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NSR database version of May 10, 2024.

Search: Author = Y.N.Xu

Found 92 matches.

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2024WA02      Phys.Rev. C 109, 014611 (2024)

B.Wang, Y.Xu, S.Goriely

Systematic study of the radiative proton capture including the compound, pre-equilibrium, and direct mechanisms

doi: 10.1103/PhysRevC.109.014611
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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
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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
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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
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2023WA36      Phys.Rev. C 108, 065805 (2023)

B.Wang, Y.Xu, X.Tang

Effective energy window of the E1 photon strength function for astrophysical neutron-capture reaction rates

doi: 10.1103/PhysRevC.108.065805
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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
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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
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2022SU13      Nucl.Sci.Eng. 196, 1031 (2022)

X.Su, Y.Xu, Y.Han

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
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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
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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
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2021BE28      Phys.Rev. C 104, 044332 (2021)

A.Berceanu, Y.Xu, Y.F.Niu

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
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2021KE02      Nucl.Phys. A1005, 122039 (2021)

W.Ke, Y.Xu, S.Bass

Quantifying heavy quark transport coefficients with an improved transport model

doi: 10.1016/j.nuclphysa.2020.122039
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2021SU05      Nucl.Sci.Eng. 195, 239 (2021)

X.Su, Y.Xu, Y.Han

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
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2021XU04      Phys.Rev. C 104, 044301 (2021)

Y.Xu, S.Goriely, E.Khan

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0260. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0970.


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
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2019KE08      Phys.Rev. C 100, 064911 (2019)

W.Ke, Y.Xu, S.A.Bass

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
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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
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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
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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
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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
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2018HU09      Nucl.Sci.Eng. 191, 262 (2018)

J.Hu, Y.Xu, Y.Han

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
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2018KE05      Phys.Rev. C 98, 064901 (2018)

W.Ke, Y.Xu, S.A.Bass

Linearized Boltzmann-Langevin model for heavy quark transport in hot and dense QCD matter

doi: 10.1103/PhysRevC.98.064901
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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
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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
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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
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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
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2018XU03      Int.J.Mod.Phys. E27, 1850023 (2018)

Y.Xu, Y.Han, Q.Shen

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
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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
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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
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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
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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
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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
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2017XU05      Phys.Rev. C 96, 024621 (2017)

Y.Xu, H.Guo, Y.Han, Q.Shen

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
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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
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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
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2017XU09      Int.J.Mod.Phys. E26, 1750065 (2017)

Y.Xu, H.Guo, Y.Han, Q.Shen

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0789.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32736.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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2014XU01      J.Phys.(London) G41, 015101 (2014)

Y.Xu, H.Guo, Y.Han, Q.Shen

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
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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
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2013HA04      Ann.Nucl.Energy 55, 75 (2013)

Y.Han, Y.Xu, C.Cai, Q.Shen

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
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2013XU07      Astrophys.J. 769, 72 (2013)

Y.Xu, Y.C.Chang, Z.Lu, C.Y.Ng

Absolute Integral Cross Sections and Product Branching Ratios for the Vibrationally Selected Ion-Molecule Reactions: N+2(X2Σ+g+ =0-2) + CH4

doi: 10.1088/0004-637X/769/1/72
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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
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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
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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
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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
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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
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2012XU09      Phys.Rev. C 86, 045801 (2012)

Y.Xu, S.Goriely

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
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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 Green¬Ěs function method. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.064618
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0300.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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