NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = Y.N.Xu Found 92 matches. 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
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
2024XU05 Phys.Lett. B 852, 138622 (2024) Y.Xu, D.L.Balabanski, V.Baran, C.Iorga, C.Matei Vortex photon induced nuclear reaction: Mechanism, model, and application to the studies of giant resonance and astrophysical reaction rate NUCLEAR REACTIONS 73,75As, 74Se, 84Sr, 92Mo, 96Ru, 106Cd(γ, p), 80Se, 79Br, 89Y, 93Nb, 96Mo, 97Tc, 106Pd, 110Cd, 118Sn, 134Ba, 138Ce, 150Gd, 156,158Dy, 162Er(γ, X), 60Fe, 64Ni, 65Zn, 77Se, 87,88Sr, 105Pd, 148Pm, 152Sm, 153Eu, 155,156Eu, 154Gd, 165Er, 171,172Tm, 180,181Ta, 187,188Os, 199Hg, 205Tl, 205,206Pb, 98,99Mo, 146,147,148,149Nd, 148,149,150Sm, 171,172,173Yb, 179,180,181Hf, 186W, 122,123Sn, 125Sn, 121Sb, 123,124,125Sb, 122,123Te, 125Te, 57,58Fe, 66,67,68Zn, 71Ga, 73,74Ge, 78Se, 81Br, 86,87Rb, 94Zr, 95Mo, 100,101,102Ru, 104Ru, 107Pd, 108,110Ag, 114In, 120Sn, 123Sb, 124Te, 129I, 134Cs, 140La, 139Ba, 63Ni, 95,96Zr, 135Cs, 149Pm, 151Sm, 154Eu, 153Gd, 160,161Tb, 163Ho, 170Tm, 179Ta, 185W, 204Tl, 113Cd, 121Sn, 176Lu, 182Hf, 89Zr, 54Fe, 90Zr, 100Mo, 114Cd, 115In, 124Sn, 128,130Te, 139La, 140Ce, 142Nd, 144Sm, 164Dy, 196Pt, 208Pb, 209Bi(n, γ), E<1 MeV; calculated nuclear reaction induced by vortex γ-rays to investigate giant resonances (GR) of higher multipolarity using the interaction formalism nd the Hauser-Feshbach model.
doi: 10.1016/j.physletb.2024.138622
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
2006TA02 Phys.Rev.Lett. 96, 034301 (2006); Erratum Phys.Rev.Lett. 96, 179903 (2006) R.P.Taleyarkhan, C.D.West, R.T.Lahey, Jr., R.I.Nigmatulin, R.C.Block, Y.Xu Nuclear Emissions During Self-Nucleated Acoustic Cavitation NUCLEAR REACTIONS 2H(d, n), E not given; measured Eγ, En for deuterated benzene and acetone mixtures. Acoustic inertial confinement.
doi: 10.1103/PhysRevLett.96.034301
2006XU10 Phys.Rev. C 74, 047303 (2006) Y.Xu, S.Zhang, H.Ding, S.Yuan, W.Yang, Y.Niu, X.Lu, Y.Li, Y.Xiao Search for β-delayed fission of 228Ac RADIOACTIVITY 228Ra(β-); measured β-delayed fission fragment tracks. 228Ac deduced β-delayed fission probability. Radiochemical separation, mica foils.
doi: 10.1103/PhysRevC.74.047303
2004XU08 J.Phys.Soc.Jpn. 73, 2588 (2004) Y.Xu, W.Yang, S.Yuan, Y.Niu, H.Ding, X.Wang, L.Zhao, P.Wang, H.Li Identification of 186mTa NUCLEAR REACTIONS W(n, X), E=14 MeV; measured β-delayed Eγ, Iγ; deduced evidence for 173Hf, 179,179m,185m,187W, 182m,184,185,186mTa. RADIOACTIVITY 186mTa(β-) [from W(n, X)]; measured Eγ, Iγ, T1/2.
doi: 10.1143/JPSJ.73.2588
2003XU08 J.Radioanal.Nucl.Chem. 258, 439 (2003) Y.Xu, W.Yang, S.Yuan, Y.Xiao, X.Zhou, J.He Observation of 197Os RADIOACTIVITY 197Os(β-) [from 198Pt(n, 2p)]; measured β-delayed Eγ, Iγ, γγ-, (X-ray)γ-coin, T1/2. 197Ir deduced levels, J, π.
doi: 10.1023/A:1026274813313
2002XU06 J.Radioanal.Nucl.Chem. 251, 341 (2002) Y.Xu, W.Yang, S.Yuan, Y.Xiao, Q.Pan, Y.Li Cross Sections of Barium Isotopes in the Interaction of 60 MeV/Nucleon 18O with 238U NUCLEAR REACTIONS 238U(18O, X)126Ba/127Ba/128Ba/129Ba/129mBa/131Ba/131mBa/133mBa/135mBa/139Ba/140Ba/141Ba/142Ba, E=60 MeV/nucleon; measured production σ. Activation, radiochemical separation.
doi: 10.1023/A:1014801302057
2001YU03 Eur.Phys.J. A 10, 1 (2001) S.Yuan, W.Yang, Y.Xu, Q.Pan, B.Xiong, J.He, D.Wang, Y.Li, T.Ma, Z.Yang Search for β-Delayed Fission of the Heavy Neutron-Rich Isotope 230Ac RADIOACTIVITY 230Ra(β-) [from 232Th(18O, 20Ne)]; measured β-delayed fission fragment tracks. 230Ac deduced β-delayed fission probability. Radiochemical separation, mica foils.
doi: 10.1007/s100500170136
2001ZH43 Hyperfine Interactions 136/137, 149 (2001) S.-Y.Zhu, J.Zhu, T.Minamisono, K.Matsuta, Y.Xu, M.Fukuda, M.Mihara, Z.Wang, K.Sato, H.Akai, C.Rong, C.Chu, J.Chen, H.Luo On-line Time Differential Perturbed Angular Correlation with Light Probe Nucleus 19F RADIOACTIVITY 19O(β-); measured Eγ, Iγ(θ, H, t). 19F deduced quadrupole moment. On-line time differential perturbed angular correlation.
doi: 10.1023/A:1020532332334
2000XU02 Phys.Rev. C61, 067308 (2000) Y.Xu, S.Yuan, W.Yang, J.He, Z.Li, T.Ma, B.Xiong New Determination of the 237Th Half-Life RADIOACTIVITY 237Th(β-) [from U(18O, X)]; 237Pa(β-) [from 237Th decay]; measured Eγ, Iγ(t), T1/2. Comparison with model predictions, previous data.
doi: 10.1103/PhysRevC.61.067308
1999HE01 Phys.Rev. C59, 520 (1999) J.He, W.Yang, S.Yuan, Y.Xu, Z.Li, T.Ma, B.Xiong, Z.Qin, W.Mou, Z.Gan, L.Shi, T.Guo, Z.Chen, J.Guo Synthesis and Identification of a New Heavy Neutron-Rich Isotope 238Th NUCLEAR REACTIONS 238U(18O, X), E=60 MeV/nucleon; measured Eγ, Iγ(t)(X-ray)γ-coin; deduced evidence for 238Th. Radiochemical separation. RADIOACTIVITY 238Th(β-) [from 238U(18O, X), E=60 MeV/nucleon]; measured Eγ, Iγ(t), (X-ray)γ-coin; deduced T1/2.
doi: 10.1103/PhysRevC.59.520
1999HE44 High Energy Phys. and Nucl.Phys. (China) 23, 1044 (1999) J.He, W.Yang, S.Yuan, T.Ma, Z.Li, B.Xiong, Y.Xu Identification of New Isotope 238Th
1999XI05 J.Radioanal.Nucl.Chem. 242, 163 (1999) B.Xiong, W.Yang, S.Yuan, T.Ma, J.He, Y.Xu, Z.Li Identification of a New Heavy Neutron-Rich Isotope 238Th NUCLEAR REACTIONS U(16O, X), E=60 MeV/nucleon; measured delayed Eγ, Iγ(t); deduced evidence for 238Th. Radiochemical separation. RADIOACTIVITY 238Th(β-) [from U(16O, X)]; measured T1/2.
1999XU06 High Energy Phys. and Nucl.Phys. (China) 23, 93 (1999) Y.Xu, S.Yuan, W.Yang, J.He, Z.Li, T.Ma, B.Xiong, Z.Qin, W.Mou, Z.Gan, L.Shi, T.Guo, Z.Chen, J.Guo A New Heavy Neutron-rich Isotope 238Th
1998HE36 High Energy Phys. and Nucl.Phys. (China) 22, 1057 (1998) J.He, S.Yuan, W.Yang, Z.Li, T.Ma, K.Fang, S.Shen, Z.Gan, Q.Pan, Z.Chen, T.Guo, W.Mou, D.Su, Y.Xu, J.Guo, H.Liu, L.Shi, Z.Zhao, H.Ma A new isotope of hafnium: 186Hf
1998YU02 Phys.Rev. C57, 1506 (1998) S.Yuan, W.Yang, Z.Li, J.He, T.Ma, K.Fang, S.Shen, Z.Gan, Q.Pan, Z.Chen, T.Guo, W.Mou, D.Su, Y.Xu, J.Guo, H.Liu, L.Shi, Z.Zhao, H.Ma Production and Identification of a New Heavy Neutron-Rich Isotope 186Hf NUCLEAR REACTIONS W(18O, X), E=60 MeV/nucleon; measured Eγ, Iγ(t); deduced evidence for 186Hf. Transfer reaction, chemical separation of source. RADIOACTIVITY 186Hf(β-) [from W(18O, X)]; measured Eγ, Iγ(t), T1/2.
doi: 10.1103/PhysRevC.57.1506
1997ZA03 Phys.Rev. C55, 2697 (1997); Erratum Phys.Rev. C57, 1006 (1998) K.Zaerpoor, Y.Xu, M.Gummin, K.S.Krane, J.L.Wood, N.J.Stone, J.Rikovska Verification of Isomerism and Direct Measurement of Half-Lives in 184Au RADIOACTIVITY 184mAu(β+), (EC) [from 181Ta(12C, 9n), E=140 Mev]; measured T1/2, Iγ, I(ce). 184Au deduced isomer ordering, T1/2, possible J, π.
doi: 10.1103/PhysRevC.55.2697
1992GU14 Hyperfine Interactions 75, 447 (1992) M.A.Gummin, K.S.Krane, Y.Xu, T.Lam, E.F.Zganjar, J.B.Breitenbach, B.E.Zimmerman, H.K.Carter, P.F.Mantica, Jr. Nuclear Structure Studies of 187Ir via On-Line Nuclear Orientation RADIOACTIVITY 187Pt(β+), (EC) [from 176Hf(16O, X), E=125 MeV]; measured γ-anisotropy vs temperature, Eγ, Iγ. 187Ir deduced levels, J, π, δ. Particle-plus-triaxial-rotor model.
doi: 10.1007/BF02399002
1992XU02 Phys.Rev.Lett. 68, 3853 (1992) Y.Xu, K.S.Krane, M.A.Gummin, M.Jarrio, J.L.Wood, E.F.Zganjar, H.K.Carter Shape Coexistence and Electric Monopole Transitions in 184Pt RADIOACTIVITY 184Au(EC), (β+) [from 181Ta(12C, xn), E=140 MeV]; measured γγ(t), γ(X-ray)(t), γ(ce)(t), (ce)(X-ray)(t). 184Pt deduced levels, J, π, K, γ-multipolarity, ICC. NUCLEAR REACTIONS 181Ta(12C, xn), E=140 MeV; measured γγ(t), γ(X-ray)(t), γ(ce)(t), (ce)(X-ray)(t) following residual decay. 184Pt deduced levels, J, π, K, γ-multipolarity, ICC.
doi: 10.1103/PhysRevLett.68.3853
1992XU06 Hyperfine Interactions 75, 481 (1992) Y.Xu, K.S.Krane, M.A.Gummin, J.L.Wood, M.M.Jarrio, J.B.Breitenbach, E.F.Zganjar, D.Rupnik, H.K.Carter, P.F.Mantica, Jr., B.E.Zimmerman On-Line Nuclear Orientation Study of 184Au RADIOACTIVITY 184Au(α), (β+), (EC) [from 181Ta(12C, 9n), E=140 MeV]; measured Eγ, Iγ, I(ce), γ-anisotropy, oriented nuclei. 184Pt deduced levels, J, π, δ(E2/M1), γ-multipolarity, ICC.
doi: 10.1007/BF02399005
1991SZ01 Phys.Rev. C43, 849 (1991) J.J.Szymanski, P.D.Barnes, G.E.Diebold, R.A.Eisenstein, G.B.Franklin, R.Grace, D.W.Hertzog, C.J.Maher, B.P.Quinn, R.Rieder, J.Seydoux, W.R.Wharton, S.Bart, R.E.Chrien, P.Pile, R.Sutter, Y.Xu, R.Hackenburg, E.V.Hungerford, T.Kishimoto, L.G.Tang, B.Bassalleck, R.L.Stearns Nonleptonic Weak Decay of 5He(Lambda) and 12C(Lambda) NUCLEAR REACTIONS 6Li, 12C(K-, π-), E not given; measured hypernuclear mass spectra; deduced decay features.
doi: 10.1103/PhysRevC.43.849
1988MU13 Phys.Rev. D38, 742 (1988) G.S.Mutchler, J.Clement, J.Kruk, R.Moss, E.Hungerford, T.Kishimoto, B.Mayes, L.Pinsky, L.Tang, Y.Xu, B.Bassalleck, T.Armstrong, K.Hartman, A.Hicks, R.Lewis, W.Lochstet, G.A.Smith, D.Lowenstein, H.Poth, W.von Witsch, M.Furic Measurement of the Imaginary Part of the I = 1 (N-Bar)N S-Wave Scattering Length NUCLEAR REACTIONS 1H(p-bar, n-bar), E at 415 MeV/c; measured n-bar spectra; deduced (p)(n-bar) S-wave scattering length.
doi: 10.1103/PhysRevD.38.742
1985GR10 Phys.Rev.Lett. 55, 1055 (1985) R.Grace, P.D.Barnes, R.A.Eisenstein, G.B.Franklin, C.Maher, R.Rieder, J.Seydoux, J.Szymanski, W.Wharton, S.Bart, R.E.Chrien, P.Pile, Y.Xu, R.Hackenburg, E.Hungerford, B.Bassalleck, M.Barlett, E.C.Milner, R.L.Stearns Weak Decay of (Lambda)12C and (Lambda)11B Hypernuclei NUCLEAR REACTIONS 12C(K-, π-), (K-, π-p), E at 800 MeV/c; measured pion momenta; deduced hypernuclei 12C, 11B ground state T1/2.
doi: 10.1103/PhysRevLett.55.1055
1983MA64 Phys.Rev.Lett. 51, 2085 (1983) M.May, S.Bart, S.Chen, R.E.Chrien, D.Maurizio, P.Pile, Y.Xu, R.Hackenburg, E.Hungerford, H.Piekarz, Y.Xu, M.Deutsch, J.Piekarz, P.D.Barnes, G.Franklin, R.Grace, C.Maher, R.Rieder, J.Szymanski, W.Wharton, R.L.Stearns, B.Bassalleck, B.Budick Observation of Hypernuclear Gamma-Ray Transitions in 7Li(Lambda) and 9Be(Lambda) NUCLEAR REACTIONS 9Be, 7Li(K-, π-), E at 820 MeV/c; measured γ-hypernucleus energy coin spectra; deduced hypernuclear state transitions, (lambda)-nucleon spin-dependent interaction strength limits.
doi: 10.1103/PhysRevLett.51.2085
1982PI02 Phys.Lett. 110B, 428 (1982) H.Piekarz, S.Bart, R.Hackenburg, A.D.Hancock, E.V.Hungerford, B.Mayes, K.Sekharan, J.Piekarz, M.Deutsch, R.E.Chrien, S.Chen, M.LeVine, D.Maurizio, M.May, H.Palevsky, Y.Xu, P.D.Barnes, B.Bassalleck, R.Eisenstein, R.Grace, C.Maher, P.Pile, R.Rieder, W.Wharton, R.L.Stearns Experimental Observation of the Σ Hypernuclei, 6H(Σ) and 16C(Σ) NUCLEAR REACTIONS 6Li, O(K-, π+), E at 713 MeV/c; measured σ(θ, E); deduced hypernuclei levels, widths, reaction strengths.
doi: 10.1016/0370-2693(82)91031-0
1981MA27 Phys.Rev.Lett. 47, 1106 (1981) M.May, H.Piekarz, R.E.Chrien, S.Chen, D.Maurizio, H.Palevsky, R.Sutter, Y.Xu, P.Barnes, B.Bassalleck, N.J.Colella, R.Eisenstein, R.Grace, P.Pile, F.Takeutchi, W.Wharton, M.Deutsch, J.Piekarz, S.Bart, R.Hackenburg, E.V.Hungerford, B.Mayes, L.Pinsky, R.Cester, R.L.Stearns Observation of Levels in 13C, 14N, and 18O Hypernuclei NUCLEAR REACTIONS 13C, 18O, 14N(K-, π-), E at 800 MeV/c; measured σ(θ, E(π)); deduced levels in 13C, 14N, 18O hypernuclei, configurations.
doi: 10.1103/PhysRevLett.47.1106
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