. 16,24O, 40,48Ca, 90Zr, 132Sn, 208Pb, 270Hs, 288,290,292,294116, N=2-240; calculated shell corrections. Skyrme energy-density functional approach. Comparison with experimental data. ATOMIC MASSES Z=10-130, N=10-230; calculated nuclear masses for 2149 nuclei using Skyrme energy-density functional approach and comparison with FRDM and HFB-17 results. Comparison with experimental data. Semiempirical nuclear mass formula based on the macroscopic-microscopic method with Woods-Saxon density distribution.
doi: 10.1103/PhysRevC.81.044322
2010WA24 Phys.Rev. C 81, 067302 (2010) Mass and isospin dependence of symmetry energy coefficients of finite nuclei NUCLEAR STRUCTURE A=1-250; analyzed symmetry-energy coefficients as a function of nuclear mass number and isospin asymmetry., Wigner energies using the liquid drop mass formula and measured nuclear masses.
doi: 10.1103/PhysRevC.81.067302
2010WA28 Nucl.Phys. A834, 212c (2010) Extraction of probability of compound-nucleus formation NUCLEAR STRUCTURE Z=102-118; compiled, analyzed capture σ, probability of compound nucleus formation. Comparison with other data.
doi: 10.1016/j.nuclphysa.2009.12.043
2010WA38 Phys.Rev. C 82, 044304 (2010) Mirror nuclei constraint in nuclear mass formula ATOMIC MASSES Z>8, N>8; analyzed model parameters of the semiempirical mass formula using measured masses of 2149 nuclei with mirror nuclei constraints, shell corrections, contour plots of β2, β4 and β6 deformation parameters as a function of neutron number, neutron drip lines, fission barriers of SHE, Q(α) values. Prediction of central region of SHE near N=176-178 and Z=116-120.
doi: 10.1103/PhysRevC.82.044304
2009NI17 Eur.Phys.J. A 42, 471 (2009) M.Niikura, E.Ideguchi, N.Aoi, H.Baba, T.Fukuchi, Y.Ichikawa, H.Iwasaki, T.Kubo, M.Kurokawa, M.Liu, S.Michimasa, T.Ohnishi, T.K.Onishi, S.Ota, S.Shimoura, H.Suzuki, D.Suzuki, Y.Wakabayashi, K.Yoshida, Y.Zheng Yrast spectroscopy in 49-51Ti via fusion-evaporation reaction induced by a radioactive beam NUCLEAR REACTIONS 9Be(46Ar, xn)49Ti/50Ti/51Ti, E=2-8 MeV/nucleon; measured Eγ, Iγ, γγ-coin in-beam using GRAPE HPGe detector array with Doppler shift correction. 49Ti, 50Ti, 51Ti; deduced high-spin yrast levels, J, π, configurations. Comparison with shell model ANTOINE. Secondary radioactive beam.
doi: 10.1140/epja/i2009-10857-7
2009YU10 Chin.Phys.C 33, Supplement 1, 188 (2009) D.-Q.Yuan, Y.-N.Zheng, Y.Zuo, P.Fan, D.-M.Zhou, M.Liu, X.-G.Wu, L.-H.Zhu, G.-S.Li, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu Study of magnetic-rotation in 82Rb by g-factor measurements NUCLEAR REACTIONS 60Ni(27Al, n4p)82Rb, E=130 MeV; measured Eγ, Iγ, γ-γ-coin.; deduced magnetic rotational bands, g factors.
doi: 10.1088/1674-1137/33/S1/060
2008SH12 Phys.Rev. C 77, 047303 (2008) T.Shizuma, T.Ishii, H.Makii, T.Hayakawa, M.Matsuda, S.Shigematsu, E.Ideguchi, Y.Zheng, M.Liu, T.Morikawa, M.Oi One-quasiparticle bands in neutron-rich 187W NUCLEAR REACTIONS 186W(18O, 17O), E=180 MeV; measured Eγ, Iγ, γγ-coin. 187W; deduced levels, J, π, band structures and configurations. 16,17,18,19O; measured ion energy losses.
doi: 10.1103/PhysRevC.77.047303
2007SH42 Eur.Phys.J. A 34, 1 (2007) T.Shizuma, T.Ishii, H.Makii, T.Hayakawa, S.Shigematsu, M.Matsuda, E.Ideguchi, Y.Zheng, M.Liu, T.Morikawa Evidence for a Kπ = 1/2+ isomer in neutron-rich 185Ta NUCLEAR REACTIONS 186W(18O, 19F), E=180 MeV; measured Eγ, Iγ, (particle)γ-coin, γγ-coin. 185Ta deduced levels, J, π.
doi: 10.1140/epja/i2007-10484-4
2007YU03 Hyperfine Interactions 180, 49 (2007) D.Yuan, Y.Zheng, D.Zhou, Y.Zuo, P.Fan, M.Liu, X.Wu, L.Zhu, G.Li, G.Xu, Q.Fan, X.Zhang, S.Zhu g-Factors of magnetic-rotational states in 85Zr NUCLEAR REACTIONS 60Ni(28Si, n2p), E=98 MeV; measured Eγ, Iγ(θ), g-factors for high spin states.
doi: 10.1007/s10751-008-9684-y
2006LI09 Nucl.Phys. A768, 80 (2006) M.Liu, N.Wang, Z.Li, X.Wu, E.Zhao Applications of Skyrme energy-density functional to fusion reactions spanning the fusion barriers NUCLEAR REACTIONS 92Zr(12C, X), E(cm) ≈ 24-48 MeV; 70,72,73,74,76Ge, 92Zr, 112Cd, 144Nd, 144,147,148,149,150,154Sm, 166Er, 186W, 208Pb, 232Th(16O, X), E(cm) ≈ 30-160; 144Sm(17O, X), E(cm) ≈ 50-100 MeV; 197Au, 208Pb(19F, X), E(cm) ≈ 70-150 MeV; 70,72,73,74,76Ge(27Al, X), E(cm) ≈ 45-65 MeV; 28Si, 92Zr, 178Hf(28Si, X), E(cm) ≈ 20-150 MeV; 186W(30Si, X), E(cm) ≈ 105-165 MeV; 175Lu(31P, X), E(cm) ≈ 100-150 MeV; 154Sm, 181Ta, 182W(32S, X), E(cm) ≈ 120-200 MeV; 90,92Zr(33S, X), E(cm) ≈ 70-100 MeV; 54Fe, 92Zr(35Cl, X), E(cm) ≈ 50-100 MeV; 90Zr(50Ti, X), E(cm) ≈ 90-130 MeV; 64Ni(132Sn, X), E(cm) ≈ 140-180 MeV; analyzed fusion excitation functions, fusion barrier features. Extended semi-classical Thomas-Fermi method, suppression and enhancement effects discussed.
doi: 10.1016/j.nuclphysa.2006.01.011
2006LI13 Chin.Phys.Lett. 23, 804 (2006) M.Liu, N.Wang, Z.-X.Li, X.-Z.Wu Neutron Skin Thickness of Nuclei and Effective Nucleon-Nucleon Interactions NUCLEAR STRUCTURE 18O, 48Ca, 114,116,118,120,122,124,132Sn, 208Pb; calculated radii, neutron skin thickness. 38,40,48,56Ca, 82,90,96,116Zr, 92,100,112,130Sn, 180,208,220,240Pb; calculated neutron and proton density distributions. Skyrme energy density functional, comparisons with data.
doi: 10.1088/0256-307X/23/4/012
2006SH23 Eur.Phys.J. A 30, 391 (2006) T.Shizuma, T.Ishii, H.Makii, T.Hayakawa, S.Shigematsu, M.Matsuda, E.Ideguchi, Y.Zheng, M.Liu, T.Morikawa, P.M.Walker, M.Oi Excited states in neutron-rich 188W produced by an 18O-induced 2-neutron transfer reaction NUCLEAR REACTIONS 186W(18O, 16O), E=180 MeV; measured Eγ, Iγ, (particle)γ-coin. 188W deduced levels, J, π, configurations. Level systematics in neighboring isotopes discussed.
doi: 10.1140/epja/i2006-10139-0
2006WA26 Phys.Rev. C 74, 044604 (2006) N.Wang, X.Wu, Z.Li, M.Liu, W.Scheid Applications of Skyrme energy-density functional to fusion reactions for synthesis of superheavy nuclei NUCLEAR REACTIONS 92Zr, 144Sm(16O, X), E(cm) ≈ 40-90 MeV; 92Zr(64Ni, X), E(cm)=120-180 MeV; calculated fusion σ. 26Mg, 27Al, 32S, 35Cl(238U, X), 208Pb, 244Pu, 248Cm(48Ca, X), 254Cf(32S, X), 254Es(35Cl, X), (36S, X), (48Ca, X), E(cm) ≈ 100-240 MeV; calculated capture σ. 248Cm, 247,249Bk, 250,252,254Cf, 252,254Es(36S, X), (37Cl, X), (48Ca, X), (50Ti, X), E not given; calculated entrance channel capture barriers.
doi: 10.1103/PhysRevC.74.044604
2004BL02 Nucl.Instrum.Methods Phys.Res. A517, 139 (2004) I.Blevis, J.Boger, E.Bonvin, B.T.Cleveland, X.Dai, F.Dalnoki-Veress, G.Doucas, J.Farine, H.Fergani, D.Grant, R.L.Hahn, A.S.Hamer, C.K.Hargrove, H.Heron, P.Jagam, N.A.Jelley, C.Jillings, A.B.Knox, H.W.Lee, I.Levine, M.Liu, S.Majerus, A.McDonald, K.McFarlane, C.Mifflin, A.J.Noble, S.Noel, V.M.Novikov, J.K.Rowley, M.Shatkay, J.J.Simpson, D.Sinclair, B.Sur, J.-X.Wang, M.Yeh, X.Zhu Measurement of 222Rn dissolved in water at the Sudbury Neutrino Observatory RADIOACTIVITY 222Rn(α); measured Eα, Iα, contribution to detector background.
doi: 10.1016/j.nima.2003.10.103
2004LI21 Phys.Rev. C 69, 034615 (2004) Mass and isotope dependence of limiting temperatures for hot nuclei NUCLEAR STRUCTURE A=20-250; calculated limiting temperatures. C, O, Ca, Zr; calculated limiting temperature vs mass.
doi: 10.1103/PhysRevC.69.034615
2004WA08 Phys.Rev. C 69, 034608 (2004) N.Wang, Z.Li, Z.Wu, J.Tian, Y.X.Zhang, M.Liu Further development of the improved quantum molecular dynamics model and its application to fusion reactions near the barrier NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 114,132Sn, 140Ce, 208Pb; calculated binding energies, radii. NUCLEAR REACTIONS 48Ca, 90Zr(40Ca, X), 16O, 208Pb(16O, X), 131I(131I, X), 208Pb(54Cr, X), 230Th(32S, X), 250Fm(12C, X), E not given; calculated static Coulomb barriers. 48Ca(40Ca, X), E(cm)=52, 54, 58, 60 MeV; calculated fusion probability. 48Ca, 48Ti, 90,96Zr(40Ca, X), E(cm)=48-112 MeV; 46Ti(46Ti, X), E(cm)=58-72 MeV; 89Y(32S, X), (34S, X), E(cm)=72-92 MeV; 92Zr(28Si, X), (35Cl, X), E(cm)=65-100 MeV; 64Ni(132Sn, X), E(cm)=140-168 MeV; calculated fusion σ. Improved quantum molecular dynamics model, comparison with data.
doi: 10.1103/PhysRevC.69.034608
2003LI44 Chin.Phys.Lett. 20, 1706 (2003) Limiting Temperatures for Finite Nuclear Systems NUCLEAR STRUCTURE A=20-250; calculated mass dependence of limiting temperatures.
doi: 10.1088/0256-307X/20/10/315
2001LI49 Phys.Lett. 516B, 293 (2001) F.Liu, H.Liao, M.Liu, F.Liu, L.Liu A Monte Carlo Study of Erraticity Behavior in Nucleus-Nucleus Collisions at High Energies NUCLEAR REACTIONS Pb(Pb, X), Ag(Ag, X), 197Au(O, X), (S, X), S(S, X), E=high; calculated average multiplicity, entropy, event-by-event fluctuation features. Monte Carlo simulation, erraticity method.
doi: 10.1016/S0370-2693(01)00960-1
1999AH07 Phys.Rev. C60, 064601 (1999) I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, C.M.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, Th.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.M.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, A.R.Young, J.E.Yurkon Positron-Electron Pairs Produced in Heavy-Ion Collisions NUCLEAR REACTIONS 232Th(238U, X), E=5.95 MeV/nucleon; 181Ta(238U, X), E=5.95, 6.1, 6.3 MeV/nucleon; measured positron, electron spectra, multiplicities, e-e+-coin, angular correlation; deduced no sharp structure in sum-energy spectra. APEX spectrometer.
doi: 10.1103/PhysRevC.60.064601
1999PA56 High Energy Phys. and Nucl.Phys. (China) 23, 1039 (1999) Q.Pan, S.Yuan, W.Yang, Z.Li, T.Ma, J.Guo, M.Liu, H.Liu, S.Xu, Z.Gan, D.Kong, J.Qiao, Z.Luo, M.Zhang, S.Wang Observation of Heavy Cluster Emission From Radioactive 230U Nuclei
1997AH01 Phys.Rev.Lett. 78, 618 (1997) I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.R.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration Search for Monoenergetic Positron Emission from Heavy-Ion Collisions at Coulomb-Barrier Energies NUCLEAR REACTIONS 181Ta(238U, X), E=5.95-6.3 MeV/nucleon; 232Th(238U, X), E=5.95 MeV/nucleon; measured positron energy spectra; deduced no structure.
doi: 10.1103/PhysRevLett.78.618
1997AH04 Phys.Rev. C55, R2755 (1997) I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.A.Chishti, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, J.S.Greenberg, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration Internal Pair Conversion in Heavy Nuclei NUCLEAR REACTIONS 206Pb(206Pb, X), E=5.90 MeV/nucleon; measured e+e--sum energy spectra, Doppler corrected Eγ; deduced internal pair conversion to gamma branching ratio. 232Th(208Pb, X), E=5.80 MeV/nucleon; 238U(208Pb, X), E=5.80 MeV/nucleon; 181Ta(238U, X), E=5.95 MeV/nucleon; 232Th(238U, X), E=5.90 MeV/nucleon; measured e+e--sum energy, Doppler corrected Eγ; deduced no discrete lines evidence in e+e- spectra. 238U deduced new levels evidence.
doi: 10.1103/PhysRevC.55.R2755
1997AH05 Z.Phys. A358, 235 (1997) I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, A.Young, J.E.Yurkon, and the APEX Collaboration The Positron-Electron Peak Puzzle: Results from APEX NUCLEAR REACTIONS 232Th(238U, X), E=5.78-5.95 MeV/nucleon; 181Ta(238U, X), E=5.79-6.3 MeV/nucleon; measured total (e+)(heavy-ion)-, (e+e-)(heavy-ion)-coin events number; deduced very low light neutral particle production upper limits.
doi: 10.1007/s002180050316
1996AH05 Acta Phys.Pol. B27, 387 (1996) I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.Gazes, A.L.Hallin, T.Happ, N.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, A.Young, J.E.Yurkon, and the APEX Collaboration The Positron Peak Puzzle - Recent Results from APEX NUCLEAR REACTIONS 232Th(238U, X), E=5.95 MeV/nucleon; 181Ta(238U, X), E=5.96-6.3 MeV/nucleon; 206Pb(206Pb, X), E not given; analyzed e+e--sum energy spectra. 232Th, 238U(208Pb, X), E=5.8 MeV/nucleon; 232Th, 181Ta(238U, X), E=5.95 MeV/nucleon; 206Pb(206Pb, X), E=5.9 MeV/nucleon; analyzed Doppler reconstructed γ spectra; deduced limits on 1.78 MeV 238U transition possible contribution to (heavy ion)γ-coin.
1996AH07 Nucl.Instrum.Methods Phys.Res. A370, 539 (1996) I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, J.S.Greenberg, J.P.Greene, A.L.Hallin, Th.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.M.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.R.Young, J.E.Yurkon A Solenoidal Spectrometer for Positron-Electron Pairs Produced in Heavy-Ion Collisions RADIOACTIVITY 85Sr(EC); 113Sn(EC); 203Hg(β-); measured electron spectra; deduced apparatus response, efficiency. New solenoidal spectrometer. NUCLEAR REACTIONS 181Ta(238U, X), E=6.1 MeV/nucleon; measured γ-, positron energy spectra. New solenoidal spectrometer.
doi: 10.1016/0168-9002(95)00829-2
1996PE14 Appl.Radiat.Isot. 47, 309 (1996) Excitation Functions and Yields of the Reactions Induced by Alpha-Particle Bombardment of Natural Silver NUCLEAR REACTIONS 107Ag(α, n), (α, 2n), (α, np), 109Ag(α, 2n), E=threshold-26.3 MeV; measured residuals production σ(E); calculated thick target yields. Stacked natural Ag target, activation technique.
doi: 10.1016/0969-8043(95)00276-6
1995AH01 Nucl.Phys. A583, 247c (1995) I.Ahmad, S.M.Austin, B.B.Back, D.Bazin, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, J.S.Greenberg, A.L.Hallin, T.Happ, J.Last, N.Kaloskamis, E.Kashy, W.Kutschera, C.J.Lister, M.Liu, M.R.Maier, D.Mercer, A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon Positron Production in Heavy Ion Collisions: Current status of the problem NUCLEAR REACTIONS 181Ta(238U, X), E=5.9-6.3 MeV/nucleon; compiled, analyzed, reviewed electron, positron production data.
doi: 10.1016/0375-9474(94)00667-C
1995AH06 Phys.Rev.Lett. 75, 2658 (1995) I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration Search for Narrow Sum-Energy Lines in Electron-Positron Pair Emission from Heavy-Ion Collisions Near the Coulomb Barrier NUCLEAR REACTIONS 181Ta(238U, X), E=5.95-6.3 MeV/nucleon; 232Th(238U, X), E=5.95 MeV/nucleon; measured pair emission sum spectra; deduced no sharp lines evidence, neutral particle isolated decay related features.
doi: 10.1103/PhysRevLett.75.2658
1994ME24 Nucl.Instrum.Methods Phys.Res. A350, 491 (1994) D.J.Mercer, D.Mikolas, J.Yurkon, S.M.Austin, D.Bazin, S.Gaff, E.Kashy, D.Kataria, J.S.Winfield, R.R.Betts, D.J.Henderson, A.L.Hallin, M.Liu, F.L.H.Wolfs A Large Solid-Angle Array for Heavy Ions from APEX NUCLEAR REACTIONS 58Ni(58Ni, 58Ni), E=200 MeV; measured σ(θ). 181Ta(238U, X), E=1.45 GeV; measured fragment tof, mass spectra. Large solid-angle array of low pressure multi-wire proportional counters. Other reactions studied.
doi: 10.1016/0168-9002(94)91249-1
1994XI05 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p.251 (1994) Y.J.Xia, X.-G.Long, X.-B.Luo, Z.Yang, M.Liu, F.He, C.Wang, X.F.Pen, J.Yang Activation cross section measurement for the Eu-(n, γ) reactions NUCLEAR REACTIONS 151Eu(n, γ), 153Eu(n, γ), E=22 keV-1.1 MeV; measured products, 152Eu, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 32623.
1992PE07 Nucl.Instrum.Methods Phys.Res. B68, 145 (1992) Excitation Functions for 107Ag(d, 2n)107Cd, 109Ag(d, 2n)109Cd and 109Ag(d, p)110mAg Reactions NUCLEAR REACTIONS, ICPND 107,109Ag(d, 2n), 109Ag(d, p), E ≤ 13.3 MeV; measured σ(E). Activation technique, natural Ag target, stacked foils.
doi: 10.1016/0168-583X(92)96066-8
1991LO09 Appl.Radiat.Isot. 42, 1234 (1991) Production of Cadmium-107 and Cadmium-109 by Deuteron Bombardment of Silver NUCLEAR REACTIONS, ICPND 107,109Ag(d, 2n), E ≤ 13.3 MeV; measured residuals production σ(E); calculated thick target yields. Natural target, activation technique, hyperpure Ge detector.
doi: 10.1016/0883-2889(91)90203-D
1991XU05 High Energy Phys. and Nucl.Phys. (China) 15, 170 (1991) S.Xu, S.Yuan, J.Guo, M.Liu, E.Hagberg, V.T.Koslowsky, G.Dyck, J.C.Hardy, H.Schmeing The Decay of 120Ba
1990XI04 Chin.J.Nucl.Phys. 12, No 3, 261 (1990) Y.Xia, C.Wang, J.Yang, Z.Yang, M.Liu Measurement of Maxwellian Averaged Neutron Capture Cross Section of 140,142Ce, 139La and 181Ta at kT = 24 keV NUCLEAR REACTIONS 140,142Ce, 139La, 181Ta(n, γ), E ≤ 250 keV; measured Eγ, Iγ following capture; deduced Maxwellian averaged capture σ. Hyperpure Ge detector.
1989LO13 Chin.J.Nucl.Phys. 11, No.3, 25 (1989) Isomeric Cross Section Ratios in 55Mn(α, n)58m,gCo Reaction NUCLEAR REACTIONS 55Mn(α, n), E=10.4-26.5 MeV; measured residual isomer to ground state production σ ratio. Activation method, stacked foil technique.
1989YU01 Phys.Rev. C39, 256 (1989) Yuan Shuanggui, Zhang Tianmei, Xu Shuwei, Li Wenxin, Zhang Li, Liu Manqing, Ou Xiulan, Li Weisheng Determination of the 235Th β-Decay End Point Energy RADIOACTIVITY 235Th(β-); measured β-, γ-spectra, Eβ, T1/2; deduced Qβ. Semiconductor telescope, hyperpure Ge detector.
doi: 10.1103/PhysRevC.39.256
1988YU06 High Energy Phys. and Nucl.Phys. (China) 12, 712 (1988) S.Yuan, T.Zhang, S.Xu, W.Li, L.Zhang, M.Liu, X.Ou, W.Li The Determination of endpoint energy for 235Th β-decay
1988YU07 High Energy Phys. and Nucl.Phys. (China) 12, 712 (1988) S.Yuan, T.Zhang, S.Xu, W.Li, L.Zhang, M.Liu, X.Ou, W.Li The Determination of endpoint energy for 235Th ν-decay
1971LI11 Nucl.Phys. A165, 118 (1971) M.Liu, W.von Oertzen, J.C.Jacmart, F.Pougheon, M.Riou, J.C.Roynette, C.Stephan Investigation of One-Nucleon Transfer Reactions between Complex Nuclei At Incident Energies between 3 MeV/Nucleon and 8 MeV/Nucleon NUCLEAR REACTIONS 11B(14N, 14N), (14N, 15O), (14N, 13C), E=41, 77, 113 MeV; 11B(12C, 12C), (12C, 11B), 12C(12C, 12C), 13C(12C, 12C)(12C, 13C), E=87 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1016/0375-9474(71)90152-7
1970VO02 Nucl.Phys. A143, 34 (1970) W.Von Oertzen, M.Liu, C.Caverzasio, J.C.Jacmart, F.Pougheon, M.Riou, J.C.Roynette, C.Stephan Direct Reactions Induced by 14N on 12C at 78 MeV NUCLEAR REACTIONS 12C(14N, 14N), 12C(14N, 14N'), 12C(14N, 13C), 12C(14N, 13N), E=78 MeV; measured σ(θ). DWBA analysis. Natural targets.
doi: 10.1016/0375-9474(70)90678-0
1969VO01 Phys.Letters 28B, 482(1969) W.Von Oertzen, J.C.Jacmart, M.Liu, F.Pougheon, J.C.Roynette, M.Riou A Heavy-Ion Reaction Leading to Members of an Isospin Multiplet: 14N+12C→13N+13C NUCLEAR REACTIONS 12C(14N, 13C), (14N, 13N), E=78 MeV; measured σ(E(13N), E(13C), θ).
doi: 10.1016/0370-2693(69)90522-X
1967RI02 Nucl.Phys. A91, 609 (1967) R.A.Ricci, J.C.Jacmart, M.Liu, M.Riou, C.Ruhla Etude des Noyaux de Masse Moyenne par Diffusion Inelastique de Protons de 155 MeV (II). Diffusion Inelastique sur Quelques Noyaux f7/2(48Ti, 52Cr, 56Fe, 51V et 59Co) NUCLEAR REACTIONS 48Ti, 52Cr, 56Fe, 51V, 59Co(p, p'), E = 155 MeV; measured σ(Ep', θ). 48Ti, 52Cr, 56Fe, 51V, 59Co deduced levels, J, π, B(EL).
doi: 10.1016/0375-9474(67)90580-5
1967RU03 Nucl.Phys. A95, 526 (1967) C.Ruhla, M.Arditi, H.Doubre, J.C.Jacmart, M.Liu, R.A.Ricci, M.Riou, J.C.Roynette Reactions (p, 2p) a 156 MeV (I). Noyaux de Z = 20 a Z = 28 NUCLEAR REACTIONS 40Ca, 45Sc, 48Ti, 51V, 52Cr, 55Mn, 56Fe, 59Co, 58Ni(p, 2p), E = 156 MeV; measured σ(Ep1+Ep2; θ). 39K, 44Ca, 47Sc, 50Ti, 51V, 54Cr, 55Mn, 58Fe, 57Co deduced L. Enriched 48Ti, 58Ni targets.
doi: 10.1016/0375-9474(67)90847-0
1966LI02 Nucl.Phys. 75, 481(1966) M.Liu, J.C.Jacmart, R.A.Ricci, M.Riou, C.Ruhla Etude des Noyaux de Masse Moyenne par Diffusion Inelastique de Protons de 155 MeV (I). Diffusion Inelastique sur 23Na, 27Al, 28Si, 31P, 32S, 39K et 40Ca NUCLEAR REACTIONS 23Na, 27Al, 28Si, 31P, 32S, 39K, 40Ca(p, p'), Ep=155 MeV; measured σ(Ep', θ). 23Na, 27Al, 28Si, 31P, 32S, 39K, 40Ca deduced levels, J, π, B(EL).
doi: 10.1016/0029-5582(66)90972-2
1964JA02 Phys.Letters 8, 273 (1964) J.C.Jacmart, M.Liu, R.A.Ricci, M.Riou, C.Ruhla Diffusion Inelastique de Protons de 155 MeV sur Na23, Al27, P31, K39, Ti48, Cr52, Fe56, et Co59 NUCLEAR STRUCTURE 27Al, 23Na, 52Cr, 56Fe, 59Co, 31P, 48Ti, 39K; measured not abstracted; deduced nuclear properties.
doi: 10.1016/S0031-9163(64)91717-2
1964RU05 Phys.Letters 10, 326 (1964) C.Ruhla, M.Riou, R.A.Ricci, M.Arditi, H.Doubre, J.C.Jacmart, M.Liu, L.Valentin Etudes des Reactions p, 2p a 150 MeV sur Ca40, Sc45, Ti48, V51 NUCLEAR STRUCTURE 40Ca, 44Ca, 39K, 45Sc, 51V, 47Sc, 48Ti, 50Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90526-8
1963HO26 J.Phys. 24, 1052 (1963) W.F.Hornyak, J.C.Jacmart, M.Riou, J.P.Garron, C.Ruhla, M.Liu Diffusion Inelastique de Protons de 155 MeV sur 28Si, 32S et 40Ca NUCLEAR STRUCTURE 32S, 28Si, 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphys:0196300240110105201
1963RU05 Phys.Letters 6, 282 (1963) C.Ruhla, M.Riou, M.Gusakow, J.C.Jacmart, M.Liu, L.Valentin Etude des Reactions Li6(p, pd) et (p, pα) et Be9(p, α) a 155 MeV NUCLEAR STRUCTURE 9Be, 6Li; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90474-8
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