NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Y.Xu Found 145 matches. Showing 1 to 100. [Next]2024WA02 Phys.Rev. C 109, 014611 (2024) Systematic study of the radiative proton capture including the compound, pre-equilibrium, and direct mechanisms
doi: 10.1103/PhysRevC.109.014611
2024WA03 Phys.Rev. C 109, 014621 (2024) Y.H.Wang, D.Y.Pang, W.D.Chen, Y.P.Xu, W.L.Hai, R.Y.Chen Nuclear radii from total reaction cross section measurements at intermediate energies with complex turning point corrections to the eikonal model
doi: 10.1103/PhysRevC.109.014621
2024WI01 Nuovo Cim. C 47, 24 (2024) O.Wieland, A.Bracco, F.Camera, S.Aogaki, D.L.Balabanski, E.Boicu, R.Borcea, M.Boromiza, I.Burducea, S.Calinescu, A.Coman, P.Constantin, C.Costache, M.Ciemala, Gh.Ciocan, C.Clisu, F.C.L.Crespi, M.Cuciuc, A.Dhal, N.Djourelov, N.M.Florea, I.Gheorghe, A.Giaz, D.Iancu, D.M.Kahl, M.Kmiecik, A.Kusoglu, R.Lica, N.Mvarginean, A.Maj, R.Marginean, C.Mihai, R.E.Mihai, B.Million, C.Neacsu, D.Nichita, C.Nitva, H.Pai, A.Pappalardo, T.Petruse, A.Rotaru, A.B.Serban, P.-A.Soderstrom, C.O.Sotty, L.Stan, A.N.State, I.Stiru, A.Stoica, D.A.Testov, S.Toma, T.Tozar, A.Turturica, G.V.Turturica, S.Ujeniuc, V.Vasilca, Y.Xu Extra yield in hot Ni isotopes below the Giant Dipole Resonance NUCLEAR REACTIONS 24Mg(32S, X)56Ni, E=90 MeV; 26Mg(34S, X)60Ni, E=79 MeV; 26Mg(36S, X)62Ni, E=78 MeV; measured reaction products, Eγ, Iγ; deduced yields, linearized measured γ-ray yields, the tail of the Giant Dipole Resonance which may be attributed to a Pygmy Dipole Resonance in an excited nucleus with statistical model using a Monte Carlo approach. The IFIN 9 MV Tandem facility.
doi: 10.1393/ncc/i2024-24024-1
2024XU04 Chin.Phys.C 48, 024106 (2024) Y.-L.Xu, X.-W.Su, Zh.-H.Sun, Y.-L.Han, X.-J.Sun, D.-H.Zhang, Ch.-H.Cai Description of elastic scattering for 7Li-induced reactions on 1p-shell nuclei NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 15N, 16O(7Li, 7Li), E=4.5-131.8 MeV; analyzed available data; deduced σ(θ), the global phenomenological optical potentials (GPOPs), the contribution of elastic transfer by the distorted wave Born approximation (DWBA) method.
doi: 10.1088/1674-1137/ad1924
2024ZO01 J.Phys.(London) G51, 045103 (2024) Y.-T.Zou, J.-H.Cheng, Y.-Y.Xu, Q.Xiao, S.-M.Liu, F.-Q.Shao, T.-P.Yu Laser-assisted two-proton radioactivity RADIOACTIVITY 6Be, 12O, 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); calculated the two-proton radioactivity assisted by an ultra-intense laser field within a deformed one-parameter model (OPM); deduced the lasers characterized by shorter wavelengths and higher intensities exert a more significant influence on the rate of the average change in pulse duration, T1/2.
doi: 10.1088/1361-6471/ad2691
2023AB32 Phys.Rev. D 108, 092009 (2023) K.Abe, N.Akhlaq, R.Akutsu, A.Ali, S.Alonso Monsalve, C.Alt, C.Andreopoulos, M.Antonova, S.Aoki, T.Arihara, Y.Asada, Y.Ashida, E.T.Atkin, M.Barbi, G.J.Barker, G.Barr, D.Barrow, M.Batkiewicz-Kwasniak, V.Berardi, L.Berns, S.Bhadra, A.Blanchet, A.Blondel, S.Bolognesi, T.Bonus, S.Bordoni, S.B.Boyd, A.Bravar, C.Bronner, S.Bron, A.Bubak, M.Buizza Avanzini, J.A.Caballero, N.F.Calabria, S.Cao, D.Carabadjac, A.J.Carter, S.L.Cartwright, M.P.Casado, M.G.Catanesi, A.Cervera, J.Chakrani, D.Cherdack, P.S.Chong, G.Christodoulou, A.Chvirova, M.Cicerchia, J.Coleman, G.Collazuol, L.Cook, A.Cudd, C.Dalmazzone, T.Daret, Yu.I.Davydov, A.De Roeck, G.De Rosa, T.Dealtry, C.C.Delogu, C.Densham, A.Dergacheva, F.Di Lodovico, S.Dolan, D.Douqa, T.A.Doyle, O.Drapier, J.Dumarchez, P.Dunne, K.Dygnarowicz, A.Eguchi, S.Emery-Schrenk, G.Erofeev, A.Ershova, G.Eurin, D.Fedorova, S.Fedotov, M.Feltre, A.J.Finch, G.A.Fiorentini Aguirre, G.Fiorillo, M.D.Fitton, J.M.Franco Patino, M.Friend, Y.Fujii, Y.Fukuda, Y.Furui, L.Giannessi, C.Giganti, V.Glagolev, M.Gonin, J.Gonzalez Rosa, E.A.G.Goodman, A.Gorin, M.Grassi, M.Guigue, D.R.Hadley, J.T.Haigh, P.Hamacher-Baumann, D.A.Harris, M.Hartz, T.Hasegawa, S.Hassani, N.C.Hastings, Y.Hayato, D.Henaff, M.Hogan, J.Holeczek, A.Holin, T.Holvey, N.T.Hong Van, T.Honjo, A.K.Ichikawa, M.Ikeda, T.Ishida, M.Ishitsuka, H.T.Israel, A.Izmaylov, M.Jakkapu, B.Jamieson, S.J.Jenkins, C.Jesus-Valls, J.J.Jiang, J.Y.Ji, P.Jonsson, S.Joshi, C.K.Jung, P.B.Jurj, M.Kabirnezhad, A.C.Kaboth, T.Kajita, H.Kakuno, J.Kameda, S.P.Kasetti, Y.Kataoka, T.Katori, M.Kawaue, E.Kearns, M.Khabibullin, A.Khotjantsev, T.Kikawa, S.King, V.Kiseeva, J.Kisiel, H.Kobayashi, T.Kobayashi, L.Koch, S.Kodama, A.Konaka, L.L.Kormos, Y.Koshio, T.Koto, K.Kowalik, Y.Kudenko, Y.Kudo, S.Kuribayashi, R.Kurjata, T.Kutter, M.Kuze, M.La Commara, L.Labarga, K.Lachner, J.Lagoda, S.M.Lakshmi, M.Lamers James, M.Lamoureux, A.Langella, J.-F.Laporte, D.Last, N.Latham, M.Laveder, L.Lavitola, M.Lawe, Y.Lee, C.Lin, S.-K.Lin, R.P.Litchfield, S.L.Liu, W.Li, A.Longhin, K.R.Long, A.Lopez Moreno, L.Ludovici, X.Lu, T.Lux, L.N.Machado, L.Magaletti, K.Mahn, M.Malek, M.Mandal, S.Manly, A.D.Marino, L.Marti-Magro, D.G.R.Martin, M.Martini, J.F.Martin, T.Maruyama, T.Matsubara, V.Matveev, C.Mauger, K.Mavrokoridis, E.Mazzucato, N.McCauley, J.McElwee, K.S.McFarland, C.McGrew, J.McKean, A.Mefodiev, G.D.Megias, P.Mehta, L.Mellet, C.Metelko, M.Mezzetto, E.Miller, A.Minamino, O.Mineev, S.Mine, M.Miura, L.Molina Bueno, S.Moriyama, S.Moriyama, P.Morrison, Th.A.Mueller, D.Munford, L.Munteanu, K.Nagai, Y.Nagai, T.Nakadaira, K.Nakagiri, M.Nakahata, Y.Nakajima, A.Nakamura, H.Nakamura, K.Nakamura, K.D.Nakamura, Y.Nakano, S.Nakayama, T.Nakaya, K.Nakayoshi, C.E.R.Naseby, T.V.Ngoc, V.Q.Nguyen, K.Niewczas, S.Nishimori, Y.Nishimura, K.Nishizaki, T.Nosek, F.Nova, P.Novella, J.C.Nugent, H.M.O'Keeffe, L.O'Sullivan, T.Odagawa, W.Okinaga, K.Okumura, T.Okusawa, N.Ospina, Y.Oyama, V.Palladino, V.Paolone, M.Pari, J.Parlone, J.Pasternak, M.Pavin, D.Payne, G.C.Penn, D.Pershey, L.Pickering, C.Pidcott, G.Pintaudi, C.Pistillo, B.Popov, K.Porwit, M.Posiadala-Zezula, Y.S.Prabhu, F.Pupilli, B.Quilain, T.Radermacher, E.Radicioni, B.Radics, M.A.Ramirez, P.N.Ratoff, M.Reh, C.Riccio, E.Rondio, S.Roth, N.Roy, A.Rubbia, A.C.Ruggeri, C.A.Ruggles, A.Rychter, K.Sakashita, F.Sanchez, C.M.Schloesser, K.Scholberg, M.Scott, Y.Seiya, T.Sekiguchi, H.Sekiya, D.Sgalaberna, A.Shaikhiev, F.Shaker, M.Shiozawa, W.Shorrock, A.Shvartsman, N.Skrobova, K.Skwarczynski, D.Smyczek, M.Smy, J.T.Sobczyk, H.Sobel, F.J.P.Soler, Y.Sonoda, A.J.Speers, R.Spina, I.A.Suslov, S.Suvorov, A.Suzuki, S.Y.Suzuki, Y.Suzuki, M.Tada, S.Tairafune, S.Takayasu, A.Takeda, Y.Takeuchi, K.Takifuji, H.K.Tanaka, M.Tani, A.Teklu, V.V.Tereshchenko, N.Thamm, L.F.Thompson, W.Toki, C.Touramanis, T.Towstego, K.M.Tsui, T.Tsukamoto, M.Tzanov, Y.Uchida, M.Vagins, D.Vargas, M.Varghese, G.Vasseur, C.Vilela, E.Villa, W.G.S.Vinning, U.Virginet, T.Vladisavljevic, T.Wachala, J.G.Walsh, Y.Wang, L.Wan, D.Wark, M.O.Wascko, A.Weber, R.Wendell, M.J.Wilking, C.Wilkinson, J.R.Wilson, K.Wood, C.Wret, J.Xia, Y.-h.Xu, K.Yamamoto, T.Yamamoto, C.Yanagisawa, G.Yang, T.Yano, K.Yasutome, N.Yershov, U.Yevarouskaya, M.Yokoyama, Y.Yoshimoto, N.Yoshimura, M.Yu, R.Zaki, A.Zalewska, J.Zalipska, K.Zaremba, G.Zarnecki, X.Zhao, T.Zhu, M.Ziembicki, E.D.Zimmerman, M.Zito, S.Zsoldos Measurements of the νμ and ν-barμ-induced coherent charged pion production cross sections on 12C by the T2K experiment NUCLEAR REACTIONS 12C(ν, μ-), (ν-bar, μ+), E ∼ 0.8 GeV; measured reaction products; deduced coherent charged pion production σ in the Tokai-to-Kamioka experiment.
doi: 10.1103/PhysRevD.108.092009
2023JA13 Astrophys.J. 955, 51 (2023) R.Jain, E.F.Brown, H.Schatz, A.V.Afanasjev, M.Beard, L.R.Gasques, S.S.Gupta, G.W.Hitt, W.R.Hix, R.Lau, P.Moller, W.J.Ong, M.Wiescher, Y.Xu Impact of Pycnonuclear Fusion Uncertainties on the Cooling of Accreting Neutron Star Crusts NUCLEAR REACTIONS 40Mg(40Mg, X)80Cr, 44Mg(40Mg, X)84Cr, 44Mg(44Mg, X)88Cr, 44Mg(38Ne, X)82Ti, 40Mg(38Ne, X)78Ti, 32Ne(32Ne, X)64Ca, 32Ne(30Ne, X)62Ca, 30Ne(30Ne, X)60Ca, 40Mg(24O, X), E not given; calculated abundances, pycnonuclear fusion rates using the reaction network with the thermal evolution code dStar. 56Fe; deduced impact of uncertainties on the depth at which nuclear heat is deposited although the total heating remains constant.
doi: 10.3847/1538-4357/acebc4
2023LI45 Chin.Phys.C 47, 094103 (2023) X.Liu, J.-D.Jiang, L.-J.Qi, Y.-Y.Xu, X.-J.Wu, X.-H.Li Systematic calculations of cluster radioactivity half-lives with a screened electrostatic barrier RADIOACTIVITY 221Fr, 221,222,223,224Ra, 226Ra, 223Ac(14C), 228Th(20O), 231Pa(23F), 230Th, 231Pa, 232,233,234U(24Ne), 234U, 233U(25Ne), 234U(26Ne), (28Mg), 236,238Pu(28Mg), 238Pu(30Mg), (32Si), 242Cm(34Si); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/ace351
2023SE09 Phys.Rev. C 107, L061302 (2023) D.Seweryniak, T.Huang, K.Auranen, A.D.Ayangeakaa, B.B.Back, M.P.Carpenter, P.Chowdhury, R.M.Clark, P.A.Copp, Z.Favier, K.Hauschild, X.-T.He, T.L.Khoo, F.G.Kondev, A.Korichi, T.Lauritsen, J.Li, C.Morse, D.H.Potterveld, G.Savard, S.Stolze, J.Wu, J.Zhang, Y.-F.Xu Nuclear rotation at the fission limit in 254Rf NUCLEAR REACTIONS 206Pb(50Ti, 2n)254Rf, E=244 MeV from the ATLAS-ANL facility; measured reaction products, prompt γ rays, Eγ, Iγ, Rf Kα and Kβ x-rays, (254Rf implants)γ-coin, (implants)(fission events)γ-coin using the Gammasphere array and the Argonne gas-filled analyzer (AGFA). 254Rf; deduced levels, J, π, ground-state rotational band up to 14+, kinematic moment of inertia. Systematics of ground-state bands in 250Fm, 252,254No, and 254,256Rf, and comparison with particle-number conserving cranked shell model (PNC-CSM) calculations.
doi: 10.1103/PhysRevC.107.L061302
2023WA36 Phys.Rev. C 108, 065805 (2023) Effective energy window of the E1 photon strength function for astrophysical neutron-capture reaction rates
doi: 10.1103/PhysRevC.108.065805
2023XI06 J.Phys.(London) G50, 085102 (2023) Q.Xiao, J.-H.Cheng, B.-L.Wang, Y.-Y.Xu, Y.-T.Zou, T.-P.Yu Half-lives for proton emission and α decay within the deformed Gamow-like model RADIOACTIVITY 109I, 112,113Cs, 117La, 121Pr, 131Eu, 135Tb, 140,141Ho, 144,145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 170,171Au, 176,177Tl, 185Bi, 111Cs, 127Pm, 137Tb(p), 106,108Te, 108,110,112Xe, 114Ba, 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156Yb, 156,158,160,162Hf, 174Hf, 158,160,162,164,166,168W, 180W, 162,164,166,168,170,172,174Os, 186Os, 168,170,172,174,176,178,180,182,184,186,188,190Pt, 170,172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194Pb, 210Pb, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210Ra, 214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230,232Th, 216,218,220,222,224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288,290Fl, 290,292Lv, 294Og, 105Te, 109Te, 109Xe, 147Sm, 149,151Gd, 151,153Dy, 153,155Er, 155Yb, 157,159Hf, 161,163W, 167W, 161Os, 167,169,171,173Os, 171,173,175,177,179,181,183,185Pt, 175,177,179,181,183,185Hg, 183,185,187,189Pb, 187,189,191,193,195,197,199,201,203,205,207,209,211,213,215,217,219Po, 193,195,197,199Rn, 203,205,207,209,211,213,215,217,219,221Rn, 201,203,205,207,209,211,213,215,217,219,221,223Ra, 211,213,215,217,219,221,223,225,227Th, 221,223,225,227,229,231,233,235U, 229,231,233,235,237,239,241Pu, 233Cm, 239,241,243,245,247Cm, 237Cf, 245,247,249,251,253Cf, 249,251,253,255,257Fm, 255,257,259No, 257Rf, 261Rf, 261Sg, 265Hs, 109I, 113I, 145Pm, 147Eu, 151Tb, 151,153Ho, 155,157Tm, 155Lu, 157,159Ta, 163,165Re, 167,169,171,173,175,177Ir, 173,175,177,179,181,183,185Au, 177,179,181Tl, 187,189,191,193,195Bi, 193,195,197,199,201,203,205,207,209,211,213,215,217,219,221,223,225,227Ac, 211,213,215,217,219,221,223,225,227,229,231Pa, 219Np, 223,225,227,229,231,233,235,237Np, 229Am, 235Am, 239,241,243Am, 243,245,247,249Bk, 247Es, 251,253Es, 249,251Md, 255,257Md, 253,255Lr, 259Lr, 259Db, 261Bh, 110,112I, 114Cs, 152,154Ho, 154,156Tm, 158Lu, 158Ta, 162Ta, 160,162Re, 168Re, 166,168Ir, 172,174Ir, 170Au, 176Au, 180Tl, 186Bi, 192,194Bi, 212,214Bi, 192At, 200,202,204,206,208,210,212,214,216,218At, 200Fr, 204,206,208,210,212,214,216,218,220Fr, 216,218,220,222,224,226Ac, 212Pa, 224Pa, 228,230Pa, 236Np, 236Am, 244Bk, 248Es, 258Md, 272Rg(α); calculated T1/2 with the deformed Gamow-like model, which introduces the effects of nucleus deformation; deduced the deformed model follows the Geiger-Nuttall law. Comparison with available data.
doi: 10.1088/1361-6471/acdfeb
2022AL01 J.Phys.(London) G49, 010501 (2022) M.Aliotta, R.Buompane, M.Couder, A.Couture, R.J.deBoer, A.Formicola, L.Gialanella, J.Glorius, G.Imbriani, M.Junker, C.Langer, A.Lennarz, Y.A.Litvinov, W.-P.Liu, M.Lugaro, C.Matei, Z.Meisel, L.Piersanti, R.Reifarth, D.Robertson, A.Simon, O.Straniero, A.Tumino, M.Wiescher, Y.Xu The status and future of direct nuclear reaction measurements for stellar burning NUCLEAR REACTIONS 12C(α, γ), 22Ne(α, n), (α, γ), 12C(12C, X), E(cm)<7 MeV; analyzed available data; deduced σ, S-factors.
doi: 10.1088/1361-6471/ac2b0f
2022HU21 Phys.Rev. C 106, L061301 (2022) T.Huang, D.Seweryniak, B.B.Back, P.C.Bender, M.P.Carpenter, P.Chowdhury, R.M.Clark, P.A.Copp, X.-T.He, R.D.Herzberg, D.E.M.Hoff, H.Jayatissa, T.L.Khoo, F.G.Kondev, G.Morgan, C.Morse, A.Korichi, T.Lauritsen, C.Muller-Gatermann, D.H.Potterveld, W.Reviol, A.M.Rogers, S.Saha, G.Savard, K.Sharma, S.Stolze, S.Waniganeththi, G.L.Wilson, J.Wu, Y.-F.Xu, S.Zhu Discovery of the new isotope 251Lr: Impact of the hexacontetrapole deformation on single-proton orbital energies near the Z=100 deformed shell gap NUCLEAR REACTIONS 203Tl(50Ti, 2n)251Lr, 205Tl(50Ti, 2n)253Lr, E=237 MeV; measured reaction products, α-decay of the reaction products, Eα, Iα. 251,253Lr; deduced levels J, π, α-decay width. 251,253,255Lr; calculated single-proton levels near the Fermi surface. Calculations with particle-number conserving cranked shell model. Beam delivered to target by ATLAS linear accelerator and recoiling reaction products were separated in the Argonne Gas-Filled Analyzer (AGFA) at (ANL). Decay of the implanted reaction products was measured in pixelized double-sided Si strip detector (DSSD). RADIOACTIVITY 251,253Lr(α)[from 203,205Tl(50Ti, 2n), E=237 MeV]; measured Eα, Iα; deduced T1/2, Q-value, α-decay branchings and widths. Comparison to other experimental data. and predictions of theoretical models.
doi: 10.1103/PhysRevC.106.L061301
2022LA06 Phys.Rev. C 105, 044618 (2022) H.Y.Lan, W.Luo, Y.Xu, D.L.Balabanski, G.L.Guardo, M.La Cognata, D.Lattuada, C.Matei, R.G.Pizzone, T.Rauscher, J.L.Zhou Feasibility of studying astrophysically important charged-particle emission with the variable energy γ-ray system at the Extreme Light Infrastructure--Nuclear Physics facility NUCLEAR REACTIONS 29Si, 47Ti, 56Fe, 73Ge, 74Se, 84Sr, 91Zr, 95Mo, 96,98Ru, 102Pd, 106Cd, 115,117,119Sn, 132Ba, 143Nd(γ, p), (γ, np), E<30 MeV; 50V, 67Zn, 87Sr, 107Ag, 113,115In, 119Sn, 123,125Te, 149,154Sm, 155,156,157,158,160Gd, 208Pb(γ, α), (γ, nα), E<30 MeV; calculated inclusive and exclusive σ(E), population of the particular excited states, energy spectra of ejectiles. TALYS-1.9 calculations with various combinations of level densities, strength functions and optical potentials available in the code.Investigated the feasibility of studying the reactions of astrophysical interest with ELI-NP facility infrastructure. Simulated achievable yields.
doi: 10.1103/PhysRevC.105.044618
2022LU11 Eur.Phys.J. A 58, 244 (2022) S.Luo, Y.-Y.Xu, D.-X.Zhu, B.He, P.-C.Chu, X.-H.Li Improved Geiger-Nuttall law for α-decay half-lives of heavy and superheavy nuclei RADIOACTIVITY 220,222,224,226,228,230,232Th, 222,224,226,228,230,232,234,236,238U, 230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 244,246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260Sg, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288Fl, 292Lv, 294Og, 221,223,225,227,229Th, 221,223,225,227,229,231Pa, 223,225,227,229,231,233U, 233,235,237Np, 229,231,233,235Pu, 245,247,249,251,253,255Es, 241,243,245,247,249,251,253,255,257Fm, 245,247,249,251,253,255,257Md, 251,253,255,257,259No, 224,226,228,230Pa, 224,226,228,230,232,234,236Np, 234,236,238,240,242Am, 234Bk, 240,242,244,246Es, 281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317Ts, 282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318Og, 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319119, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320120(α); calculated T1/2. Comparison with available data.
doi: 10.1140/epja/s10050-022-00898-1
2022SU04 Int.J.Mod.Phys. E31, 2250001 (2022) Z.-H.Sun, Y.-L.Xu, X.-J.Sun, Y.-L.Han, C.-H.Cai Global phenomenological optical model potential for 14N-nucleus elastic scattering NUCLEAR REACTIONS 24Mg, 27Al, 28,29Si, 32S, 40Ca, 56Fe, 59Co, 58,62Ni, 70,74Ge, 90Zr, 92,100Mo, 118Sn, 208Pb(14N, 14N), E<100 MeV; analyzed available data; deduced global optical model potential parameters, σ, σ(θ).
doi: 10.1142/S021830132250001X
2022SU13 Nucl.Sci.Eng. 196, 1031 (2022) Theoretical Analysis of Cross Sections for n+46, 47, 49, 50, nat.Ti Reactions NUCLEAR REACTIONS 46,47,49,50Ti, Ti(n, X), E<20 MeV; calculated σ, σ(θ), σ(E), σ(θ, E) using the optical model the unified Hauser-Feshbach theory, the exciton model, which includes the improved Iwamoto-Harada model, and the distorted wave Born approximation theory. Comparison with ENDF/B-VIII, JENDL-4, and JEFF33.
doi: 10.1080/00295639.2022.2049990
2022SU23 Phys.Rev. C 106, 034614 (2022) Y.Z.Sun, S.T.Wang, Y.P.Xu, D.Y.Pang, J.G.Li, C.X.Yuan, L.F.Wan, Y.Qiao, Y.Q.Wang, X.Y.Chen Spectroscopic strength reduction of intermediate-energy single-proton removal from oxygen isotopes NUCLEAR STRUCTURE C(13O, p), E=397 MeV/nucleon;C(14O, p), E=305, 349 MeV/nucleon;C(15O, p), E=308 MeV/nucleon;C(16O, p), E=450 MeV/nucleon;C(17O, p), E=629 MeV/nucleon;C(18O, p), E=573 MeV/nucleon;C(19O, p), E=635 MeV/nucleon;C(20O, p), E=415 MeV/nucleon;C(22O, p), E=414 MeV/nucleon; calculated inclusive single-proton removal σ, shell-model spectroscopic factors, reduction factors of the spectroscopic factors with the experimental data. Glauber reaction model calculations performed with MOMDIS code. Comparison to experimental data obtained at GSI and ETF(Lanzhou, China).
doi: 10.1103/PhysRevC.106.034614
2022XU04 Eur.Phys.J. A 58, 16 (2022) Y.-Y.Xu, H.-M.Liu, D.-X.Zhu, X.Pan, Y.-T.Zou, X.-H.Li, P.-C.Chu An improved formula for the favored α decay half-lives RADIOACTIVITY 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156Yb, 156,158,160,162Hf, 174Hf, 158,160,162,164,166,168W, 180W, 162,164,166,168,170,172,174Os, 186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190Pt, 170,172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194Pb, 210Pb, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 208,210,212,214,216,218,220,222,224,226,228,230,232Th, 218,220,222,224,226,228,230,232,234,236,238U, 230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 244,246Fm, 252,254,256No, 256,258Rf, 260Sg, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288Fl, 290,292Lv, 294Og, 105,107,109Te, 113I, 109,111Xe, 145Pm, 147Sm, 147Eu, 149,151Gd, 151,153Dy, 151,153Ho, 153,155Er, 153,155,157Tm, 155Yb, 155,157Lu, 157,159,161Hf, 157,159,161Ta, 159,161,163,165,167W, 159,161,163,165Re, 161,163,165,167,169,171,173Os, 165,167,169,171,173Ir, 177Ir, 165,167,169,171,173Pt, 177Pt, 181,183,185Pt, 171,173,175,177,179,181,183,185Au, 173,175Hg, 179Hg, 183Hg, 185Hg, 177,179,181Tl, 185,187,189,191Pb, 185,187,189,191,193,195,197Bi, 191,193,195,197,199,201Po, 205,207,209Po, 213,215,217,219Po, 187Po, 191,193,195,197,199,201,203,205,207,209,211,213,215,217,219At, 195,197,199,201,203,205,207,209Rn, 215,217Rn, 197,199,201,203,205,207,209,211,213,215,217,219Fr, 201,203,205Ra, 209,211Ra, 217Ra, 207,209,211,213,215,217,219,221Ac, 227Ac, 209,211,213Th, 219Th, 211,213,215,217,219,221,223,225,227,229,231Pa, 221U, 229U, 233U, 219Np, 223,225Np, 233Np, 231Pu, 235Pu, 239Pu, 233Cm, 239,241Cf, 245Cf, 253Cf, 241,243,245,247Es, 251,253,255Es, 241Fm, 247Fm, 251No, 253,255Lr, 259Lr, 261Rf, 257Db, 263Sg, 263,265Hs, 267Ds, 148Eu, 152,154Ho, 154,156Tm, 156,158Lu, 158Ta, 162,164Re, 164,166,168,170,172Ir, 170,172,174,176,178Au, 184Au, 188Bi, 196Bi, 192,194,196,198,200,202At, 214,216At, 256,258,260Rf, 260Sg, 262,264Hs, 268,270,272Hs, 266Ds, 270Ds, 276,278Ds, 270Cn, 280,282Cn, 284,286,288Fl, 288,290,292,294,296Lv, 294,296,298,300,302,304Og, 296,298,300,302,304,306,308120, 302,304,306,308,310,312122, 308,310,312,314,316,318124, 314,316,318,320,322,324,326126, 320,322,324,326,328,330,332128(α); calculated T1/2 using the modified Hatsukawa formula. Comparison with available data.
doi: 10.1140/epja/s10050-022-00666-1
2022XU07 Chin.Phys.C 46, 064102 (2022) Y.-P.Xu, D.-Y.Pang, C.-X.Yuan, X.-Y.Yun Quenching of single-particle strengths of carbon isotopes 9-12, 14-20C with knockout reactions for incident energies 43-2100 MeV/nucleon NUCLEAR REACTIONS 9Be, C(9C, 8C), (10C, 9C), (11C, 10C), (12C, 11C), (14C, 13C), (15C, 14C), (16C, 15C), (17C, 16C), (18C, 17C), (19C, 18C), (20C, 19C), E=43-2100 MeV/nucleon; analyzed available data; deduced the quenching of single-particle strengths of carbon isotopes, dependence on the proton-neutron asymmetry.
doi: 10.1088/1674-1137/ac5236
2022XU10 Eur.Phys.J. A 58, 163 (2022) Y.-Y.Xu, D.-X.Zhu, X.Chen, X.-J.Wu, B.He, X.-H.Li A unified formula for α decay half-lives RADIOACTIVITY 109I, 151Eu, 149,151Tb, 155Lu, 157Ta, 169Re, 171,173,175Ir, 175Pt, 179Pt, 185Hg, 171Hg, 177Hg, 181Hg, 181,183Tl, 187Tl, 179,181,183,185,187,189Pb, 187,189Bi, 209,211,213Bi, 211Po, 187,189Po, 203Po, 191,193,195At, 193Rn, 205Rn, 211,213Rn, 219,221Rn, 221,223Fr, 213Ra, 215,217,219,221,223Ra, 207Ra, 223,225Ac, 217Th, 221,223,225,227,229Th, 217Pa, 225Pa, 229Pa, 219U, 223,225,227U, 231U, 227,229,231Np, 235,237Np, 229Pu, 233Pu, 241Pu, 229Am, 233,235,237,239,241,243Am, 235Cm, 241,243,245,247Cm, 245,247,249Bk, 237Cf, 243Cf, 247,249,251Cf, 249Es, 243,245,247Fm, 251,253Fm, 257Fm, 245,247,249,251,253,255,257Md, 253,255,257,259No, 255Lr, 255,257,259,261Rf, 257,259Db, 263Db, 259,261,263,265Sg, 261Bh, 263Hs, 269Hs, 205Ac, 217Ac, 257Lr, 154Ho, 156Lu, 162Ta, 158Ta, 160Re, 168Re, 170,172,174Ir, 180,182,184,186Au, 178Tl, 184,186Tl, 186,188,190,192,194Bi, 212,214Bi, 206At, 210,212At, 218At, 192At, 200At, 198Fr, 212,214Fr, 218,220Fr, 214,216At, 220At, 208At, 222,224,226At, 216,218Pa, 228,230Pa, 224Np, 228,230Np, 236Np, 234Am, 242Am, 242,244,246,248Es, 252,254Es, 244,246Md, 250Md, 256,258Md, 254,256Lr, 256Db, 281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317Ts, 282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318Og, 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319119, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320120, 254No, 256,258Rf(α); calculated T1/2; deduced formula. Comparison with NUBASE2020 values.
doi: 10.1140/epja/s10050-022-00812-9
2022XU13 Chin.Phys.C 46, 114103 (2022) Y.-Y.Xu, D.-X.Zhu, Y.-T.Zou, X.-J.Wu, B.He, X.-H.Li Systematic study on α-decay half-lives of uranium isotopes with a screened electrostatic barrier RADIOACTIVITY 216,217,218U, 221U, 222,223,224,225,226,227,228U, 229U, 230,231,232U, 233U, 234,235,236,237,238,239,240,241,242,243U(α); calculated T1/2 using the Gamow model with a screened electrostatic barrier. Comparison with available data.
doi: 10.1088/1674-1137/ac7fe8
2022XU14 Int.J.Mod.Phys. E31, 2250093 (2022) Y.Xu, X.Su, Y.Han, X.Sun, D.Zhang, C.Cai Optical potential for the elastic scattering of 6Li projectile on 1p-shell nuclei NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 12,13,14C, 15N, 16,18O(6Li, 6Li), E=2-210 MeV; analyzed available data; deduced σ(θ), a set of global optical potential parameters by fitting the experimental data of elastic scattering angular distributions.
doi: 10.1142/S0218301322500938
2022ZH39 Chin.Phys.C 46, 044106 (2022) D.-X.Zhu, H.-M.Liu, Y.-Y.Xu, Y.-T.Zou, X.-J.Wu, P.-C.Chu, X.-H.Li Two-proton radioactivity within Coulomb and proximity potential model RADIOACTIVITY 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); calculated T1/2 using the Coulomb and proximity potential model (CPPM). Comparison with available data.
doi: 10.1088/1674-1137/ac45ef
2021AB12 Phys.Rev. C 104, L061901 (2021) M.S.Abdallah, B.E.Aboona, J.Adam, L.Adamczyk, J.R.Adams, J.K.Adkins, G.Agakishiev, I.Aggarwal, M.M.Aggarwal, Z.Ahammed, I.Alekseev, D.M.Anderson, A.Aparin, E.C.Aschenauer, M.U.Ashraf, F.G.Atetalla, A.Attri, G.S.Averichev, V.Bairathi, W.Baker, J.G.Ball Cap, K.Barish, A.Behera, R.Bellwied, P.Bhagat, A.Bhasin, J.Bielcik, J.Bielcikova, I.G.Bordyuzhin, J.D.Brandenburg, A.V.Brandin, I.Bunzarov, J.Butterworth, X.Z.Cai, H.Caines, M.Calderon de la Barca Sanchez, D.Cebra, I.Chakaberia, P.Chaloupka, B.K.Chan, F.-H.Chang, Z.Chang, N.Chankova-Bunzarova, A.Chatterjee, S.Chattopadhyay, D.Chen, J.Chen, J.H.Chen, X.Chen, Z.Chen, J.Cheng, M.Chevalier, S.Choudhury, W.Christie, X.Chu, H.J.Crawford, M.Csanad, M.Daugherity, T.G.Dedovich, I.M.Deppner, A.A.Derevschikov, A.Dhamija, L.Di Carlo, L.Didenko, P.Dixit, X.Dong, J.L.Drachenberg, E.Duckworth, J.C.Dunlop, N.Elsey, J.Engelage, G.Eppley, S.Esumi, O.Evdokimov, A.Ewigleben, O.Eyser, R.Fatemi, F.M.Fawzi, S.Fazio, P.Federic, J.Fedorisin, C.J.Feng, Y.Feng, P.Filip, E.Finch, Y.Fisyak, A.Francisco, C.Fu, L.Fulek, C.A.Gagliardi, T.Galatyuk, F.Geurts, N.Ghimire, A.Gibson, K.Gopal, X.Gou, D.Grosnick, A.Gupta, W.Guryn, A.I.Hamad, A.Hamed, Y.Han, S.Harabasz, M.D.Harasty, J.W.Harris, H.Harrison, S.He, W.He, X.H.He, Y.He, S.Heppelmann, S.Heppelmann, N.Herrmann, E.Hoffman, L.Holub, Y.Hu, H.Huang, H.Z.Huang, S.L.Huang, T.Huang, X.Huang, Y.Huang, T.J.Humanic, G.Igo, D.Isenhower, W.W.Jacobs, C.Jena, A.Jentsch, Y.Ji, J.Jia, K.Jiang, X.Ju, E.G.Judd, S.Kabana, M.L.Kabir, S.Kagamaster, D.Kalinkin, K.Kang, D.Kapukchyan, K.Kauder, H.W.Ke, D.Keane, A.Kechechyan, M.Kelsey, Y.V.Khyzhniak, D.P.Kikola, C.Kim, B.Kimelman, D.Kincses, I.Kisel, A.Kiselev, A.G.Knospe, H.S.Ko, L.Kochenda, L.K.Kosarzewski, L.Kramarik, P.Kravtsov, L.Kumar, S.Kumar, R.Kunnawalkam Elayavalli, J.H.Kwasizur, R.Lacey, S.Lan, J.M.Landgraf, J.Lauret, A.Lebedev, R.Lednicky, J.H.Lee, Y.H.Leung, C.Li, C.Li, W.Li, X.Li, Y.Li, X.Liang, Y.Liang, R.Licenik, T.Lin, Y.Lin, M.A.Lisa, F.Liu, H.Liu, H.Liu, P.Liu, T.Liu, X.Liu, Y.Liu, Z.Liu, T.Ljubicic, W.J.Llope, R.S.Longacre, E.Loyd, N.S.Lukow, X.F.Luo, L.Ma, R.Ma, Y.G.Ma, N.Magdy, D.Mallick, S.Margetis, C.Markert, H.S.Matis, J.A.Mazer, N.G.Minaev, S.Mioduszewski, B.Mohanty, M.M.Mondal, I.Mooney, D.A.Morozov, A.Mukherjee, M.Nagy, J.D.Nam, Md.Nasim, K.Nayak, D.Neff, J.M.Nelson, D.B.Nemes, M.Nie, G.Nigmatkulov, T.Niida, R.Nishitani, L.V.Nogach, T.Nonaka, A.S.Nunes, G.Odyniec, A.Ogawa, S.Oh, V.A.Okorokov, B.S.Page, R.Pak, J.Pan, A.Pandav, A.K.Pandey, Y.Panebratsev, P.Parfenov, B.Pawlik, D.Pawlowska, H.Pei, C.Perkins, L.Pinsky, R.L.Pinter, J.Pluta, B.R.Pokhrel, G.Ponimatkin, J.Porter, M.Posik, V.Prozorova, N.K.Pruthi, M.Przybycien, J.Putschke, H.Qiu, A.Quintero, C.Racz, S.K.Radhakrishnan, N.Raha, R.L.Ray, R.Reed, H.G.Ritter, M.Robotkova, O.V.Rogachevskiy, J.L.Romero, D.Roy, L.Ruan, J.Rusnak, N.R.Sahoo, H.Sako, S.Salur, J.Sandweiss, S.Sato, W.B.Schmidke, N.Schmitz, B.R.Schweid, F.Seck, J.Seger, M.Sergeeva, R.Seto, P.Seyboth, N.Shah, E.Shahaliev, P.V.Shanmuganathan, M.Shao, T.Shao, A.I.Sheikh, D.Shen, S.S.Shi, Y.Shi, Q.Y.Shou, E.P.Sichtermann, R.Sikora, M.Simko, J.Singh, S.Singha, M.J.Skoby, N.Smirnov, Y.Sohngen, W.Solyst, P.Sorensen, H.M.Spinka, B.Srivastava, T.D.S.Stanislaus, M.Stefaniak, D.J.Stewart, M.Strikhanov, B.Stringfellow, A.A.P.Suaide, M.Sumbera, B.Summa, X.M.Sun, X.Sun, Y.Sun, Y.Sun, B.Surrow, D.N.Svirida, Z.W.Sweger, P.Szymanski, A.H.Tang, Z.Tang, A.Taranenko, T.Tarnowsky, J.H.Thomas, A.R.Timmins, D.Tlusty, T.Todoroki, M.Tokarev, C.A.Tomkiel, S.Trentalange, R.E.Tribble, P.Tribedy, S.K.Tripathy, T.Truhlar, B.A.Trzeciak, O.D.Tsai, Z.Tu, T.Ullrich, D.G.Underwood, I.Upsal, G.Van Buren, J.Vanek, A.N.Vasiliev, I.Vassiliev, V.Verkest, F.Videbaek, S.Vokal, S.A.Voloshin, F.Wang, G.Wang, J.S.Wang, P.Wang, Y.Wang, Y.Wang, Z.Wang, J.C.Webb, P.C.Weidenkaff, L.Wen, G.D.Westfall, H.Wieman, S.W.Wissink, J.Wu, Y.Wu, B.Xi, Z.G.Xiao, G.Xie, W.Xie, H.Xu, N.Xu, Q.H.Xu, Y.Xu, Z.Xu, Z.Xu, C.Yang, Q.Yang, S.Yang, Y.Yang, Z.Ye, Z.Ye, L.Yi, K.Yip, Y.Yu, H.Zbroszczyk, W.Zha, C.Zhang, D.Zhang, J.Zhang, S.Zhang, S.Zhang, X.P.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, Z.J.Zhang, Z.Zhang, Z.Zhang, J.Zhao, C.Zhou, X.Zhu, M.Zurek, M.Zyzak Global Λ-hyperon polarization in Au+Au collisions at √ sNN = 3 GeV
doi: 10.1103/PhysRevC.104.L061901
2021BE28 Phys.Rev. C 104, 044332 (2021) Temperature effects on neutron-capture cross sections and rates through electric dipole transitions in hot nuclei NUCLEAR STRUCTURE 126,128,130,132,134,136,138,140,142,144,146Sn; calculated E1 transition strengths as a function of excitation energy for temperatures T=0 MeV, ratio between neutron-capture rate using relativistic quasiparticle random phase approximation (RQRPA) model, and for T=1 and 2 MeV using self-consistent finite-temperature relativistic random-phase approximation (FTRRPA) model, based on DD-ME2 energy density functional. 126,136,146Sn; calculated transition densities of neutrons and protons for the low-lying peaks at T=0 for 8.33-MeV peak in 126Sn, 6.04- and 8.28-MeV peaks in 136Sn, and 5.11- and 7.54-MeV peaks in 146Sn using RQRPA model based on DD-ME2 energy density functional, main single-particle transition configurations for selected low-lying dipole states, E1 transition strength as function of excitation energy. Self-consistent QRPA and finite-temperature RPA model based on relativistic energy density functionals.
doi: 10.1103/PhysRevC.104.044332
2021KE02 Nucl.Phys. A1005, 122039 (2021) Quantifying heavy quark transport coefficients with an improved transport model
doi: 10.1016/j.nuclphysa.2020.122039
2021SU05 Nucl.Sci.Eng. 195, 239 (2021) Calculations and Evaluations of the n + 48Ti Reaction Below 200 MeV NUCLEAR REACTIONS 48Ti(n, X), (n, n), (n, n'), E<200 MeV; analyzed available data; calculated σ, σ(θ). Comparison with the EXFOR library.
doi: 10.1080/00295639.2020.1808388
2021XU04 Phys.Rev. C 104, 044301 (2021) Systematical studies of the E1 photon strength functions combining the Skyrme-Hartree-Fock-Bogoliubov plus quasiparticle random-phase approximation model and experimental giant dipole resonance properties NUCLEAR STRUCTURE 70,72,74Ge, 80,82Se, 89Y, 90,91,92,94Zr, 93Nb, 96,100Mo, 103Rh, 107Ag, 115In, 119,120,124Sn, 124,126,128Te, 127I, 128,134Xe, 133Ce, 138Ba, 140Ce, 141Pr, 143,145,146Nd, 144,150Sm, 165Ho, 181Ta, 188Os, 197Au, 206,208Pb, 209Bi, 239Pu; calculated E1 photon strength function using BSk27+QRPA, and compared with extracted strength from experimental photoabsorption cross sections. A=70-190; calculated parameters of giant-dipole resonances (GDR) using BSk27+QRPA, and compared with compiled in the RIPL-3 database. A=25-250; calculated E1 strength functions and compared with compiled data in RIPL3 for 60 nuclei from 25Mg to 239U, and comparison between ARC E1 strength function for 25 nuclei from 96Mo to 240Pu. 115,120,125,130,135,140,145,150,155Sn; calculated E1 photon strength functions from empirical Lorentzian model SMLO, D1M+QRPA, BSk7+QRPA, and the present BSk27+QRPA. 115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155Sn; calculated neutron capture reaction rates at the temperature of T9=1 using present BSk27+QRPA model and compared with those from BSk7+QRPA, D1M+QRPA, SMLO. Z=1-110, N=0-255; calculated neutron capture reaction rates at T9=1 present BSk27+QRPA model and compared with those from previous D1M+QRPA model. 43,44Sc, 44,45Ti; calculated temperature-dependent E1 strength functions using present BSk27+QRPA, and compared with shell-model calculationsSystematic investigation of E1 photon strength functions for about 10, 000 nuclei with Z=8-124 lying between the proton and neutron drip lines by combining simultaneously microscopic Hartree-Fock-Bogoliubov plus quasiparticle random-phase approximation (HFB+QRPA) model and the constraints from available experimental results for photon strength functions from giant dipole resonance (GDR) data, and other types of experiments. Relevance to future measurement of the photonuclear excitation using the Extreme Light Infrastructure (ELI-NP) facilities, and to improve study of r and p nucleosynthesis processes.
doi: 10.1103/PhysRevC.104.044301
2021XU07 Chin.Phys.C 45, 114103 (2021) Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai Description of elastic scattering induced by the unstable nuclei 9, 10, 11, 13, 14C NUCLEAR REACTIONS 208Pb(9C, 9C), (11C, 11C), E=222-227 MeV; 27Al, 58Ni, 208Pb(10C, 10C), E=29.1-256 MeV; 28Si, 208Pb(9C, 9C), E<500 MeV; 28Si, 208Pb(11C, 11C), E<500 MeV; 28Si(13C, 13C), E=25-60 MeV; 40Ca, 56Fe, 60Ni, 66Zn, 88Sr(14C, 14C), E=51 MeV; 92,100Mo(14C, 14C), E=71 MeV; 28Si(14C, 14C), E<500 MeV; analyzed available data; deduced σ, σ(θ), global optical model potentials.
doi: 10.1088/1674-1137/ac1fe1
2021YA04 Nucl.Phys. A1005, 121854 (2021) X.Yao, W.Ke, Y.Xu, S.A.Bass, T.Mehen, B.Muller Quarkonium Production in Heavy Ion Collisions: From Open Quantum System to Transport Equation
doi: 10.1016/j.nuclphysa.2020.121854
2020MU07 Phys.Rev. C 101, 055801 (2020) M.Munch, C.Matei, S.D.Pain, M.T.Febbraro, K.A.Chipps, H.J.Karwowski, C.Aa.Diget, A.Pappalardo, S.Chesnevskaya, G.L.Guardo, D.Walter, D.L.Balabanski, F.D.Becchetti, C.R.Brune, K.Y.Chae, J.Frost-Schenk, M.J.Kim, M.S.Kwag, M.La Cognata, D.Lattuada, R.G.Pizzone, G.G.Rapisarda, G.V.Turturica, C.A.Ur, Y.Xu Measurement of the 7Li(γ, t)4He ground-state cross section between Eγ = 4.4. and 10 MeV NUCLEAR REACTIONS 7Li(γ, t), E=4.4-10 MeV from High Intensity Gamma-ray Source (HIγS) at TUNL; measured E(t), I(t), Eα, Iα, Eγ and Iγ, αt-coin, ground state σ(E) using the SIDAR silicon detector array. 3H(α, γ), E(cm)=0-7 MeV; deduced astrophysical S-factor from R-matrix analysis. Comparison with model predictions, and with previous experimental results. Relevance to primordial Li problem and the mirror α-capture reactions.
doi: 10.1103/PhysRevC.101.055801
2020SO09 Phys.Rev. C 101, 044903 (2020) Ta.Song, P.Moreau, Y.Xu, V.Ozvenchuk, E.Bratkovskaya, J.Aichelin, S.A.Bass, P.B.Gossiaux, M.Nahrgang Traces of nonequilibrium effects, initial condition, bulk dynamics, and elementary collisions in the charm observables
doi: 10.1103/PhysRevC.101.044903
2020XU03 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 12C, 27Al, 28Si, 58Ni, 208Pb(8B, 8B), 9Be, 12C, 16O, 28Si, 58Ni, 120Sn, 208Pb(10B, 10B), 12C, 28Si, 58Ni, 208Pb, 209Bi(11B, 11B), E<50 MeV; analyzed available data. 8,10,11B; calculated σ; deduced global phenomenological optical model potentials.
doi: 10.1088/1674-1137/44/3/034101
2020XU04 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 27Al, 58Ni, 208Pb, 12C, 28Si(8B, 8B), E<100 MeV; 27Al, 28Si, 58Ni, 120Sn, 16O, 9Be, 208Pb(10B, 10B), E<100 MeV; 28Si, 58Ni, 209Bi, 12C, 209Bi(11B, 11B), E<100 MeV; analyzed available data. 9Be; deduced optical model potential parameters, σ, σ(θ).
doi: 10.1088/1674-1137/44/3/034101
2020XU07 J.Phys.(London) G47, 085105 (2020) Y.-G.Xu, X.-D.Cheng, J.-L.Zhang, R.-M.Wang Studying two-body nonleptonic weak decays of hyperons with topological diagram approach
doi: 10.1088/1361-6471/ab97c7
2020XU10 Chin.Phys.C 44, 124103 (2020) Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai Global optical model potential describing 12C-nucleus elastic scattering NUCLEAR REACTIONS 24Mg, 28Si, 32S, 39K, 40,42,48Ca, 50Cr, 56Fe, Fe, 58,64Ni, Ni, 90,91,92,94,96Zr, 92Mo, 116,117,118,119,120,122,124Sn, 194,198Pt, 208Pb, 209Bi(12C, 12C), E<200 MeV; analyzed available data; deduced a new global optical model potential parameters.
doi: 10.1088/1674-1137/abb4d0
2020ZH02 Phys.Lett. B 801, 135170 (2020), Corrigendum Phys.Lett. B 803, 135278 (2020) N.T.Zhang, X.Y.Wang, D.Tudor, B.Bucher, I.Burducea, H.Chen, Z.J.Chen, D.Chesneanu, A.I.Chilug, L.R.Gasques, D.G.Ghita, C.Gomoiu, K.Hagino, S.Kubono, Y.J.Li, C.J.Lin, W.P.Lin, R.Margineanu, A.Pantelica, I.C.Stefanescu, M.Straticiuc, X.D.Tang, L.Trache, A.S.Umar, W.Y.Xin, S.W.Xu, Y.Xu Constraining the 12C+12C astrophysical S-factors with the 12C+13C measurements at very low energies NUCLEAR REACTIONS 12C(13C, p)24Na, E=4.640-10.995 MeV; measured reaction products, Eγ, Iγ; deduced σ, branching ratio, S-factor.
doi: 10.1016/j.physletb.2019.135170
2019CA14 Phys.Rev. C 99, 054907 (2019) S.Cao, G.Coci, S.K.Das, W.Ke, S.Y.F.Liu, S.Plumari, T.Song, Y.Xu, J.Aichelin, S.Bass, E.Bratkovskaya, X.Dong, P.B.Gossiaux, V.Greco, M.He, M.Nahrgang, R.Rapp, F.Scardina, X.-N.Wang Toward the determination of heavy-quark transport coefficients in quark-gluon plasma
doi: 10.1103/PhysRevC.99.054907
2019KE08 Phys.Rev. C 100, 064911 (2019) Modified Boltzmann approach for modeling the splitting vertices induced by the hot QCD medium in the deep Landau-Pomeranchuk-Migdal region
doi: 10.1103/PhysRevC.100.064911
2019SU03 Phys.Rev. C 99, 024605 (2019) Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, B.H.Sun, J.W.Zhao, Y.P.Xu, D.Y.Pang, Y.H.Yu, K.Yue, S.W.Tang, C.Dong, Y.X.Zhao, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, P.Ma, H.R.Yang, C.G.Lu, L.M.Duan Two-neutron removal cross sections from 15, 16C at around 240 MeV/nucleon NUCLEAR REACTIONS 12C(15C, X), (15C, 13C), (16C, X), (16C, 14C)8Li/10Be/11Be/12B/13B/15C/16C/17N, E=237, 239 MeV/nucleon, [secondary 15,16C beams from 9Be(18O, X), E=280 MeV/nucleon primary reaction followed by in-flight fragment separator RIBLL2 at HIRFL-Lanzhou]; measured reaction products, particle identification spectra, time of flight of fragments, and two-neutron removal σ(E) using multiwire drift chambers for particle detection and identification, and plastic scintillators for time of flight measurements. Comparison with previous experimental values, and theoretical calculations for two-neutron removal σ based on eikonal-model and shell-model structure information. Systematics of odd-even staggering in two-neutron removal σ from 15,16,17,18,19,20C projectiles.
doi: 10.1103/PhysRevC.99.024605
2019WA01 Phys.Scr. 94, 015302 (2019) Energy dependence of the reduced single-particle strength for strongly-bound proton removal on 16C NUCLEAR REACTIONS 12C(16C, 15B), E=400 MeV/nucleon; analyzed available data; deduced reduction factors of the one-proton σ.
doi: 10.1088/1402-4896/aaed64
2019XU02 Phys.Rev. C 99, 014902 (2019) Y.Xu, S.A.Bass, P.Moreau, T.Song, M.Nahrgang, E.Bratkovskaya, P.Gossiaux, J.Aichelin, S.Cao, V.Greco, G.Coci, K.Werner Resolving discrepancies in the estimation of heavy quark transport coefficients in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.99.014902
2019XU05 Phys.Rev. C 99, 034618 (2019) Y.Xu, Y.Han, H.Liang, Z.Wu, H.Guo, C.Cai Global optical model potential for the weakly bound projectile 9Be NUCLEAR REACTIONS Mg(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 27Al(9Be, 9Be), E=12.0, 14.0, 18.0, 20.0, 22.0, 25.0, 28.0, 32.0, 33.0, 35.0.40.0, 47.5 MeV; 28Si(9Be, 9Be), E=12.0, 13.0, 14.0, 17.0, 20.0, 23.0, 26.0, 30.0, 45.0, 50.0, 60.0 MeV; 40Ca(9Be, 9Be), E=14.0, 20.0, 26.0, 45.0.50.0, 60.0 MeV; 58Ni(9Be, 9Be), E=20.0, 26.0 MeV; 64Zn(9Be, 9Be), E=17.0, 19.0, 21.0, 23.0, 26.0, 28.0, 28.4, 28.97 MeV; 89Y(9Be, 9Be), E=18.6, 20.6, 22.7, 24.7, 26.7, 28.7, 33.2 MeV; Ag(9Be, 9Be), E=26.0 MeV; 144Sm(9Be, 9Be), E=30.0, 31.5, 33.0, 34.0, 35.0, 37.0, 39.0, 41.0, 44.0, 48.0 MeV; 208Pb(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 9.5, 40.0, 41.0, 42.0, 44.0, 46.0, 47.2, 48.0, 50.0, 60.0, 68.0, 75.0 MeV; 209Bi(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 39.5, 40.0, 41.0, 42.0, 44.0, 46.0, 48.0 MeV; analyzed elastic σ(θ, E) data for global phenomenological energy-dependent optical model potential parameters for 9Be. 9Be, 12,13C, 27Al, 64Zn, 89Y, 144Sm(9Be, X), E=10-300 MeV; 28Si, Cu(9Be, X), E=10-500 MeV; 89Y(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (9Be, X), (11B, X); calculated reaction σ(E) using optical model and compared with experimental data. 9Be(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 12C(9Be, 9Be), E=13.0, 14.0, 14.5, 17.3, 19.0, 20.0, 21.0, 26.0, 153.8 MeV; 13C(9Be, 9Be), E=19.46, 25.05 MeV; 16O(9Be, 9Be), E=20.0, 25.94 MeV; calculated elastic σ(θ, E) using optical model parameters and compared with experimental data.
doi: 10.1103/PhysRevC.99.034618
2019YA01 Nucl.Phys. A982, 755c (2019) X.Yao, W.Ke, Y.Xu, S.Bass, B.Muller Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations
doi: 10.1016/j.nuclphysa.2018.10.005
2018HE01 Chin.Phys.C 42, 015001 (2018) J.-J.He, I.Lombardo, D.Dell'Aquila, Y.Xu, L.-Y.Zhang, W.-P.Liu Thermonuclear 19F(p, α0)16O reaction rate NUCLEAR REACTIONS 19F(p, α), E<1 MeV; analyzed available data; deduced reaction rate, σ, σ(θ), S-factor using theoretical R-matrix extrapolations.
doi: 10.1088/1674-1137/42/1/015001
2018HU09 Nucl.Sci.Eng. 191, 262 (2018) Calculation and Evaluations for n+64, 66, 67, 68, 70, natZn Reactions NUCLEAR REACTIONS 64,66,67,68,70Zn, Zn(n, X), E<200 MeV; calculated σ(θ), σ(E), σ(θ, E). Comparison with experimental data, JEFF-3.2 and JENDL-4.0 evaluated nuclear data libraries.
doi: 10.1080/00295639.2018.1469334
2018KE05 Phys.Rev. C 98, 064901 (2018) Linearized Boltzmann-Langevin model for heavy quark transport in hot and dense QCD matter
doi: 10.1103/PhysRevC.98.064901
2018LA06 Astrophys.J. 859, 62 (2018) R.Lau, M.Beard, S.S.Gupta, H.Schatz, A.V.Afanasjev, E.F.Brown, A.Deibel, L.R.Gasques, G.W.Hitt, W.R.Hix, L.Keek, P.Moller, P.S.Shternin, A.W.Steiner, M.Wiescher, Y.Xu Nuclear Reactions in the Crusts of Accreting Neutron Stars
doi: 10.3847/1538-4357/aabfe0
2018LA14 Phys.Rev. C 98, 054601 (2018) H.Y.Lan, Y.Xu, W.Luo, D.L.Balabanski, S.Goriely, M.La Cognata, C.Matei, A.Anzalone, S.Chesnevskaya, G.L.Guardo, D.Lattuada, R.G.Pizzone, S.Romano, C.Spitaleri, A.Taffara, A.Tumino, Z.C.Zhu Determination of the photodisintegration reaction rates involving charged particles: Systematic calculations and proposed measurements based on the facility for Extreme Light Infrastructure--Nuclear Physics NUCLEAR REACTIONS 74Se, 84Sr, 92Mo, 96Ru, 102Pd, 106Cd, 112Sn, 120Te(γ, p), E(cm)=8-20 MeV; 74Se, 84Sr, 92Mo, 96Ru, 102Pd, 106Cd, 112Sn, 120Te, 132Ba, 144Sm, 148Gd, 184Os(γ, α), E(cm)=6-20 MeV; calculated σ(E), proton and α-particle spectra and yields, Gamow windows at T9=2.5 and minimum required energies of the incident γ beam satisfying the measurable criteria of the minimum detectable limit and the particle identification. Z=10-100, N=10-160; calculated ratios of the (γ, p) and (γ, α) astrophysical reaction rates at T9=2.5 for 3000 targets of stable and proton-rich nuclei. Optical potential model calculations using Woods-Saxon and microscopic folding JLMB optical model potentials. Relevance to p-process nucleosynthesis, and the measurements of six (γ, p) and eight (γ, α) reactions based on the γ-beam facility and the Extreme Light Infrastructure Silicon Strip Array (ELISSA) for the detection of charged particles at ELI-NP, Bucharest facility.
doi: 10.1103/PhysRevC.98.054601
2018XU01 Phys.Rev. C 97, 014615 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai Global phenomenological optical model potential for the 7Li projectile nucleus NUCLEAR REACTIONS 9Be(7Li, 7Li), E=15.75, 24.0, 30.0, 63.0, 130.0 MeV; 12C(7Li, 7Li), E=7.5, 9.0, 12.0, 15.0, 36.0, 131.8 MeV; 16O(7Li, 7Li), E=26.0, 36.0, 42.0, 50.0 MeV; 11B, 12,13C, 24Mg(7Li, 7Li), E=34.0 MeV; 24,26Mg(7Li, 7Li), E=88.7 MeV; 27Al(7Li, 7Li), E=6.0, 7.0, 8.0, 9.0, 10.0, 11.0, 12.0, 13.0, 14.0, 16.0, 18.0, 19.0, 24.0 MeV; 28Si(7Li, 7Li), E=8.0, 8.5, 9.0, 10.0, 11.0, 11.5, 13.0, 15.0, 16.0, 21.0, 26.0, 36.0, 177.8 MeV; 40,44,48Ca(7Li, 7Li), E=34.0; 40Ca(7Li, 7Li), E=88.7 MeV; 46,48Ti(7Li, 7Li), E=17.0 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe, 65Cu, 90Zr(7Li, 7Li), E=34.0 MeV; 58Ni(7Li, 7Li), E=14.22, 16.25.18.28, 19.0, 20.31.34.0, 42.0 MeV; 60,62Ni, 64,68Zn(7Li, 7Li), E=34.0 MeV; 80Se(7Li, 7Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 23.0, 26.0 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 116Sn(7Li, 7Li), E=18.0, 19.0, 20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0 MeV; 120Sn(7Li, 7Li), E=19.5, 20.0, 20.5, 22.0, 24.0, 25.0, 26.0, 28.0, 30.044.0 MeV; 138Ba(7Li, 7Li), E=21.0, 22.0, 23.0, 24.0, 28.0, 30.0, 32.0, 52.0 MeV; 140Ce, 142Nd(7Li, 7Li), E=52.0 MeV; 144Sm(7Li, 7Li), E=21.6, 22.1, 22.6.23.0, 25.0, 27.0, 29.0, 30.0, 32.0, 35.0, 40.8, 52.0 MeV; 208Pb(7Li, 7Li), E=27.0, 29.0, 33.0, 39.0, 42.0, 52.0 MeV; 232Th(7Li, 7Li), E=24.0, 26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed σ(θ, E) experimental data by global phenomenological optical model potential. 13C, 27Al, 64Zn, 116Sn, 138Ba, (7Li, X), E<300 MeV; 28Si, Cu, 208Pb(7Li, X), E<400 MeV; calculated reaction σ(E) using optical model, and compared with experimental data.
doi: 10.1103/PhysRevC.97.014615
2018XU02 Phys.Rev. C 97, 014907 (2018) Yi.Xu, J.E.Bernhard, S.A.Bass, M.Nahrgang, S.Cao Data-driven analysis for the temperature and momentum dependence of the heavy-quark diffusion coefficient in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.97.014907
2018XU03 Int.J.Mod.Phys. E27, 1850023 (2018) The proton microscopic optical potential based on Skyrme interaction NUCLEAR REACTIONS 54,56Fe, 51V, 40Ca, 28Si, 27Al, 59Co, 58,60Ni, 63Cu, 90Zr, 120Sn, 208Pb, 232Th, 238U(p, p), E<100 MeV; calculated σ, σ(θ). Comparison with available data.
doi: 10.1142/S0218301318500234
2018XU10 Phys.Rev. C 98, 024619 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai 6Li global phenomenological optical model potential NUCLEAR REACTIONS 24Mg, 48Ca(6Li, 6Li), E=240.0 MeV; 25,26Mg, 39K, 91Zr(6Li, 6Li), E=34.0 MeV; 27Al(6Li, 6Li), E=7.0, 8.0, 10.0, 12.0, 18.0, 34.0 MeV; 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 16.0, 20.0, 21.0, 25.0, 27.0, 34.0, 46.0, 99.0, 135.0, 154.0, 210.0, 240.0, 318.0, 350.0 MeV; 40Ca(6Li, 6Li), E=50.6, 99.0, 156.0, 210.0, 240.0 MeV; 54Fe(6Li, 6Li), E=38.0, 44.0, 50.0 MeV; 59Co(6Li, 6Li), E=12.0, 18.0, 26.0, 30.0 MeV; 58Ni(6Li, 6Li), E=9.85, 11.21, 12.13, 13.04, 14.04, 34.0, 50.6, 73.7, 90.0, 99.0, 210.0, 240.0 MeV; 65Cu(6Li, 6Li), E=25.0 MeV; 64Zn(6Li, 6Li), E=10.77, 11.69, 12.0, 12.43, 13.0, 13.54, 13.8, 14.92, 15.0, 16.30, 16.5, 18.0, 18.14, 19.98, 22.0 MeV; 72,74,76Ge(6Li, 6Li), E=28.0 MeV; 80Se(6Li, 6Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 22.19, 23.0, 26.0 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=11.0, 12.0, 13.0, 15.0, 17.0, 19.0, 21.0, 25.0, 30.0, 34.0, 60.0, 70.0, 73.7, 99.0, 156.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 112Sn(6Li, 6Li), E=21.0, 22.0, 23.0, 25.0, 30.0, 35.0 MeV; 116Sn(6Li, 6Li), E=20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0, 40.0 MeV; 118Sn(6Li, 6Li), E=42.0 MeV; 120Sn(6Li, 6Li), E=30.0, 44.0, 90.0 MeV; 124Sn(6Li, 6Li), E=73.7 MeV; 138Ba(6Li, 6Li), E=21.0, 22.0, 23.0, 24.0, 26.0, 28.0 MeV; 144Sm(6Li, 6Li), E=21.0, 22.1, 22.6, 24.1, 26.0, 28.0, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25.0, 29.0, 31.0, 33.0, 35.0, 36.0, 37.0, 39.0, 42.0, 43.0, 46.0, 48.0, 50.6, 73.7, 88.0, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=24.0, 26.0, 28.0, 29.9, 30.0, 32.0, 32.8, 34.0, 36.0, 40.0, 44.0, 50.0 MeV; 232Th(6Li, 6Li), E=26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed differential σ(θ, E) data; deduced a new set of 6Li global phenomenological energy-dependent optical potential parameters based on the form of the Woods-Saxon potential within the optical model. 63,65Cu, 64Zn, 112,116Sn, 138Ba, 208Pb(6Li, X), E<400 MeV; calculated reaction σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.98.024619
2018XU11 Phys.Rev. C 98, 044622 (2018) Y.P.Xu, D.Y.Pang, X.Y.Yun, S.Kubono, C.A.Bertulani, C.X.Yuan Possible determination of high-lying single-particle components with (d, p) reactions NUCLEAR REACTIONS 12C, 24Mg, 28Si, 40Ca(d, p), E=51.93 MeV; analyzed experimental σ(θ) distributions, spectroscopic amplitudes for neutrons in normal and high-lying single-particle components in the ground and excited states by fitting the angular distributions of the ground and the j-forbidden excited states simultaneously, effects of one-step transfer (OST), two-step transfer (TST) and inelastic excitation processes in neutron pickup reactions. Coupled reaction channel calculations.
doi: 10.1103/PhysRevC.98.044622
2018XU12 Int.J.Mod.Phys. E27, 1850099 (2018) Y.-Li.Xu, H.-R.Guo, Y.-L.Han, Q.-B.Shen Global phenomenological optical model potentials for 8, 10, 11B projectiles NUCLEAR REACTIONS 28,30Si, 40Ca, 58Ni, 208Pb, 209Bi(11B, 11B), E<100 MeV; 7Li, 9Be, 12C, 28Si, 58Ni, 208Pb(8B, 8B), E < 100 MeV; 16O, 28Si, 120Sn, 208Pb, 232Th(10B, 10B), E<100 MeV; analyzed available data for 11B; deduced global phenomenological optical model potential for 11B, calculated σ.
doi: 10.1142/S0218301318500994
2017GU06 Phys.Rev. C 95, 034614 (2017) H.Guo, H.Liang, Y.Xu, Y.Han, Q.Shen, C.Cai, T.Ye Microscopic optical potential for 6He NUCLEAR REACTIONS 12C(6He, 6He), E=8.79, 9.18, 9.9, 18, 230, 250 MeV; 27Al(6He, 6He), E=9.54, 11.0, 12.0, 13.4 MeV; 51V(6He, 6He), E=15.4, 23.0 MeV; 58Ni(6He, 6He), E=9.0, 10.0, 12.2, 16.5, 21.7 MeV; 64Zn(6He, 6He), E=10.0, 13.6 MeV; 65Cu(6He, 6He), E=19.56, 22.6, 30.05 MeV; 120Sn(6He, 6He), E=17.4, 18.05, 19.8, 20.05 MeV; 197Au(6He, 6He), E=10.1, 27.0 MeV; 209Bi(6He, 6He), E=14.71, 16.26, 17.8, 19.0, 19.14, 22.02, 22.5 MeV; 208Pb(6He, 6He), E=14.0, 16, 18, 22, 27, 56.6 MeV; 9Be(6He, 6He), E=16.2, 16.8, 21.3, 150 MeV; calculated differential σ(θ, E) relative to Rutherford cross section using microscopic optical potential (MOP) and global phenomenological 6He optical potential (GOP) based on experimental data. 28Si(6He, X), E<330 MeV; calculated total σ(E) using MOP and GOP. Comparison with experimental data. Isospin-dependent nucleon microscopic optical potential derived by using Green's function method through the nuclear matter approximation and the local density approximation based on the Skyrme nucleon-nucleon effective interaction.
doi: 10.1103/PhysRevC.95.034614
2017GU11 Nucl.Sci.Eng. 186, 156 (2017) H.Guo, Y.Xu, Y.Han, Q.Shen, T.Ye, W.Sun Calculation and Evaluation for the n+51V Reaction NUCLEAR REACTIONS 51V(n, n), E<300 MeV; calculated σ, σ(E), σ(θ), σ(θ, E). Optical model, distorted wave Born approximation theory, Hauser-Feshbach theory, evaporation model, exciton model, and intranuclear cascade model, comparison with the experimental data and the evaluated results in ENDF/B-VII.1 and JENDL-4 libraries.
doi: 10.1080/00295639.2016.1273008
2017HE19 Phys.Rev. C 96, 045801 (2017) J.J.He, A.Parikh, Y.Xu, Y.H.Zhang, X.H.Zhou, H.S.Xu Thermonuclear 46Cr (p, γ) 47Mn rate in type-I x-ray bursts NUCLEAR REACTIONS 46Cr(p, γ)47Mn, T9=0.01-2.0; analyzed astrophysical thermonuclear reaction rates, and proton resonances in 47Mn using known structure information and parameters in the ENSDF database for the mirror nucleus 47Ti. Comparison with previous statistical model and shell-model calculations. Pointed out need for experimental studies of the level structure of 47Mn near the proton threshold to improve model predictions. Relevance to Type-I x-ray bursts (XRBs).
doi: 10.1103/PhysRevC.96.045801
2017WE03 Chin.Phys.C 41, 054104 (2017) C.Wen, Y-P.Xu, D.-Y.Pang, Y.-L.Ye Quenching of neutron spectroscopic factors of radioactive carbon isotopes with knockout reactions within a wide energy range NUCLEAR REACTIONS C(15C, X), E=54, 62 MeV; Be(15C, X), E=103, 700 MeV; C(16C, X), E=55, 83 MeV; Be(16C, X), E=62, 700 MeV; C(17C, X), E=49, 79, 904 MeV; Be(17C, X), E=62, 700 MeV; C(18C, X), E=43, 80 MeV; Be(18C, X), E=700 MeV; C(19C, X), E=243, 910 MeV; Be(19C, X), E=57, 64, 88, 700 MeV; analyzed available data; deduced quenching factors of one-neutron spectroscopic factors. Comparison with systematics.
doi: 10.1088/1674-1137/41/5/054104
2017XU05 Phys.Rev. C 96, 024621 (2017) New extended Skyrme interaction for nuclear properties and nuclear reactions NUCLEAR STRUCTURE 16O, 40,48Ca, 56,60Ni, 88Sr, 90Zr, 114Sn, 146Gd, 204Hg, 206,208Pb; calculated relative deviations of charge radii and energies per nucleon using SkC17, SkC, and GS2 Skyrme interactions. 208Pb; calculated neutron and proton single-particle energy levels near the Fermi surface using various Skyrme interactions, and compared with experimental data. NUCLEAR REACTIONS 56Fe, 208Pb(n, X), E=0.1-100 MeV; calculated total and non-elastic σ(E) using SkC17, SkC, GS2, and SkOP4 Skyrme interactions, and compared with experimental data. 24Mg, 54,58Fe, 59Co, 90Zr, 93Nb, 92,96,98,100Mo, 120Sn, 206,208Pb(n, n), E=11.0 MeV; 28Si, 40Ca, 56Fe, 90Zr, 120Sn, 208Pb(n, n), E=65.0 MeV; 56Fe, 208Pb(n, n), E=1.68-96.0 MeV; 100Mo(n, n), E=0.34-26.0 MeV; 12C(n, n), E=0.5-94.8 MeV; 238U(n, n), E=4.5=10 MeV; 181Ta(n, n), E=0.32-15.2 MeV; 54Fe(polarized n, n), E=9.94, 13.92, 16.93 MeV; 89Y(polarized n, n), E=9.95, 13.93, 16.93 MeV; 208Pb(polarized n, n), E=5.97, 6.97, 7.96, 8.96, 9.95, 13.9, 23.0 MeV;calculated σ(θ, E), analyzing powers using different Skyrme interaction parameters; deduced SkC17 Skyrme interaction by simultaneously fitting variety of experimental data. Extended Skyrme interaction involving additional momentum- and density-dependent terms.
doi: 10.1103/PhysRevC.96.024621
2017XU06 Phys.Rev. C 96, 024902 (2017) Y.Xu, P.Moreau, T.Song, M.Nahrgang, S.A.Bass, E.Bratkovskaya Traces of nonequilibrium dynamics in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.96.024902
2017XU08 Nucl.Phys. A967, 668 (2017) Y.Xu, M.Nahrgang, J.E.Bernhard, S.Cao, S.A.Bass A data-driven analysis of the heavy quark transport coefficient
doi: 10.1016/j.nuclphysa.2017.05.035
2017XU09 Int.J.Mod.Phys. E26, 1750065 (2017) Isospin dependence of the nucleon density distributions NUCLEAR STRUCTURE 40,48Ca, 124Sn, 208Pb; calculated proton density distributions, rms radii. Comparison with available data.
doi: 10.1142/S0218301317500653
2016MA82 Nuovo Cim. C 39, 360 (2016) C.Matei, D.L.Balabanski, O.Tesileanu, Y.Xu, M.La Cognata, C.Spitaleri Nuclear astrophysics measurements with ELISSA at ELI-NP NUCLEAR REACTIONS 3H(α, γ), E(cm)<9 MeV; Calculated S-factor. Comparison with available data.
doi: 10.1393/ncc/i2016-16360-4
2016XU02 Int.J.Mod.Phys. E25, 1650013 (2016) Y.-L.Xu, H.-R.Guo, Y.-L.Han, Q.-B.Shen The neutron microscopic optical potential based on skyrme interaction NUCLEAR REACTIONS 24Mg, 54,56Fe, 59Co, 90Zr, 93Nb, 92,96,98,100Mo, 120Sn, 206,208Pb(n, n), E=11 MeV; 12C, 16O, 23Na, 14N, 232Th, 235,238U, 239Pu(n, X), E=0.1-100 MeV; calculated σ(θ), σ. Comparison with experimental data.
doi: 10.1142/S0218301316500130
2016XU05 Astrophys.J. 827, 17 (2016) Y.Xu, B.Xiong, Y.C.Chang, C.Y.Ng Absolute Integral Cross Sections for the State-selected Ion-Molecule Reaction N+2(X2Σg+; ν+ = 0-2) + C2H2 in the Collision Energy Range of 0.03-10.00 eV NUCLEAR REACTIONS C, H(14N, p), (14N, E), E=0.03-10.00 eV; measured reaction products; deduced integral σ for charge and hydrogen-atom transfers.
doi: 10.3847/0004-637X/827/1/17
2015DE34 Phys.Part. and Nucl.Lett. 12, 703 (2015) A.S.Denikin, S.M.Lukyanov, N.K.Skobelev, Yu.G.Sobolev, E.I.Voskoboynik, Yu.E.Penionzhkevich, W.H.Trzaska, G.P.Tyurin, V.Burjan, V.Kroha, J.Mrazek, S.Piskor, V.Glagolev, Y.Xu, S.V.Khlebnikov, M.N.Harakeh, K.A.Kuterbekov, Yu.Tuleushev Inelastic scattering and clusters transfer in 3, 4He + 9Be reactions NUCLEAR REACTIONS 9Be(α, α), (α, α'), (α, 3He), (α, t), (3He, 6Li), (3He, 6Be), E ∼ 50 MeV; measured reaction products, spectra of total energies; deduced σ(θ), optical potential parameters. Comparison with DWBA calculations.
doi: 10.1134/S1547477115050052
2015HE25 Nucl.Instrum.Methods Phys.Res. B361, 517 (2015) M.He, Y.Xu, Y.Guan, H.Shen, L.Du, C.Hongtao, K.Dong, S.Jiang, X.Yang, X.Wang, X.d.Ruan, J.Liu, S.Wu, Q.Zhao, L.Cai, F.Pang Determination of cross sections of 60Ni(n, 2n)59Ni induced by 14 MeV neutrons with accelerator mass spectrometry NUCLEAR REACTIONS 60Ni(n, 2n), E≈14 MeV; measured reaction products; deduced σ. Comparison with ENDF/B-VII.0 and JENDL-3.3 evaluated nuclear libraries.
doi: 10.1016/j.nimb.2015.01.060
2015XU04 Int.J.Mod.Phys. E24, 1550005 (2015) Y.-L.Xu, H.-R.Guo, Y.-L.Han, Q.-B.Shen Applicability of the systematic helium-3 potential for triton-nucleus reactions NUCLEAR REACTIONS 28Si, 58Ni, 116Sn, 208Pb(t, t), (3He, 3He), E<60 MeV/nucleon; calculated σ; deduced optical model potential parameters. Comparison with available data.
doi: 10.1142/S0218301315500056
2015ZH41 Phys.Rev. C 92, 054616 (2015) Q.Z.Zhao, X.M.Wang, W.Wang, M.He, K.J.Dong, C.J.Xiao, X.D.Ruan, H.T.Shen, S.Y.Wu, X.R.Yang, L.Dou, Y.N.Xu, L.Cai, F.F.Pang, H.Zhang, Y.J.Pang, S.Jiang Determination of the α-decay half-life of 210Po based on film and slice bismuth samples at room temperature RADIOACTIVITY 210Po(α)[from 209Po(n, γ), E=thermal]; measured Eα, Iα, T1/2 for a film sample of Bi2O3 and slice sample of Bi metal; deduced no difference in T1/2 using samples with two different physical configurations. Comparison with the recommended value in the ENSDF database.
doi: 10.1103/PhysRevC.92.054616
2014GU01 Nucl.Phys. A922, 84 (2014) H.Guo, Y.Xu, H.Liang, Y.Han, Q.Shen Microscopic optical model potential for triton NUCLEAR REACTIONS A=6-232(t, t), (t, X), E=threshold-60 MeV/nucleon; calculated triton microscopic optical model potential, reaction σ, elastic scattering σ(θ). Compared with some data.
doi: 10.1016/j.nuclphysa.2013.11.007
2014HA17 Nucl.Data Sheets 118, 132 (2014) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculation of Actinide Nuclear Reaction Data
doi: 10.1016/j.nds.2014.04.018
2014XU01 J.Phys.(London) G41, 015101 (2014) New Skyrme interaction parameters for a unified description of the nuclear properties NUCLEAR REACTIONS 28Si, 56Fe, 208Pb(n, X), (n, n), 27Al, 90Zr, 208Pb, 232Th(p, p), E<100 MeV; calculated σ, σ(θ). Skyrme-Hartree-Fock approach, comparison with available data.
doi: 10.1088/0954-3899/41/1/015101
2014XU09 Phys.Rev. C 90, 024604 (2014) Y.Xu, S.Goriely, A.J.Koning, S.Hilaire Systematic study of neutron capture including the compound, pre-equilibrium, and direct mechanisms NUCLEAR REACTIONS 16,18O, 22Ne, 26Mg, 27Al, 37Cl, 48Ca, 61Ni, 97Mo, 112Sn, 176Lu, 208Pb, 232Th(n, γ), E=0.001-10 MeV; calculated total capture σ(E) for three processes of compound-nucleus capture (CNC), pre-equilibrium capture (PEC), and direct capture (DIC) using Hauser-Feshbach model, the exciton model, and potential model, respectively, and Compared with experimental data. Z=8-100, N=10-180; calculated total neutron-capture cross sections and astrophysical reaction rates using TALYS code for about 8000 nuclei. Impact of the newly determined reaction rates on the r process abundances.
doi: 10.1103/PhysRevC.90.024604
2013HA04 Ann.Nucl.Energy 55, 75 (2013) Double differential cross sections of light charged particle emission of n + 27Al reaction NUCLEAR REACTIONS 27Al(n, xp), (n, xd), (n, xt), (n, xα), (n, 3He), E<40 MeV; calculated σ(E, θ), σ(E). Comparison with available data.
doi: 10.1016/j.anucene.2012.11.031
2013XU06 Phys.Rev. C 87, 044605 (2013) Toward a systematic nucleus-nucleus potential for peripheral collisions NUCLEAR REACTIONS 40Ca(6Li, 6Li), E=99.0, 156.0, 210.0, 240.0 MeV; 48Ca(6Li, 6Li), E=240.0 MeV; 58Ni(6Li, 6Li), E=12, 20, 34.0, 73.7, 90.0, 99.0, 240.0 MeV; 58Fe(6Li, 6Li), E=15 MeV; 65Cu(6Li, 6Li), E=25 MeV; 70Ge(6Li, 6Li), E=28 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=70.0, 73.7, 99.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 116Sn(6Li, 6Li), E=20, 240.0; 120Sn(6Li, 6Li), E=44.0, 90.0; 124Sn(6Li, 6Li), E=73.7 MeV; 144Sm(6Li, 6Li), E=21, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25, 31.0, 33.0, 35.0, 39.0, 50.6, 73.7, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=32.8, 36.0, 40.0 MeV; 40,48Ca(7Li, 7Li), E=34.0, 88.0 MeV; 44Ca(7Li, 7Li), E=34.0; 48Ca(7Li, 7Li), E=88 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe(7Li, 7Li), E=34.0; 58Ni(7Li, 7Li), E=34.0, 42.0, 73.7, 90, 99 MeV; 59Co(7Li, 7Li), E=12, 18 MeV; 60Ni(7Li, 7Li), E=34.0 MeV; 65Cu(7Li, 7Li), E=2 MeV; 80Se(7Li, 7Li), E=14, 23 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 90Zr(7Li, 7Li), E=34.0, 70, 99 MeV; 118Sn(7Li, 7Li), E=48.0 MeV; 120Sn(7Li, 7Li), E=90 MeV; 124Sn(7Li, 7Li), E=73.7 MeV; 144Sm(7Li, 7Li), E=21.6, 30.1, 35.1, 40.8, 42.3, 52.0 MeV; 208Pb(7Li, 7Li), E=27, 33.0, 39.0, 42.0, 52.0, 73.7 MeV; 208Pb(12C, 12C), E=58.9.64.9, 74.9, 84.9 MeV; 208Pb(16O, 16O), E=80, 90, 102 MeV; 12C, 28Si, 40Ca, 90Zr, 208Pb(16O, 16O), E=94 MeV/nucleon; 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=44 MeV/nucleon; 40Ca, 58Ni, 96Mo(32S, 32S), E=151.5, 107.3, 180 MeV; analyzed σ(E, θ) data; deduced optical model parameters, and comparison with experimental data. 27Al, 40Ca, 54,56,57Fe, 64,66,68Zn, 89Y, Ag(12C, X), E=30, 83 MeV/nucleon; 12C, 27Al, 64Zn, 93Nb, 107Ag, 118Sn, 144,150,154Sm(20Ne, X), E=30 MeV/nucleon; 12C, 27Al, 51V, 54Fe, 107Ag, 118Sn, 208Pb(40Ar, X), E=44 MeV/nucleon; 27Al, 64Zn, 93Nb, 118Sn, 144Sm, 181Ta, 208Pb(40Ca, X), E=77 MeV/nucleon; analyzed total reaction cross sections with optical model calculations. A single-folding model based on Bruyeres Jeukenne-Lejeune-Mahaux (JLMB) nucleon-nucleus potential.
doi: 10.1103/PhysRevC.87.044605
2013XU07 Astrophys.J. 769, 72 (2013) Absolute Integral Cross Sections and Product Branching Ratios for the Vibrationally Selected Ion-Molecule Reactions: N+2(X2Σ+g;υ+ =0-2) + CH4
doi: 10.1088/0004-637X/769/1/72
2013XU14 Nucl.Phys. A918, 61 (2013) Y.Xu, K.Takahashi, S.Goriely, M.Arnould, M.Ohta, H.Utsunomiya NACRE II: an update of the NACRE compilation of charged-particle-induced thermonuclear reaction rates for nuclei with mass number A ≤ 16 COMPILATION 2,3H, 3He, 6,7Li, 7,9Be, 10,11B, 12,13C, 13,14,15N(p, X), (α, X), E≈0.1 keV-1 MeV;2,3H, 3He(d, X), E≈0.1 keV-1 MeV;3He(3He, 2p), E≈0.1 keV-1 MeV; compiled, evaluated Q-value, σ, S-factor, reaction rates using DWBA, potential models; deduced model parameters.
doi: 10.1016/j.nuclphysa.2013.09.007
2013zu01 Hyperfine Interactions 220, 87 (2013) Y.Zuo, Y.Zheng, Y.Xu, B.Cui, L.Li, Y.Ma, F.Ping, D.Yuan, S.Gao, S.Zhu Production of 62Zn radioactive nuclear beam and on-line PAC investigation of quadrupole interaction in nano-magnetic material Fe73.5Cu1Nb3Si13.5B9 NUCLEAR REACTIONS 63Cu(p, 2n), E=22.9 MeV; Cd(p, X)111In, E=16.9 MeV; 186W(d, p), E=12.6 MeV; measured reaction products, Eγ, Iγ; deduced σ, spin rotation functions, quadrupole interaction frequencies. Perturbed angular correlation (PAC) and positron annihilation spectroscopy (PAS).
doi: 10.1007/s10751-013-0848-Z
2012CO01 Astrophys.J. 744, 158 (2012) A.Coc, S.Goriely, Y.Xu, M.Saimpert, E.Vangioni Standard Big Bang Nucleosynthesis up to CNO with an Improved Extended Nuclear Network NUCLEAR REACTIONS 7Li(d, γ), (t, n), (t, p), (d, n), 8Li(α, n), 11B(d, n), (d, p), (n, γ), 11C(d, p), (n, α), E<10 MeV; calculated astrophysical reaction rates. TALYS code, comparison with NACRE compilations.
doi: 10.1088/0004-637X/744/2/158
2012HA16 Ann.Nucl.Energy 46, 179 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen The analysis of n+237Np reactions for energies up to 200 MeV NUCLEAR REACTIONS 237Np(n, γ), (n, F), (n, 2n), (n, xn), (n, xp), (n, xd), (n, xt), (n, xα) E<200 MeV; calculated σ, σ(θ, E), σ(θ), σ(E). Optical model, the intra-nuclear cascade model, the unified Hauser-Feshbach theory, comparison with ENDF/B-VII and JENDL-3 libraries and available data.
doi: 10.1016/j.anucene.2012.03.013
2012HA24 Nucl.Sci.Eng. 172, 102 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculations and Analysis of n + 27Al Reaction NUCLEAR REACTIONS 27Al(n, X), (n, n), (n, n'), (n, p), (n, γ), (n, d), (n, t), (n, α), (n, 2n), (n, xn), (n, xp), (n, xα), E<200 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Comparison with ENDF/B-VII and JENDL-3 evaluated nuclear libraries.
doi: 10.13182/NSE11-28
2012XU09 Phys.Rev. C 86, 045801 (2012) Systematic study of direct neutron capture NUCLEAR STRUCTURE Z=8-102; calculated E1, E2, and M1 neutron direct capture reaction rates of astrophysical interest for 6400 nuclei at temperature T9=1. NUCLEAR REACTIONS 16O, 18O, 22Ne, 26Mg, 27Al, 36S, 37Cl, 46,48Ca, 122,132Sn(n, γ), E=1-10000 keV; calculated total neutron direct capture cross sections. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.045801
2011GU15 Phys.Rev. C 83, 064618 (2011) H.Guo, Y.Xu, H.Liang, Y.Han, Q.Shen 4He microscopic optical model potential NUCLEAR REACTIONS 12C, 58Ni, 116Sn, 208Pb(α, X), E=20-300 MeV; calculated radial dependence of real and imaginary parts of the potential, volume integral and rms radii. 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb, 209Bi(α, X), E=5-200 MeV; calculated reaction σ(E). 62,64Ni, 63,65Cu, 64,66,68,70Zn, 70,72Ge(α, α), E=25.0 MeV; 94Mo, 107Ag, 116,122,124Sn(α, α), E=25.2 MeV; 20,22Ne, 24,26Mg, 28Si, 40Ar, 40,42,44,48Ca, 56Fe, 56,58,60,62Ni, 90Zr, 124Sn, 208Pb(α, α), E=104 MeV; 16O, 46,48Ti, 58Ni, 116Sn, 197Au(α, α), E=240 MeV; 12C, 58Ni, 90Zr, 116Sn, 144Sm, 208Pb(α, α), E=386.0 MeV; calculated σ(θ). 12C(α, α), E=120.0-400 MeV; 58Ni(α, α), E=29.0-386 MeV; 24Mg(α, α), E=39.0-172.5 MeV; 107Ag(α, α), E=15.0-43.0 MeV; 116Sn(α, α), E=23.3-386 MeV; 124Sn(α, α), E=23.3-104 MeV; 208Pb(α, α), E=23.6-386.0 MeV; 209Bi(α, α), E=19.0-104 MeV; calculated σ(E, θ); deduced 4He microscopic optical model potential by Greens function method. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064618
2011HA28 Ann.Nucl.Energy 38, 1852 (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Calculation and evaluations for n + 63, 65, nat.Cu reactions NUCLEAR REACTIONS Cu, 63,65Cu(n, X), (n, n), (n, n'), (n, γ), (n, p), (n, d), (n, α), (n, 2n), (n, 3n), E<250 MeV; calculated σ, σ(θ). Optical model, preequilibrium theory, comparison with ENDF/B-VII.0, JENDL-3.3 evaluated nuclear libraries and experimental data.
doi: 10.1016/j.anucene.2011.05.016
2011HA29 Ann.Nucl.Energy 38, 1950 (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Double differential cross sections of n + 63, 65, nat.Cu reactions NUCLEAR REACTIONS Cu, 63,65Cu(n, X), (n, xn), (n, xp), (n, xα), (n, xd), (n, xt), E<200 MeV; calculated σ(θ, E). Optical model, unified Hauser-Feshbach and exciton model, comparison with ENDF/B-VII.0, JENDL-3.3 evaluated nuclear libraries and experimental data.
doi: 10.1016/j.anucene.2011.05.001
2011HA44 J.Korean Phys.Soc. 59, 855s (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen, C.Cai The Theoretical Calculation of Cross Section and Spectrum for n+238U Reaction up to 150 MeV NUCLEAR REACTIONS 238U(n, f), (n, xn), (n, d), (n, t), (n, p), (n, α), E=0-200 MeV; calculated σ, dσ(E, θ) using different reaction models.
doi: 10.3938/jkps.59.855
2010HA06 Phys.Rev. C 81, 024616 (2010) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Global phenomenological optical model potential for nucleon-actinide reactions at energies up to 300 MeV NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np, 239,240,242Pu, 241Am(n, X), E=0.01-300 MeV; calculated total σ. 235,238U(n, n), E=0.01-300 MeV; calculated σ. 232Th, 235,238U, 239Pu(n, n'), E=0.1-300 MeV; calculated non-inelastic σ. 232Th, 235,238U, 239Pu(n, n), (n, n'), E=0.14-15.2 MeV; 238U(n, n), E=96 MeV; calculated σ(θ) for elastic σ, inelastic σ and elastic+inelastic σ. 232Th, 238U(p, X), E=0-300 MeV; calculated σ. 232Th, 235,238U(p, p), (p, p'), E=16-95 MeV; calculated σ(θ). global phenomenological optical model potential. Deduced of neutron and proton global optical model potential parameters. Comparison and analysis with experimental data.
doi: 10.1103/PhysRevC.81.024616
2010YU04 Nucl.Phys. A834, 97c (2010) Z.Yu, G.-Z.Liu, M.-F.Zhu, Y.Xu, E.-G.Zhao Thermal neutron stars including the hyperon-hyperon interactions
doi: 10.1016/j.nuclphysa.2010.01.029
2010ZH03 Chin.Phys.Lett. 27, 022102 (2010) Y.-N.Zheng, D.-M.Zhou, D.-Q.Yuan, Y.zuo, P.fan, M.Mihara, K.Matsuta, M.Fukuda, T.Minamisono, T.Suzuki, Y.-J.Xu, J.-Z.Zhu, Z.-Q.Wang, H.-L.Luo, X.-Z.Zhang, S.-Y.Zhu Nuclear Structure and Magnetic Moment of the Unstable 12B-12N Mirror Pair NUCLEAR MOMENTS 12B, 12N; measured β-NMR spectra; deduced magnetic moments, magic numbers. Comparison with shell model calculations.
doi: 10.1088/0256-307X/27/2/022102
2010ZH38 Nucl.Phys. A834, 761c (2010) Y.Zheng, Y.Zuo, D.Yuan, D.Zhou, Y.Xu, P.Fan, J.Zhu, Z.Wang, S.Zhu Investigation of Radiation Damage in Stainless steel, Tungsten and Tantalum by Heavy Ion Irradiations
doi: 10.1016/j.nuclphysa.2010.01.139
2009IJ01 Phys.Rev. C 80, 034322 (2009) Q.A.Ijaz, W.C.Ma, H.Abusara, A.V.Afanasjev, Y.B.Xu, R.B.Yadav, Y.C.Zhang, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, D.T.Nisius Excited superdeformed bands in 154Dy and cranked relativistic mean field interpretation NUCLEAR REACTIONS 122Sn(36S, 4n), E=165 MeV; measured Eγ, Iγ, γγ-coin using Gammasphere array. 154Dy; deduced levels, J, π, superdeformed bands, dynamic moments of inertia, neutron single particle energies. Comparison with the cranked relativistic mean field calculations.
doi: 10.1103/PhysRevC.80.034322
2009LU19 Phys.Rev. A 80, 051201 (2009) H.Y.Lu, J.S.Liu, C.Wang, W.T.Wang, Z.L.Zhou, A.H.Deng, C.Q.Xia, Y.Xu, X.M.Lu, Y.H.Jiang, Y.X.Leng, X.Y.Liang, G.Q.Ni, R.X.Li, Z.Z.Xu Efficient fusion neutron generation from heteronuclear clusters in intense femtosecond laser fields NUCLEAR REACTIONS 2H(γ, xnyp), E not given; measured densities and average kinetic energies of deuterium ions; deduced fusion neutron yields as a function of laser energy.
doi: 10.1103/PhysRevA.80.051201
2009TA07 Phys.Rev. C 79, 051901 (2009) Z.Tang, Y.Xu, L.Ruan, G.van Buren, F.Wang, Z.Xu Spectra and radial flow in relativistic heavy ion collisions with Tsallis statistics in a blast-wave description
doi: 10.1103/PhysRevC.79.051901
2009XU02 Chem.Phys. 18, 1421 (2009) Y.Xu, W.Xu, Y.-G.Ma, X.-Z.Cai, J.-G.Chen, G.-T.Fan, G.-W.Fan, W.Guo, W.Luo, Q.-Y.Pan, W.-Q.Shen, L.-F.Yang Determination of the stellar reaction rate for 12C(α, γ)16O: using a new expression with the reaction mechanism NUCLEAR REACTIONS 12C(α, γ);E not given; calculated astrophysical reaction rates.
doi: 10.1088/1674-1056/18/4/023
2009XU06 Nucl.Phys. A830, 701c (2009) Y.Xu, and the STAR collaboration Measurements of neutral and charged kaon production at high pT up to 15 GeV/c at STAR
doi: 10.1016/j.nuclphysa.2009.09.059
2009YA25 Chin.Phys.C 33, Supplement 1, 196 (2009) W.-F.Yang, Z.-Z.Zhao, S.-G.Yuan, Y.-B.Xu, X.T.Lu Dependence of the cross sections for Ir isotopes on the values of Qgg in the heavy ion collision NUCLEAR REACTIONS 197Au(12C, X)184Ir/185Ir/186Ir/187Ir/189Ir/190Ir/192Ir/194Ir/195Ir/196Ir, E=47 MeV/nucleon; measured Eγ, Iγ; deduced σ.
doi: 10.1088/1674-1137/33/S1/063
2009YU11 Chin.Phys.C 33, Supplement 1, 191 (2009) S.-G.Yuan, Y.-B.Xu, H.-J.Ding, W.-F.Yang, Y.-H.Xiao, Y.-N.Niu Gamma decay of the lowly excited states of 189Re RADIOACTIVITY 189W(β-) [from 192Os(n, α)189Re, E=14 MeV];measured Eγ, Iγ, X-γ-coin., γ-γ-coin.; deduced decay scheme, J, π, energies.
doi: 10.1088/1674-1137/33/S1/061
2007XU04 J.Radioanal.Nucl.Chem. 272, 227 (2007) Y.B.Xu, S.D.Zhang, H.J.Ding, X.T.Lu, W.F.Yang, S.G.Yuan, Y.H.Xiao, Y.N.Niu Production cross section of 236Th in the interaction of 238U with 60 MeV/u 18O ions NUCLEAR REACTIONS 238U(18O, 20Ne), E=60 MeV/nucleon; measured Eγ, Iγ; deduced σ.
doi: 10.1007/s10967-007-0505-6
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