NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Y.He Found 84 matches. 2024CH17 Eur.Phys.J. A 60, (2024) Y.Chen, Y.Qiu, Q.Li, Sh.Tang, Y.Yang, Zh.Ren, W.Jiang, R.Fan, H.Yi, R.Liu, J.Tang, H.Jing, Ch.Lan, Y.Li, Zh.Tan, Q.An, J.Bai, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Zh.Chen, Z.Cui, Ch.Feng, K.Gao, X.Gao, M.Gu, Ch.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, H.Huang, X.Huang, H.Jiang, Zh.Jiang, L.Kang, B.Li, Ch.Li, J.Li, X.Li, J.Liu, Sh.Liu, X.Liu, Z.Long, G.Luan, Ch.Ning, M.Niu, B.Qi, J.Ren, X.Ruan, Zh.Song, K.Sun, Zh.Sun, X.Tang, B.Tian, L.Wang, P.Wang, Zh.Wang, Zh.Wen, X.Wu, X.Wu, L.Xie, X.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Zh.Zhang, L.Zhou, Zh.Zhou, K.Zhu Measurement of the neutron flux of CSNS Back-n ES#1 under small collimators from 0.5 eV to 300 MeV NUCLEAR REACTIONS 235U(n, F), 6Li(n, X), E=0.0000005-300 MeV; measured reaction products, En, In, TOF; deduced σ, neutron flux and uncertainties. China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-024-01272-z
2024LU05 Phys.Rev. C 109, 034919 (2024) T.Luo, Y.He, Sh.Cao, X.-N.Wang Linear Boltzmann transport for jet propagation in the quark-gluon plasma: Inelastic processes and jet modification
doi: 10.1103/PhysRevC.109.034919
2024PU01 Ann.Nucl.Energy 203, 110490 (2024) N.Pu, X.-Ch.Zhang, H.-J.Cai, H.Jia, Y.He Simulation of in-core neutron monitoring with U-235 micro fission chamber for CiADS-like LFR
doi: 10.1016/j.anucene.2024.110490
2024WA14 Phys.Lett. B 850, 138503 (2024) J.G.Wang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, H.B.Yang, C.L.Yang, Y.H.Qiang, X.Y.Huang, Z.Zhao, S.Y.Xu, Z.C.Li, L.X.Chen, L.C.Sun, H.Zhou, X.Zhang, X.L.Wu, Y.L.Tian, Y.S.Wang, J.Y.Wang, W.X.Huang, M.L.Liu, Z.W.Lu, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α-decay properties of new neutron-deficient isotope 203Ac RADIOACTIVITY 203Ac, 199Fr, 195At, 191Bi(α) [from 169Tm(40Ca, 6n)203Ac, E=226 MeV]; measured decay products, Eα, Iα; deduced α-particle energies, transitions T1/2, J, π, partial decay scheme, reduced α-decay widths, proton separation energies, the onset of deformation in neutron-deficient Ac isotopes. Comparison with systematics. The superconducting linear accelerator, China Accelerator Facility for superheavy Elements (CAFE2) at Institute of Modern Physics, Chinese Academy of Sciences.
doi: 10.1016/j.physletb.2024.138503
2024ZH04 Phys.Rev. C 109, 014608 (2024) M.M.Zhang, Z.Y.Zhang, Z.G.Gan, N.Wang, H.Yao, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, C.L.Yang, Y.L.Tian, Y.S.Wang, J.Y.Wang, Y.H.Qiang, X.L.Wu, S.Y.Xu, X.Y.Huang, Z.C.Li, Z.Zhao, L.C.Sun, H.Zhou, X.Zhang, G.Xie, L.Zhu, J.H.Zheng, Y.J.Li, F.Guan, Z.W.Lu, W.X.Huang, Y.He, H.S.Xu, Z.Z.Ren, S.G.Zhou Experimental cross section study of 40Ca + 175Lu: Searching for new neutron-deficient Pa isotopes
doi: 10.1103/PhysRevC.109.014608
2024ZH19 Phys.Rev. C 109, 034314 (2024) Z.Zhao, Z.G.Gan, Z.Y.Zhang, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, M.M.Zhang, C.L.Yang, S.Y.Xu, X.Y.Huang, Z.C.Li, L.C.Sun, X.L.Wu, Y.S.Wang, Y.L.Tian, Y.H.Qiang, J.Y.Wang, W.X.Huang, Y.He, L.T.Sun, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov Reinvestigation of the decay properties of 261, 262Bh at the gas-filled recoil separator SHANS2
doi: 10.1103/PhysRevC.109.034314
2023EK01 Eur.Phys.J. A 59, 103 (2023) H.Ekawa, W.Dou, Y.Gao, Y.He, A.Kasagi, E.Liu, A.Muneem, M.Nakagawa, C.Rappold, N.Saito, T.R.Saito, M.Taki, Y.K.Tanaka, H.Wang, J.Yoshida Development of machine learning analyses with graph neural network for the WASA-FRS experiment
doi: 10.1140/epja/s10050-023-01016-5
2023HU15 Phys.Rev. C 108, 024608 (2023) D.-y.Huo, Z.Wei, K.Wu, C.Han, Y.-n.Han, Y.-x.Wang, P.-q.Zhang, Y.He, X.-j.Bao, Z.-y.Deng, Z.-e.Yao Effect of octupole deformation of fragments on mass-asymmetric yields of fission of actinide nuclei NUCLEAR REACTIONS 235,236,238,239U, 232Th, 239,240Pu, 237Np(n, F), E=1-10 MeV; calculated mass distributions of fission fragments, quadrupole and octupole deformations of scission configurations as a function of mass number of the fission fragments, neutron-charge ratio of fragments. Scission-point model with considering octupole deformation of fragments. Comparison to experimental data.
doi: 10.1103/PhysRevC.108.024608
2023WA35 Eur.Phys.J. A 59, 224 (2023) J.Wang, J.Ren, W.Jiang, X.Ruan, Q.Sun, J.Hu, B.Jiang, J.Bao, Q.Zhang, G.Luan, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, J.Bai, P.Cao, Q.Chen, Y.Chen, Z.Chen, Z.Cui, A.Fan, R.Fan, C.Feng, F.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, W.Jia, H.Jiang, Z.Jiang, Z.Jin, L.Kang, B.Li, C.Li, G.Li, J.Li, Q.Li, Y.Li, J.Liu, R.Liu, S.Liu, C.Ning, B.Qi, Z.Ren, Z.Song, K.Sun, Z.Tan, J.Tang, S.Tang, L.Wang, P.Wang, Z.Wang, Z.Wen, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, Y.Yu, G.Zhang, L.Zhang, M.Zhang, X.Zhang, Y.Zhang, Y.Zhang, Z.Zhang, M.Zhao, L.Zhou, K.Zhu, J.Zhang Determination of the 232Th(n, γ) cross section from 10 to 200 keV at the Back-n facility at CSNS NUCLEAR REACTIONS 232Th, 197Au(n, γ), E=10-200 keV; measured reaction products, En, In, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, CENDL-3.2, JENDL-5 libraries and TALYS 1.96 calculations. The back-streaming white neutron beam-line (Back-n) of China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-023-01126-0
2022HE15 Phys.Rev. C 106, 044904 (2022) Y.He, W.Chen, T.Luo, S.Cao, L.-G.Pang, X.-N.Wang Event-by-event jet anisotropy and hard-soft tomography of the quark-gluon plasma
doi: 10.1103/PhysRevC.106.044904
2022HU12 Phys.Lett. B 834, 137484 (2022) M.H.Huang, Z.G.Gan, Z.Y.Zhang, L.Ma, J.G.Wang, M.M.Zhang, H.B.Yang, C.L.Yang, X.Y.Huang, Z.Zhao, S.Y.Xu, L.X.Chen, X.J.Wen, Y.F.Niu, C.X.Yuan, Y.L.Tian, Y.S.Wang, J.Y.Wang, M.L.Liu, Y.H.Qiang, W.Q.Yang, H.B.Zhang, Z.W.Lu, S.Guo, W.X.Huang, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α decay of the new isotope 204Ac RADIOACTIVITY 204,205Ac(α) [from 169Tm(40Ca, xn), E=202, 210, 212, 214 MeV using SHANS2 separator at CAFE2 and SHANS separator at HRIFL, Lanzhou accelerator facility]; 200Fr, 196At(α) [from 204Ac α-decay chain]; measured evaporation residues (ERs), Eα, (ER)α-α-α correlated events, production cross sections, T1/2 of decays using two multiwire proportional counters for implanted events, double-sided silicon strip detectors (DSSSDs) for α particles, and a segmented clover Ge detector for γ radiation. 204,205Ac, 200Fr, 196At; deduced T1/2 of decays of ground-state decays, and Eα values, reduced α-width in Rasmussen formalism, favored α decay for 204Ac decay. 204Ac(p); no proton decay events observed. 201,201m,202,202m,203,204,205Fr, 204,205,206Ra(α); observed α spectra, (ERs)-α-α-correlated events. Comparison with previous available experimental results. Systematics of experimental and theoretical T1/2 and Q(α) values for 196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211At, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Fr, 203,204,205,206,207,208,209,210,211,212,213,214,215Ac, 211,212,213,214,215,216,217Pa, using Hartree-Fock-BCS (HFBSC) method, and macroscopic-microscopic (MM) mass formula for theory.
doi: 10.1016/j.physletb.2022.137484
2022ZH04 Phys.Rev. C 105, 014604 (2022) D.Zhang, Y.Li, J.Bao, C.Fu, M.Guan, Y.He, X.Ji, H.Jia, Y.Li, J.Liu, J.Xia, W.Xiong, J.You, C.Yuan, N.Zhou 83Rb/83mKr production and cross-section measurement with 3.4 MeV and 20 MeV proton beams NUCLEAR REACTIONS Kr(p, n)83Rb/84Rb/86Rb, E=3.4 MeV beam from China Institute of Atomic Energy; Kr(p, n), E=20 MeV beam from Institute of Modern Physics; measured Eγ, Iγ, total generated radioactivities and thick-target yields for rubidium isotope. 83mKr/83Rb; measured production rate of 83mKr from 83Rb decay; produced 83mKr yielded enough statistics for detector calibration injected into the PandaX-II liquid xenon detector for dark matter studies. Relevance to calibration source such as short half-life 83mKr for liquid xenon or liquid argon detectors in experiments dealing with search for dark matter.
doi: 10.1103/PhysRevC.105.014604
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
2021CH41 Phys.Rev.Lett. 127, 082301 (2021) W.Chen, Z.Yang, Y.He, W.Ke, L.-G.Pang, X.-N.Wang Search for the Elusive Jet-Induced Diffusion Wake in Z/γ-Jets with 2D Jet Tomography in High-Energy Heavy-Ion Collisions
doi: 10.1103/PhysRevLett.127.082301
2021HE05 Nucl.Phys. A1005, 122032 (2021) Y.He, S.Cao, W.Chen, T.Luo, L.-G.Pang, X.-N.Wang Interplaying mechanisms behind inclusive jet RAA and extraction of jet energy loss distributions
doi: 10.1016/j.nuclphysa.2020.122032
2021HE08 Chin.Phys.C 45, 014106 (2021) Y.Q.He, J.K.Ge, G.J.Fu, H.Jiang Isospin dependence of the nuclear binding energy NUCLEAR STRUCTURE A>15; analyzed available data; deduced symmetry energy and the Wigner energy in the binding energy formula for atomic nuclei.
doi: 10.1088/1674-1137/abc23d
2021HE09 Chin.Phys.C 45, 014110 (2021) Improved empirical formula for α particle preformation factor RADIOACTIVITY 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220Po, 191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221At, 194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226Rn, 206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225Ac, 209Th, 224,225,226,227,228,229,230,231,232Th, 217,218,219,220,221,222,223,224,225,226,227,228,229,230,231Pa, 219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238U, 229,230,231,232,233,234,235,236,237,238,239,240,241,242,243Am, 233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250Cm, 245,247Bk, 237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255Cf, 246,247,248,249,250,251,252,253,254,255Es, 244,245,246,247,248,249,250,251,252,253,254,255,256,257Fm, 247,248,249,250,251,252,253,254,255,256,257Md, 251,252,253,254,255,256,257,258No, 253,255,257,259Lr(α); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/abc684
2021HU29 Chin.Phys.C 45, 114104 (2021) D.-Y.Huo, X.Yang, C.Han, C.-Q.Liu, K.Wu, X.-Y.Liu, C.Huang, Q.Xie, Y.He, X.J.Bao Evaluation of pre-neutron-emission mass distributions of neutron-induced typical actinide fission using scission point model NUCLEAR REACTIONS 235,238U, 237Np, 239Pu, 232Th(n, F), E=0.5, 1.08, 2.02, 3.51, 5.04, 15.50 MeV; analyzed available data; calculated pre-neutron-emission mass distributions.
doi: 10.1088/1674-1137/ac2298
2021LI35 Eur.Phys.J. A 57, 232 (2021); Erratum Eur.Phys.J. A 57, 252 (2021) X.Liu, Y.Yang, R.Liu, Z.Wen, J.Wen, Z.Han, Y.Chen, H.Jing, H.Yi, J.Bao, Z.Ren, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS NUCLEAR REACTIONS 27Al(n, X), E<20 MeV; measured reaction products, En, In; deduced neutron transmission, total σ and uncertainties. Comparison withENDF/B-VIII.0, JEFF-3.3 and CENDL-3.2 library evaluations, EXFOR compilations. Spallation Neutron Source Science Center.
doi: 10.1140/epja/s10050-021-00513-9
2021PA28 Eur.Phys.J. A 57, 218 (2021) F.Pan, Y.He, A.Li, Y.Wang, Y.Wu, J.P.Draayer Extended Heine-Stieltjes polynomials related to the isovector pairing model
doi: 10.1140/epja/s10050-021-00535-3
2021RE01 Nucl.Instrum.Methods Phys.Res. A985, 164703 (2021) J.Ren, X.Ruan, W.Jiang, J.Bao, G.Luan, Q.Zhang, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, Z.Cui, R.Fan, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, Q.Mu, C.Ning, B.Qi, Z.Ren, Y.Song, Z.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Background study for (n, γ) cross section measurements with C6D6 detectors at CSNS Back-n NUCLEAR REACTIONS 197Au, Pb, C, 181Ta, 59Co(n, γ), E<400 MeV; measured reaction products, Eγ, Iγ; deduced σ.
doi: 10.1016/j.nima.2020.164703
2020BA03 Chin.Phys.C 44, 014003 (2020) H.Bai, R.Fan, H.Jiang, Z.Cui, Y.Hu, G.Zhang, Z.Chen, W.Jiang, H.Yi, J.Tang, L.Zhou, Q.An, J.Bao, P.Cao, Q.Chen, Y.Chen, P.Cheng, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the differential cross sections and angle-integrated cross sections of the 6Li(n, t)4He reaction from 1.0 eV to 3.0 MeV at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), E=0.000001-3 MeV; measured reaction products; deduced σ. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries, experimental data.
doi: 10.1088/1674-1137/44/1/014003
2020HE13 Eur.Phys.J. A 56, 123 (2020) Particle productions and anisotropic flows from the AMPT model for Cu+Au collisions at √ sNN = 200 Gev
doi: 10.1140/epja/s10050-020-00128-6
2020HE21 Phys.Rev.Lett. 125, 122301 (2020) Gradient Tomography of Jet Quenching in Heavy-Ion Collisions
doi: 10.1103/PhysRevLett.125.122301
2020JI06 Nucl.Instrum.Methods Phys.Res. A973, 164126 (2020) W.Jiang, H.Bai, H.Jiang, H.Yi, R.Fan, G.Zhang, J.Tang, Z.Sun, C.Ning, K.Sun, K.Gao, Z.Cui, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Y.Song, Z.Song, H.Sun, X.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Application of a silicon detector array in (n, lcp) reaction cross-section measurements at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), 10B(n, α), E<1 MeV; measured reaction products, En, In; deduced σ. Comparison with experimental data, ENDF/B-VIII.0, JEFF-3.3, ROSFOND evaluated libraries.
doi: 10.1016/j.nima.2020.164126
2020LI33 Nucl.Instrum.Methods Phys.Res. A980, 164506 (2020) Q.Li, H.Jing, B.Zhou, C.Ning, J.Tang, J.Ren, H.Yi, X.Zhu, L.Zhang, W.Jiang, R.Fan, J.Bao, C.Feng, X.Ruan, Y.Chen, L.Zhou, Y.Li, Z.Tan, Y.Chen, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, L.Kang, M.Kang, B.Li, L.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, B.Qi, Z.Song, H.Sun, X.Sun, Z.Sun, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron and γ background measurements of the experimental halls at the CSNS back-streaming white neutron source
doi: 10.1016/j.nima.2020.164506
2020PA38 Phys.Rev. C 102, 044306 (2020) F.Pan, Y.He, Y.Wu, Y.Wang, K.D.Launey, J.P.Draayer Neutron-proton pairing correction in the extended isovector and isoscalar pairing model NUCLEAR STRUCTURE 18,20,22O, 18,20F, 18,20,22,24Ne, 20,22,24Na, 20,22,24,26Mg, 22,24,26,28Si, 24,26Al; calculated binding energies, energies of 0+ states with isospin T=1-3, isovector np, nn, and pp pairing contributions to the binding energies. Extended isovector and isoscalar pairing model. Comparison with experimental values.
doi: 10.1103/PhysRevC.102.044306
2020RE11 Phys.Rev. C 102, 034604 (2020) Z.Ren, Y.Yang, J.Wen, H.Guo, Z.Wen, R.Liu, Z.Han, W.Sun, X.Liu, Q.Chen, T.Ye, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the 236U(n, f) cross section for neutron energies from 0.4 MeV to 40 MeV from the back-streaming white neutron beam at the China Spallation Neutron Source NUCLEAR REACTIONS 235,236U(n, F), E AP 0.4-40 MeV beam from the China Spallation Neutron Source (CSNS)-Back-streaming white neutron source (WNS); measured fission fragments, energy spectra, time-of-flight using Fast Ionization Chamber Spectrometer; deduced 236U(n, F)/235U(n, F) cross section ratios. Comparison with theoretical calculation using the UNF code, and with evaluated data in JENDL-4.0, CENDL-3.1, and ENDF/B-VIII.0 libraries.
doi: 10.1103/PhysRevC.102.034604
2020WE04 Ann.Nucl.Energy 140, 107301 (2020) J.Wen, Y.Yang, Z.Wen, R.Liu, X.Liu, Z.Han, Q.Chen, Z.Ren, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the U-238/U-235 fission cross section ratio at CSNS - Back-in WNS NUCLEAR REACTIONS 235,238U(n, F), E=1-20 MeV; measured reaction products, fission fragments, Eγ, Iγ; deduced neutron resonances, σ. Comparison with ENDF/B-VIII.0 library evaluations.
doi: 10.1016/j.anucene.2019.107301
2019CH37 Eur.Phys.J. A 55, 115 (2019), Erratum Eur.Phys.J. A 55, 145 (2019) Y.Chen, G.Luan, J.Bao, H.Jing, L.Zhang, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, Ch.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron energy spectrum measurement of the Back-n white neutron source at CSNS
doi: 10.1140/epja/i2019-12808-1
2019HE01 Nucl.Phys. A982, 635c (2019) Y.He, S.Cao, W.Wei, T.Luo, L.-G.Pang, X.N.Wang E-by-e jet suppression, anisotropy, medium response and hard-soft tomography NUCLEAR REACTIONS 1H(p, γ), E at σNN=2.76 TeV;208Pb(208Pb, γ), E at σNN=2.76 TeV; measured γ-jets; deduced γ-jets distribution vs transverse momentum, azimuthal anisotropy of hard jets vs elliptic flow of bulk hadrons, suppression factor vs transverse momentum; calculated γ-jets distribution vs transverse momentum using Linear Boltzmann Transport (LBT) model with interaction in Quark-Gluon Plasma (QGP). Compared also with published data from PHENIX and STAR and the suppression factor with ATLAS data.
doi: 10.1016/j.nuclphysa.2018.11.023
2019HE09 Phys.Rev. C 99, 054911 (2019) Y.He, S.Cao, W.Chen, T.Luo, L.-G.Pang, X.-N.Wang Interplaying mechanisms behind single inclusive jet suppression in heavy-ion collisions
doi: 10.1103/PhysRevC.99.054911
2019HE13 Phys.Rev.Lett. 122, 252302 (2019) Bayesian Extraction of Jet Energy Loss Distributions in Heavy-Ion Collisions
doi: 10.1103/PhysRevLett.122.252302
2019JI07 Chin.Phys.C 43, 124002 (2019) H.Jiang, W.Jiang, H.Bai, Z.Cui, G.Zhang, R.Fan, H.Yi, C.Ning, L.Zhou, J.Tang, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Z.Song, Y.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurements of differential and angle-integrated cross sections for the 10B(n, α)7Li reaction in the neutron energy range from 1.0 eV to 2.5 MeV NUCLEAR REACTIONS 10B(n, α), E=0.000001-2.5 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ and uncertainties. Comparison with ENDF/B-VIII.0, JEFF-3.3, CENDL-3.1 and JENDL 4.0 libraries.
doi: 10.1088/1674-1137/43/12/124002
2019PA15 Nucl.Phys. A984, 68 (2019) F.Pan, S.Yuan, Y.He, Y.Zhang, S.Yang, J.P.Draayer An exact solution of spherical mean-field plus orbit-dependent non-separable pairing model with two non-degenerate j-orbits
doi: 10.1016/j.nuclphysa.2019.01.005
2019PA38 Chin.Phys.C 43, 074106 (2019) F.Pan, D.Zhou, S.Yang, G.Sargsyan, Y.He, K.D.Launey, J.P.Draayer A close look at the competition of isovector and isoscalar pairing in A=18 and 20 even-even N ≈ Z nuclei NUCLEAR STRUCTURE 18,20O, 18,20F, 18,20Ne, 20Na; calculated energy levels, J, π using using the mean-field plus dynamic QQ, pairing and particle-hole interaction model.
doi: 10.1088/1674-1137/43/7/074106
2019WA13 Chin.Phys.C 43, 054101 (2019) H-K.Wang, Z.-H.Li, C.-X.Yuan, Z.-Q.Chen, N.Wang, W.Qin, Y.-Q.He Monopole effects, core excitations, and β decay in the A = 130 hole nuclei near 132Sn NUCLEAR STRUCTURE 130In, 130Sn, 130Cd; calculated energy levels, J, π. RADIOACTIVITY 130In, 130Sn, 130Cd(β-); calculated Gamow-Teller transition probability (B(GT)).
doi: 10.1088/1674-1137/43/5/054101
2018WA34 Yuan.Wul.Ping. 35, 445 (2018); Nucl.Phys.Rev. 35, 445 (2018) Y.Wang, J.Su, Z.Han, B.Tang, B.Cui, T.Ge, Y.Lu, Z.Chen, B.Guo, X.Li, Y.Li, Z.Li, G.Lian, T.Ma, Y.Ma, Y.Shen, Y.Su, C.Wang, H.Wu, S.Yan, S.Zeng, Y.Zheng, C.Zhou, Y.Dang, G.Fu, Y.He, F.Liu, D.Wu, T.Zhang, W.Liu, for the BRIF collaboration Study of the Exotic Decay Mode of 20Na with an Intense ISOL Beam RADIOACTIVITY 20Na(β+α) [from 24Mg(p, nα), E<100 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced γ-ray energies and intensities, exotic β-γ-α decay mode.
doi: 10.11804/NuclPhysRev.35.04.445
2017CA27 Nucl.Phys. A967, 628 (2017) S.Cao, T.Luo, Y.He, G.-Y.Qin, X.-N.Wang Heavy and light hadron production and D-hadron correlation in relativistic heavy-ion collisions
doi: 10.1016/j.nuclphysa.2017.05.086
2017HE13 Phys.Rev. C 96, 014910 (2017) Improved quark coalescence for a multi-phase transport model
doi: 10.1103/PhysRevC.96.014910
2017WA03 Phys.Rev. C 95, 011304 (2017) H.-K.Wang, K.Kaneko, Y.Sun, Y.-Q.He, S.-F.Li, J.Li Monopole effects, isomeric states, and cross-shell excitations in the A=129 hole nuclei near 132Sn NUCLEAR STRUCTURE 129Sn, 129In, 129Cd; calculated levels, J, π, predicted cross-shell excited states, monopole effect on the ground-state energies, configurations. Large-scale shell-model calculations for A=129 hole nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.011304
2017YA17 Phys.Rev. C 95, 064307 (2017) T.Ya, Y.He, Z.-C.Gao, J.-Q.Wang, Y.S.Chen Implementation of the variation-after-projection approach in calculations with a time-odd Hartree-Fock mean field NUCLEAR STRUCTURE 24,25,26Mg, 26Al; calculated variation-after-projection (VAP) energies, B(E2), J-scheme shell model dimension; deduced energy differences between the shell model energies and the present VAP energies. 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated VAP energies, and compared with previous VAP calculations and shell-model energies for the ground states of even-even nuclei. Time-odd Hartree-Fock (HF) mean field with Slater determinants.
doi: 10.1103/PhysRevC.95.064307
2016LU11 Nucl.Phys. A956, 585 (2016) T.Luo, Y.He, E.Wang, X.-N.Wang Modification of reconstructed gamma-jets in heavy-ion collisions
doi: 10.1016/j.nuclphysa.2016.04.007
2015HE15 Phys.Rev. C 91, 054908 (2015); Erratum Phys.Rev. C 97, 019902 (2018) Linear Boltzmann transport for jet propagation in the quark-gluon plasma: Elastic processes and medium recoil
doi: 10.1103/PhysRevC.91.054908
2014LU14 Nucl.Phys. A932, 99c (2014) Jet propagation within a Linearized Boltzmann Transport model
doi: 10.1016/j.nuclphysa.2014.09.052
2013YA11 Phys.Rev. C 88, 014312 (2013) T.Yang, R.Ze, H.Wu, T.Jiang, Y.He Search for induced emission from the 178Hfm2 isomer by low-energy x rays NUCLEAR REACTIONS 178mHf(γ, γ'), E=20.825 keV x rays, [31-year, 16+ isomer of 178Hf in 176Yb(α, 2n), followed by chemical separation]; measured Eγ, Iγ at the SSRF facility in China; deduced no enhancement in γ-ray intensity of 426-, 495-, and 574-keV γ rays from the decay of 31-y isomer of 178Hf. Search for induced emission from 31-y isomer of 178Hf by x rays proved negative. RADIOACTIVITY 172Lu, 175Hf(EC), 175mHf(IT); measured Eγ, Iγ.
doi: 10.1103/PhysRevC.88.014312
2013ZH24 Nucl.Phys. A904-905, 799c (2013) Jet probes of QCD matter: Single jets and dijets in heavy-ion collisions
doi: 10.1016/j.nuclphysa.2013.02.137
2013ZH44 Nucl.Phys. 910-911, 256c (2013) B.-W.Zhang, Y.He, R.B.Neufeld, I.Vitev, E.Wang Probing nuclear matter with jets
doi: 10.1016/j.nuclphysa.2012.12.113
2012FA06 Appl.Radiat.Isot. 70, 2295 (2012) Measurement of fission cross section for 232Th(n, x)89Rb reaction induced by neutrons around 14 MeV NUCLEAR REACTIONS 232Th(n, x)89Rb, 90Zr, 93Nb(n, 2n), E≈14 MeV; measured fission products, Eγ, Iγ; deduced σ and its uncertainties. Comparison with available data.
doi: 10.1016/j.apradiso.2012.06.006
2012YA17 Eur.Phys.J. A 48, 149 (2012) T.Yang, TaoJiang, R.Ze, H.Wu, Y.He, J.Yang, C.Yang Preparation of the 178m2Hf isomer used in the induced gamma decay experiment by X-ray from synchrotron radiation facility NUCLEAR REACTIONS 176Yb(α, 2n)178m2Hf, (α, X), E≈27 MeV; measured Eγ, Iγ after cooling using HPGe; deduced isomeric state (after radiochemical separation).
doi: 10.1140/epja/i2012-12149-7
2009GU05 Nucl.Phys. A823, 83 (2009) Relativistic BCS-BEC crossover of a two-species Fermi gas with number density asymmetry at zero temperature
doi: 10.1016/j.nuclphysa.2009.03.003
2007LI04 Chin.Phys.Lett. 24, 494 (2007) H.-J.Liu, Z-J.Zheng, Y.-Q.Gu, B.-H.Zhang, Y.-J.Rhee, S.-M.Nam, J.-M.Han, Y.-W.Rhee, K.-H.Yea, J.-B.Chen, H.-B.Wang, C.-Y.Jiao, Y.-L.He, T.-S.Wen, X.-L.Wen, M.Chen Deuterium Cluster Fusion Induced by the Intense Femtosecond Laser Pulse NUCLEAR REACTIONS 2H(d, n), E not given; measured neutron spectra, yields. Cluster fusion Induced by femtosecond laser pulse.
doi: 10.1088/0256-307X/24/2/053
2000HE02 Phys.Lett. 477B, 93 (2000) Y.B.He, J.Hufner, B.Z.Kopeliovich J/ψ and ψ' Total Cross Sections and Formation Times from Data for Cross Sections and Formation Times from Data for Chromonium Suppression in pA Collisions NUCLEAR REACTIONS Be, W(p, X), E=800 GeV; analyzed charmonium yields; deduced charmonium-nucleon cross sections.
doi: 10.1016/S0370-2693(00)00198-2
2000HU05 Eur.Phys.J. A 7, 239 (2000) J.Hufner, Y.B.He, B.Z.Kopeliovich Charmonium Suppression by Gluon Bremsstrahlung in p-A and A-B Collisions NUCLEAR REACTIONS S(U, X), E at 200 GeV/c; Pb(Pb, X), E at 158 GeV/c; calculated J/ψ production σ, ratio of J/ψ and ψ' to Drell-Yan σ; deduced supresmechanism features. Comparison with data.
doi: 10.1007/s100500050387
1999HE13 Eur.Phys.J. A 5, 111 (1999) The Effect of Hadronization on the Instabilities in an Expanding Parton Plasma
doi: 10.1007/s100500050264
1998BO13 Phys.Rev. C57, 3263 (1998) Transport Theory with Self-Consistent Confinement Related to the Lattice Data
doi: 10.1103/PhysRevC.57.3263
1998HE09 Nucl.Phys. A630, 719 (1998) Y.B.He, J.Hufner, S.P.Klevansky, P.Rehberg ππ Scattering in the ρ-Meson Channel at Finite Temperature
doi: 10.1016/S0375-9474(97)00807-5
1997HE18 Phys.Rev.Lett. 79, 3134 (1997) Search for a Dirac Magnetic Monopole in High Energy Nucleus-Nucleus Collisions NUCLEAR REACTIONS Pb(197Au, X), E=11 GeV/nucleon; Pb(208Pb, X), E=160 GeV/nucleon; measured magnetic monopole production σ upper limit vs mass. BP-1 glass plate detectors.
doi: 10.1103/PhysRevLett.79.3134
1997WA33 Nuovo Cim. 110A, 599 (1997) Probability Description of Final-State Distribution in Independent Fragmentation Model
1996HE08 Phys.Rev. C53, 1903 (1996) Y.B.He, C.S.Gao, X.Q.Li, W.Q.Chao Properties of Strangelets at Finite Temperature in the Liquid Drop Model
doi: 10.1103/PhysRevC.53.1903
1996HE12 Phys.Rev. C54, 857 (1996) Y.B.He, W.Q.Chao, C.S.Gao, X.Q.Li Cold Strangelets Formation with Finite Size Effects in High Energy Heavy-Ion Collisions
doi: 10.1103/PhysRevC.54.857
1995HE38 Nucl.Instrum.Methods Phys.Res. B95, 225 (1995) Enhancing the Sensitivity of CR-39 Detectors to Relativistic Ions by Etching in Potassium and Sodium Hydroxides
doi: 10.1016/0168-583X(94)00541-9
1995SO26 Nucl.Instrum.Methods Phys.Res. B100, 188 (1995) Dependence of CR-39 Etch Rates on Concentration of Etched Products in Sodium Hydroxide Etchant
doi: 10.1016/0168-583X(95)00484-X
1994HE07 Nucl.Instrum.Methods Phys.Res. B84, 67 (1994) Y.D.He, A.J.Westphal, P.B.Price Response of the BP-1 Phosphate Glass Detector to Relativistic Heavy Ions
doi: 10.1016/0168-583X(94)95705-3
1994HE16 Z.Phys. A348, 105 (1994) Nuclear and Electromagnetic Fragmentation of 2.25-TeV 197Au Nuclei
doi: 10.1007/BF01289597
1994ZH24 J.Phys.(London) G20, 1383 (1994) Q.Q.Zhu, L.K.Ding, G.J.Wang, Y.D.He A Monte Carlo Model for Diffractive Dissociation in Hadron-Hadron Collisions at High Energies NUCLEAR REACTIONS 1H(π+, X), E=high; analyzed diffractive meson dissociation multiplicity distributions. Monte Carlo model, other reactions, other aspects included.
doi: 10.1088/0954-3899/20/9/007
1993PA07 J.Phys.(London) G19, 861 (1993) E.S.Paul, S.Davis, P.Vaska, P.J.Bishop, S.A.Forbes, D.B.Fossan, Y.-J.He, J.R.Hughes, I.Jenkins, Y.Liang, R.Ma, M.S.Metcalfe, S.M.Mullins, P.J.Nolan, R.J.Poynter, P.H.Regan, R.Wadsworth, N.Xu Prolate and Oblate Rotational Bands in 136Sm NUCLEAR REACTIONS 92Mo(50Cr, 2pα), E=220 MeV; measured γγ-coin, γγ(θ), Iγ ratios. 136Sm deduced levels, J, π, rotational bands. Other data input. NUCLEAR STRUCTURE 134,136,138Sm; calculated total Routhian surface, alignments, dynamic moments of inertia. Cranked Woods-Saxon model.
doi: 10.1088/0954-3899/19/6/007
1992HE03 J.Phys.(London) G18, 99 (1992) Y.He, M.J.Godfrey, I.Jenkins, A.J.Kirwan, S.M.Mullins, P.J.Nolan, E.S.Paul, R.Wadsworth Rotational Band Structures in 129La NUCLEAR REACTIONS 51V(82Se, 4n), E=290 MeV; measured γγ-coin, Iγ, DCO ratios. 129La deduced levels, J, π, B(λ) ratios, band structure, configurations. Cranked shell model.
doi: 10.1088/0954-3899/18/1/009
1992MU09 Phys.Rev. C45, 2683 (1992) S.M.Mullins, I.Jenkins, Y.-J.He, A.J.Kirwan, P.J.Nolan, J.R.Hughes, R.Wadsworth, R.A.Wyss Second Minimum Lifetime Measurements in 133Nd and 137Nd NUCLEAR REACTIONS 105Pd(32S, 2n2p), E=152 MeV; 104Ru(36S, 3n), E=145 MeV; measured γγ-coin, DSA, centroid shifts. 133,137Nd deduced levels, T1/2, deformed band quadrupole moments. Total Routhian surface calculations.
doi: 10.1103/PhysRevC.45.2683
1992RE05 J.Phys.(London) G18, 847 (1992) P.H.Regan, R.Wadsworth, S.M.Mullins, J.Nyberg, A.Atac, S.A.Forbes, D.B.Fossan, Y.-J.He, J.R.Hughes, I.Jenkins, R.Ma, M.S.Metcalfe, P.J.Nolan, E.S.Paul, R.J.Poynter, D.Santonicio, A.Virtanen, N.Xu Measurement of the Intrinsic Quadrupole Moments in the νi13/2 Bands of 135,137Sm NUCLEAR REACTIONS 92Mo(46Ti, n2p), E=210 MeV; 104Pd(37Cl, 3np), E=168 MeV; measured γγ-coin, DSA. 137Sm deduced levels, J, π, T1/2, deformation parameter β2, quadrupole moments, band structure. 135Sm deduced levels, J, π, T1/2, deformation parameter β2, quadrupole moments, band structure, superdeformation features.
doi: 10.1088/0954-3899/18/5/013
1991MU08 Phys.Rev.Lett. 66, 1677 (1991) S.M.Mullins, R.A.Wyss, P.Fallon, T.Byrski, D.Curien, S.A.Forbes, Y.-J.He, M.S.Metcalfe, P.J.Nolan, E.S.Paul, R.J.Poynter, P.H.Regan, R.Wadsworth Superdeformation and Double Blocking in 142Eu NUCLEAR REACTIONS 110Pd(37Cl, 5n), E=160 MeV; measured γγ-coin sum spectra. 142Eu deduced levels, superdeformed band.
doi: 10.1103/PhysRevLett.66.1677
1991RE03 Nucl.Phys. A533, 476 (1991) P.H.Regan, R.Wadsworth, J.R.Hughes, G.J.Gyapong, W.Gelletly, M.J.Godfrey, I.Jenkins, Y.-J.He, S.M.Mullins, P.J.Nolan, J.Simpson, B.J.Varley, D.L.Watson Spectroscopy of the Light Rare-Earth Nuclei 133Pm and 133Sm: Configuration-dependent pairing and evidence for strong residual proton-neutron interactions in neighbouring odd-N and odd-Z nuclei NUCLEAR REACTIONS 96Ru(40Ca, 2np), (40Ca, 3p), E=180 MeV; measured Iγ, Eγ. 133Sm, 133Pm levels deduced J, π, configurations.
doi: 10.1016/0375-9474(91)90529-F
1990HE12 J.Phys.(London) G16, 657 (1990) Y.He, M.J.Godfrey, I.Jenkins, A.J.Kirwan, P.J.Nolan, S.M.Mullins, R.Wadsworth, D.J.G.Love Quadrupole Moment of the Superdeformed Band in 131Ce NUCLEAR REACTIONS 100Mo(36S, 5n), E=155 MeV; measured γγ-coin, DSA. 131Ce deduced levels, J, π, mean T1/2, β2, superdeformed intrinsic quadrupole moment, band structure.
doi: 10.1088/0954-3899/16/4/016
1990MA53 J.Phys.(London) G16, 1233 (1990) R.Ma, D.B.Fossan, E.S.Paul, N.Xu, R.J.Poynter, P.H.Regan, R.Wadsworth, Y.-J.He, I.Jenkins, M.S.Metcalfe, S.M.Mullins, P.J.Nolan An i13/2 Intruder Band in 139Gd NUCLEAR REACTIONS 92Mo(50Cr, n2p), E=220 MeV; measured γγ(θ), oriented nuclei. 139Gd deduced levels, J, π, band structure.
doi: 10.1088/0954-3899/16/8/019
1990RE12 Phys.Rev. C42, R1805 (1990) P.H.Regan, R.Wyss, R.Wadsworth, D.B.Fossan, Y.-J.He, J.R.Hughes, I.Jenkins, R.Ma, M.S.Metcalfe, S.M.Mullins, P.J.Nolan, E.S.Paul, R.J.Poynter, N.Xu Lifetime Measurements in 135Sm: Large deformation in the N = 6 intruder band and evidence for quenched proton pairing NUCLEAR REACTIONS 92Mo(46Ti, n2p), E=210 MeV; measured γ-spectra, DSA. 135Sm levels deduced T1/2, deformed band quadrupole moment.
doi: 10.1103/PhysRevC.42.R1805
1989GO04 J.Phys.(London) G15, 487 (1989) M.J.Godfrey, Y.He, I.Jenkins, A.Kirwan, P.J.Nolan, D.J.Thornley, S.M.Mullins, R.Wadsworth The Competition between Collective and Single Particle Behaviour in the Odd-Odd Isotopes 128,130La NUCLEAR REACTIONS 95Mo(36S, 2np), E=135, 145 MeV; 54Cr(78Se, 3np), E not given; 51V(82Se, 3n), E=290 MeV; measured E(γ), I(γ), γγ-coin. 115In(16O, 3n), E=68 MeV; measured σ(θ(residual)), γγ-coin. 128,130La deduced levels, J, π, relative I(γ), branching ratio, B(M1)/B(E2).
doi: 10.1088/0954-3899/15/4/012
1989GO06 J.Phys.(London) G15, 671 (1989) M.J.Godfrey, Y.He, I.Jenkins, A.Kirwan, P.J.Nolan, D.J.Thornley, S.M.Mullins, R.Wadsworth, R.A.Wyss Collective Oblate Structure in the Odd-Odd Isotopes 128,130La NUCLEAR REACTIONS 95Mo(36S, 2np), E=135, 145 MeV; measured γγ-coin. 115In(16O, 3n), E=68 MeV; measured γ(θ). 51V(82Se, 3n), E=290 MeV; measured γγ-coin, γ-spectra. 128,130La deduced levels, J, π, γ-branching, B(λ) ratios.
doi: 10.1088/0954-3899/15/5/019
1989GO13 J.Phys.(London) G15, L163 (1989) M.J.Godfrey, Y.He, I.Jenkins, A.Kirwan, P.J.Nolan, R.Wadsworth, S.M.Mullins The Proton Structure of the Superdeformed Bands in the N = 73 Isotones 130La, 131Ce and 133Nd NUCLEAR REACTIONS 51V(82Se, 3n), E=290 MeV; measured γγ-coin. 130La deduced levels, superdeformed band structure, shape features, moments of inertia.
doi: 10.1088/0954-3899/15/8/004
1989HU02 J.Labelled Compd.Radiopharm. 26, 168 (1989) I.Huszar, He Youfeng, J.Jegge, R.Weinreich Development of a Production Process for 82Sr NUCLEAR REACTIONS Rb(p, xnyp)82Sr, E=72 MeV; measured residual production yield.
1989WA20 Z.Phys. A333, 409 (1989) R.Wadsworth, P.Regan, S.M.Mullins, G.J.Gyapong, D.L.Watson, P.J.Nolan, M.J.Godfrey, I.Jenkins, Y.J.He, B.J.Varley, W.Gelletly, J.Simpson Evidence for an i13/2 Neutron Band in 133Sm NUCLEAR REACTIONS 96Ru(40Ca, n2p), E=195 MeV; measured γγ-, nγ-, nnγ-coin. 133Sm deduced levels, J, π, band structure.
1989WA21 Z.Phys. A333, 411 (1989) R.Wadsworth, P.Regan, S.M.Mullins, G.J.Gyapong, D.L.Watson, P.J.Nolan, M.J.Godfrey, I.Jenkins, Y.J.He, B.J.Varley, J.Simpson, W.Gelletly Yrast Band Spectroscopy of 132Sm and 130Nd NUCLEAR REACTIONS 96Ru(40Ca, 2n2p), 96Ru(40Ca, 2pα), E=195 MeV; measured γγ-, nγ-, nnγ-coin. 130Nd, 132Sm deduced levels, J, π, band structure.
1986HE08 Phys.Lett. 168B, 177 (1986) Nucleon Core Size and Nuclear Forces NUCLEAR STRUCTURE 1n, 1H; calculated rms radius, nucleon quark core size.
doi: 10.1016/0370-2693(86)90959-7
1982BL24 J.Labelled Compd.Radiopharm. 19, 1431 (1982) G.Blessing, K.Suzuki, He Youfeng, S.M.Qaim, G.Stocklin Production of High-Purity 77Kr NUCLEAR REACTIONS, ICPND 77Se(3He, 3n), E=22-36 MeV; measured production σ(E). Metallic target, activation technique.
1982HE01 Int.J.Appl.Radiat.Isotop. 33, 13 (1982) He Youfeng, S.M.Qaim, G.Stocklin Excitation Functions for 3He-Particle Induced Nuclear Reactions on 76Se, 77Se and (nat)Se: Possibilities of production of 77Kr NUCLEAR REACTIONS 76Se(3He, xnyp), E=threshold-36 MeV; measured σ(E) for x=2, 3, y=0; 77Se, Se(3He, xn), E=threshold-36 MeV; measured production σ(E) for 76,77,79Kr; 76Se(3He, α), E=10-36 MeV; measured σ(E); 77,76Se(3He, xnyp), E=threshold-36 MeV; measured σ(E) for x=1, 2, 3, y=1; 77Se(3He, nα), E=14-36 MeV; measured σ(E). Activation, stacked foil techniques. Cumulative yield calculations.
doi: 10.1016/0020-708X(82)90199-5
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