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NSR database version of April 24, 2024.

Search: Author = Y.He

Found 83 matches.

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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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
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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
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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
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2021HE09      Chin.Phys.C 45, 014110 (2021)

Y.He, X.Yu, H.-F.Zhang

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32800.


2020HE13      Eur.Phys.J. A 56, 123 (2020)

Y.He, Z.-W.Lin

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
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2020HE21      Phys.Rev.Lett. 125, 122301 (2020)

Y.He, L.-G.Pang, X.-N.Wang

Gradient Tomography of Jet Quenching in Heavy-Ion Collisions

doi: 10.1103/PhysRevLett.125.122301
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32811.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32798.


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
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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
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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
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2019HE13      Phys.Rev.Lett. 122, 252302 (2019)

Y.He, L.-G.Pang, X.-N.Wang

Bayesian Extraction of Jet Energy Loss Distributions in Heavy-Ion Collisions

doi: 10.1103/PhysRevLett.122.252302
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32804.


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
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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
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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
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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
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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
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2017HE13      Phys.Rev. C 96, 014910 (2017)

Y.He, Z.-W.Lin

Improved quark coalescence for a multi-phase transport model

doi: 10.1103/PhysRevC.96.014910
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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
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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
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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
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2015HE15      Phys.Rev. C 91, 054908 (2015); Erratum Phys.Rev. C 97, 019902 (2018)

Y.He, T.Luo, X.-N.Wang, Y.Zhu

Linear Boltzmann transport for jet propagation in the quark-gluon plasma: Elastic processes and medium recoil

doi: 10.1103/PhysRevC.91.054908
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2014LU14      Nucl.Phys. A932, 99c (2014)

T.Luo, Y.He, X.-N.Wang, Y.Zhu

Jet propagation within a Linearized Boltzmann Transport model

doi: 10.1016/j.nuclphysa.2014.09.052
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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
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2013ZH24      Nucl.Phys. A904-905, 799c (2013)

B.-W.Zhang, Y.He, E.Wang

Jet probes of QCD matter: Single jets and dijets in heavy-ion collisions

doi: 10.1016/j.nuclphysa.2013.02.137
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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
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2012FA06      Appl.Radiat.Isot. 70, 2295 (2012)

K.Fang, C.Lan, Y.He, X.Kong

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32705.


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
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2009GU05      Nucl.Phys. A823, 83 (2009)

H.Guo, C.-C.Chien, Y.He

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
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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
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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
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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
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1999HE13      Eur.Phys.J. A 5, 111 (1999)

Y.B.He, J.Hufner, P.Zhuang

The Effect of Hadronization on the Instabilities in an Expanding Parton Plasma

doi: 10.1007/s100500050264
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1998BO13      Phys.Rev. C57, 3263 (1998)

P.Bozek, Y.B.He, J.Hufner

Transport Theory with Self-Consistent Confinement Related to the Lattice Data

doi: 10.1103/PhysRevC.57.3263
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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
Citations: PlumX Metrics


1997HE18      Phys.Rev.Lett. 79, 3134 (1997)

Y.D.He

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
Citations: PlumX Metrics


1997WA33      Nuovo Cim. 110A, 599 (1997)

G.J.Wang, Y.D.He

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1995HE38      Nucl.Instrum.Methods Phys.Res. B95, 225 (1995)

Y.D.He, M.Solarz

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
Citations: PlumX Metrics


1995SO26      Nucl.Instrum.Methods Phys.Res. B100, 188 (1995)

M.Solarz, Y.D.He

Dependence of CR-39 Etch Rates on Concentration of Etched Products in Sodium Hydroxide Etchant

doi: 10.1016/0168-583X(95)00484-X
Citations: PlumX Metrics


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
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1994HE16      Z.Phys. A348, 105 (1994)

Y.D.He, P.D.Price

Nuclear and Electromagnetic Fragmentation of 2.25-TeV 197Au Nuclei

doi: 10.1007/BF01289597
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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)

Y.He, F.Wang, C.W.Wong

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
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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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Note: The following list of authors and aliases matches the search parameter Y.He: , Y.B.HE, Y.D.HE, Y.J.HE, Y.L.HE, Y.Q.HE