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2024AC01      Phys.Rev. C 109, 014911 (2024)

S.Acharya, D.Adamova, G.Aglieri Rinella, M.Agnello, N.Agrawal, Z.Ahammed, S.Ahmad, S.U.Ahn, I.Ahuja, A.Akindinov, M.Al-Turany, D.Aleksandrov, B.Alessandro, H.M.Alfanda, R.Alfaro Molina, B.Ali, A.Alici, N.Alizadehvandchali, A.Alkin, J.Alme, G.Alocco, T.Alt, A.R.Altamura, I.Altsybeev, J.R.Alvarado, M.N.Anaam, C.Andrei, N.Andreou, A.Andronic, V.Anguelov, F.Antinori, P.Antonioli, N.Apadula, L.Aphecetche, H.Appelshauser, C.Arata, S.Arcelli, M.Aresti, R.Arnaldi, J.G.M.C.A.Arneiro, I.C.Arsene, M.Arslandok, A.Augustinus, R.Averbeck, M.D.Azmi, H.Baba, A.Badala, J.Bae, Y.W.Baek, X.Bai, R.Bailhache, Y.Bailung, A.Balbino, A.Baldisseri, B.Balis, D.Banerjee, Z.Banoo, R.Barbera, F.Barile, L.Barioglio, M.Barlou, B.Barman, G.G.Barnafoldi, L.S.Barnby, V.Barret, L.Barreto, C.Bartels, K.Barth, E.Bartsch, N.Bastid, S.Basu, G.Batigne, D.Battistini, B.Batyunya, D.Bauri, J.L.Bazo Alba, I.G.Bearden, C.Beattie, P.Becht, D.Behera, I.Belikov, A.D.C.Bell Hechavarria, F.Bellini, R.Bellwied, S.Belokurova, Y.A.V.Beltran, G.Bencedi, S.Beole, Y.Berdnikov, A.Berdnikova, L.Bergmann, M.G.Besoiu, L.Betev, P.P.Bhaduri, A.Bhasin, M.A.Bhat, B.Bhattacharjee, L.Bianchi, N.Bianchi, J.Bielcik, J.Bielcikova, J.Biernat, A.P.Bigot, A.Bilandzic, G.Biro, S.Biswas, N.Bize, J.T.Blair, D.Blau, M.B.Blidaru, N.Bluhme, C.Blume, G.Boca, F.Bock, T.Bodova, A.Bogdanov, S.Boi, J.Bok, L.Boldizsar, M.Bombara, P.M.Bond, G.Bonomi, H.Borel, A.Borissov, A.G.Borquez Carcamo, H.Bossi, E.Botta, Y.E.M.Bouziani, L.Bratrud, P.Braun-Munzinger, M.Bregant, M.Broz, G.E.Bruno, M.D.Buckland, D.Budnikov, H.Buesching, S.Bufalino, P.Buhler, N.Burmasov, Z.Buthelezi, A.Bylinkin, S.A.Bysiak, M.Cai, H.Caines, A.Caliva, E.Calvo Villar, J.M.M.Camacho, P.Camerini, F.D.M.Canedo, S.L.Cantway, M.Carabas, A.A.Carballo, F.Carnesecchi, R.Caron, L.A.D.Carvalho, J.Castillo Castellanos, F.Catalano, C.Ceballos Sanchez, I.Chakaberia, P.Chakraborty, S.Chandra, S.Chapeland, M.Chartier, S.Chattopadhyay, S.Chattopadhyay, T.Cheng, C.Cheshkov, B.Cheynis, V.Chibante Barroso, D.D.Chinellato, E.S.Chizzali, J.Cho, S.Cho, P.Chochula, D.Choudhury, P.Christakoglou, C.H.Christensen, P.Christiansen, T.Chujo, M.Ciacco, C.Cicalo, F.Cindolo, M.R.Ciupek, G.Clai, F.Colamaria, J.S.Colburn, D.Colella, M.Colocci, M.Concas, G.Conesa Balbastre, Z.Conesa del Valle, G.Contin, J.G.Contreras, M.L.Coquet, P.Cortese, M.R.Cosentino, F.Costa, S.Costanza, C.Cot, J.Crkovska, P.Crochet, R.Cruz-Torres, P.Cui, A.Dainese, M.C.Danisch, A.Danu, P.Das, P.Das, S.Das, A.R.Dash, S.Dash, A.De Caro, G.de Cataldo, J.de Cuveland, A.De Falco, D.De Gruttola, N.De Marco, C.De Martin, S.De Pasquale, R.Deb, R.Del Grande, L.Dello Stritto, W.Deng, P.Dhankher, D.Di Bari, A.Di Mauro, B.Diab, R.A.Diaz, T.Dietel, Y.Ding, J.Ditzel, R.Divia, D.U.Dixit, O.Djuvsland, U.Dmitrieva, A.Dobrin, B.Donigus, J.M.Dubinski, A.Dubla, S.Dudi, P.Dupieux, M.Durkac, N.Dzalaiova, T.M.Eder, R.J.Ehlers, F.Eisenhut, R.Ejima, D.Elia, B.Erazmus, F.Ercolessi, B.Espagnon, G.Eulisse, D.Evans, S.Evdokimov, L.Fabbietti, M.Faggin, J.Faivre, F.Fan, W.Fan, A.Fantoni, M.Fasel, P.Fecchio, A.Feliciello, G.Feofilov, A.Fernandez Tellez, L.Ferrandi, M.B.Ferrer, A.Ferrero, C.Ferrero, A.Ferretti, V.J.G.Feuillard, V.Filova, D.Finogeev, F.M.Fionda, E.Flatland, F.Flor, A.N.Flores, S.Foertsch, I.Fokin, S.Fokin, E.Fragiacomo, E.Frajna, U.Fuchs, N.Funicello, C.Furget, A.Furs, T.Fusayasu, J.J.Gaardhoje, M.Gagliardi, A.M.Gago, T.Gahlaut, C.D.Galvan, D.R.Gangadharan, P.Ganoti, C.Garabatos, T.Garcia Chavez, E.Garcia-Solis, C.Gargiulo, P.Gasik, A.Gautam, M.B.Gay Ducati, M.Germain, A.Ghimouz, C.Ghosh, M.Giacalone, G.Gioachin, P.Giubellino, P.Giubilato, A.M.C.Glaenzer, P.Glassel, E.Glimos, D.J.Q.Goh, V.Gonzalez, M.Gorgon, K.Goswami, S.Gotovac, V.Grabski, L.K.Graczykowski, E.Grecka, A.Grelli, C.Grigoras, V.Grigoriev, S.Grigoryan, F.Grosa, J.F.Grosse-Oetringhaus, R.Grosso, D.Grund, N.A.Grunwald, G.G.Guardiano, R.Guernane, M.Guilbaud, K.Gulbrandsen, T.Gundem, T.Gunji, W.Guo, A.Gupta, R.Gupta, R.Gupta, K.Gwizdziel, L.Gyulai, C.Hadjidakis, F.U.Haider, S.Haidlova, H.Hamagaki, A.Hamdi, Y.Han, B.G.Hanley, R.Hannigan, J.Hansen, M.R.Haque, J.W.Harris, A.Harton, H.Hassan, D.Hatzifotiadou, P.Hauer, L.B.Havener, S.T.Heckel, E.Hellbar, H.Helstrup, M.Hemmer, T.Herman, G.Herrera Corral, F.Herrmann, S.Herrmann, K.F.Hetland, B.Heybeck, H.Hillemanns, B.Hippolyte, F.W.Hoffmann, B.Hofman, G.H.Hong, M.Horst, A.Horzyk, Y.Hou, P.Hristov, C.Hughes, P.Huhn, L.M.Huhta, T.J.Humanic, A.Hutson, D.Hutter, R.Ilkaev, H.Ilyas, M.Inaba, G.M.Innocenti, M.Ippolitov, A.Isakov, T.Isidori, M.S.Islam, M.Ivanov, M.Ivanov, V.Ivanov, K.E.Iversen, M.Jablonski, B.Jacak, N.Jacazio, P.M.Jacobs, S.Jadlovska, J.Jadlovsky, S.Jaelani, C.Jahnke, M.J.Jakubowska, M.A.Janik, T.Janson, S.Ji, S.Jia, A.A.P.Jimenez, F.Jonas, D.M.Jones, J.M.Jowett, J.Jung, M.Jung, A.Junique, A.Jusko, M.J.Kabus, J.Kaewjai, P.Kalinak, A.S.Kalteyer, A.Kalweit, V.Kaplin, A.Karasu Uysal, D.Karatovic, O.Karavichev, T.Karavicheva, P.Karczmarczyk, E.Karpechev, U.Kebschull, R.Keidel, D.L.D.Keijdener, M.Keil, B.Ketzer, S.S.Khade, A.M.Khan, S.Khan, A.Khanzadeev, Y.Kharlov, A.Khatun, A.Khuntia, B.Kileng, B.Kim, C.Kim, D.J.Kim, E.J.Kim, J.Kim, J.S.Kim, J.Kim, J.Kim, M.Kim, S.Kim, T.Kim, K.Kimura, S.Kirsch, I.Kisel, S.Kiselev, A.Kisiel, J.P.Kitowski, J.L.Klay, J.Klein, S.Klein, C.Klein-Bosing, M.Kleiner, T.Klemenz, A.Kluge, A.G.Knospe, C.Kobdaj, T.Kollegger, A.Kondratyev, N.Kondratyeva, E.Kondratyuk, J.Konig, S.A.Konigstorfer, P.J.Konopka, G.Kornakov, M.Korwieser, S.D.Koryciak, A.Kotliarov, V.Kovalenko, M.Kowalski, V.Kozhuharov, I.Kralik, A.Kravcakova, L.Krcal, M.Krivda, F.Krizek, K.Krizkova Gajdosova, M.Kroesen, M.Kruger, D.M.Krupova, E.Kryshen, V.Kucera, C.Kuhn, P.G.Kuijer, T.Kumaoka, D.Kumar, L.Kumar, N.Kumar, S.Kumar, S.Kundu, P.Kurashvili, A.Kurepin, A.B.Kurepin, A.Kuryakin, S.Kushpil, M.J.Kweon, Y.Kwon, S.L.La Pointe, P.La Rocca, A.Lakrathok, M.Lamanna, A.R.Landou, R.Langoy, P.Larionov, E.Laudi, L.Lautner, R.Lavicka, R.Lea, H.Lee, I.Legrand, G.Legras, J.Lehrbach, T.M.Lelek, R.C.Lemmon, I.Leon Monzon, M.M.Lesch, E.D.Lesser, P.Levai, X.Li, J.Lien, R.Lietava, I.Likmeta, B.Lim, S.H.Lim, V.Lindenstruth, A.Lindner, C.Lippmann, D.H.Liu, J.Liu, G.S.S.Liveraro, I.M.Lofnes, C.Loizides, S.Lokos, J.Lomker, P.Loncar, X.Lopez, E.Lopez Torres, P.Lu, F.V.Lugo, J.R.Luhder, M.Lunardon, G.Luparello, Y.G.Ma, M.Mager, A.Maire, E.M.Majerz, M.V.Makariev, M.Malaev, G.Malfattore, N.M.Malik, Q.W.Malik, S.K.Malik, L.Malinina, D.Mallick, N.Mallick, G.Mandaglio, S.K.Mandal, V.Manko, F.Manso, V.Manzari, Y.Mao, R.W.Marcjan, G.V.Margagliotti, A.Margotti, A.Marin, C.Markert, P.Martinengo, M.I.Martinez, G.Martinez Garcia, M.P.P.Martins, S.Masciocchi, M.Masera, A.Masoni, L.Massacrier, O.Massen, A.Mastroserio, O.Matonoha, S.Mattiazzo, A.Matyja, C.Mayer, A.L.Mazuecos, F.Mazzaschi, M.Mazzilli, J.E.Mdhluli, Y.Melikyan, A.Menchaca-Rocha, J.E.M.Mendez, E.Meninno, A.S.Menon, M.Meres, S.Mhlanga, Y.Miake, L.Micheletti, D.L.Mihaylov, K.Mikhaylov, A.N.Mishra, D.Miskowiec, A.Modak, B.Mohanty, M.Mohisin Khan, M.A.Molander, S.Monira, C.Mordasini, D.A.Moreira De Godoy, I.Morozov, A.Morsch, T.Mrnjavac, V.Muccifora, S.Muhuri, J.D.Mulligan, A.Mulliri, M.G.Munhoz, R.H.Munzer, H.Murakami, S.Murray, L.Musa, J.Musinsky, J.W.Myrcha, B.Naik, A.I.Nambrath, B.K.Nandi, R.Nania, E.Nappi, A.F.Nassirpour, A.Nath, C.Nattrass, M.N.Naydenov, A.Neagu, A.Negru, L.Nellen, R.Nepeivoda, S.Nese, G.Neskovic, N.Nicassio, B.S.Nielsen, E.G.Nielsen, S.Nikolaev, S.Nikulin, V.Nikulin, F.Noferini, S.Noh, P.Nomokonov, J.Norman, N.Novitzky, P.Nowakowski, A.Nyanin, J.Nystrand, M.Ogino, S.Oh, A.Ohlson, V.A.Okorokov, J.Oleniacz, A.C.Oliveira Da Silva, A.Onnerstad, C.Oppedisano, A.Ortiz Velasquez, J.Otwinowski, M.Oya, K.Oyama, Y.Pachmayer, S.Padhan, D.Pagano, G.Paic, S.Paisano-Guzman, A.Palasciano, S.Panebianco, H.Park, H.Park, J.Park, J.E.Parkkila, Y.Patley, R.N.Patra, B.Paul, H.Pei, T.Peitzmann, X.Peng, M.Pennisi, S.Perciballi, D.Peresunko, G.M.Perez, Y.Pestov, V.Petrov, M.Petrovici, R.P.Pezzi, S.Piano, M.Pikna, P.Pillot, O.Pinazza, L.Pinsky, C.Pinto, S.Pisano, M.Ploskon, M.Planinic, F.Pliquett, M.G.Poghosyan, B.Polichtchouk, S.Politano, N.Poljak, A.Pop, S.Porteboeuf-Houssais, V.Pozdniakov, I.Y.Pozos, K.K.Pradhan, S.K.Prasad, S.Prasad, R.Preghenella, F.Prino, C.A.Pruneau, I.Pshenichnov, M.Puccio, S.Pucillo, Z.Pugelova, S.Qiu, L.Quaglia, S.Ragoni, A.Rai, A.Rakotozafindrabe, L.Ramello, F.Rami, T.A.Rancien, M.Rasa, S.S.Rasanen, R.Rath, M.P.Rauch, I.Ravasenga, K.F.Read, C.Reckziegel, A.R.Redelbach, K.Redlich, C.A.Reetz, H.D.Regules-Medel, A.Rehman, F.Reidt, H.A.Reme-Ness, Z.Rescakova, K.Reygers, A.Riabov, V.Riabov, R.Ricci, M.Richter, A.A.Riedel, W.Riegler, A.G.Riffero, C.Ristea, M.V.Rodriguez, M.Rodriguez Cahuantzi, S.A.Rodriguez Ramirez, K.Roed, R.Rogalev, E.Rogochaya, T.S.Rogoschinski, D.Rohr, D.Rohrich, P.F.Rojas, S.Rojas Torres, P.S.Rokita, G.Romanenko, F.Ronchetti, A.Rosano, E.D.Rosas, K.Roslon, A.Rossi, A.Roy, S.Roy, N.Rubini, D.Ruggiano, R.Rui, P.G.Russek, R.Russo, A.Rustamov, E.Ryabinkin, Y.Ryabov, A.Rybicki, H.Rytkonen, J.Ryu, W.Rzesa, O.A.M.Saarimaki, S.Sadhu, S.Sadovsky, J.Saetre, K.Safarik, P.Saha, S.K.Saha, S.Saha, B.Sahoo, B.Sahoo, R.Sahoo, S.Sahoo, D.Sahu, P.K.Sahu, J.Saini, K.Sajdakova, S.Sakai, M.P.Salvan, S.Sambyal, D.Samitz, I.Sanna, T.B.Saramela, P.Sarma, V.Sarritzu, V.M.Sarti, M.H.P.Sas, S.Sawan, J.Schambach, H.S.Scheid, C.Schiaua, R.Schicker, F.Schlepper, A.Schmah, C.Schmidt, H.R.Schmidt, M.O.Schmidt, M.Schmidt, N.V.Schmidt, A.R.Schmier, R.Schotter, A.Schroter, J.Schukraft, K.Schweda, G.Scioli, E.Scomparin, J.E.Seger, Y.Sekiguchi, D.Sekihata, M.Selina, I.Selyuzhenkov, S.Senyukov, J.J.Seo, D.Serebryakov, L.Serksnyte, A.Sevcenco, T.J.Shaba, A.Shabetai, R.Shahoyan, A.Shangaraev, A.Sharma, B.Sharma, D.Sharma, H.Sharma, M.Sharma, S.Sharma, S.Sharma, U.Sharma, A.Shatat, O.Sheibani, K.Shigaki, M.Shimomura, J.Shin, S.Shirinkin, Q.Shou, Y.Sibiriak, S.Siddhanta, T.Siemiarczuk, T.F.Silva, D.Silvermyr, T.Simantathammakul, R.Simeonov, B.Singh, B.Singh, K.Singh, R.Singh, R.Singh, R.Singh, S.Singh, V.K.Singh, V.Singhal, T.Sinha, B.Sitar, M.Sitta, T.B.Skaali, G.Skorodumovs, M.Slupecki, N.Smirnov, R.J.M.Snellings, E.H.Solheim, J.Song, C.Sonnabend, F.Soramel, A.B.Soto-hernandez, R.Spijkers, I.Sputowska, J.Staa, J.Stachel, I.Stan, P.J.Steffanic, S.F.Stiefelmaier, D.Stocco, I.Storehaug, P.Stratmann, S.Strazzi, A.Sturniolo, C.P.Stylianidis, A.A.P.Suaide, C.Suire, M.Sukhanov, M.Suljic, R.Sultanov, V.Sumberia, S.Sumowidagdo, S.Swain, I.Szarka, M.Szymkowski, S.F.Taghavi, G.Taillepied, J.Takahashi, G.J.Tambave, S.Tang, Z.Tang, J.D.Tapia Takaki, N.Tapus, L.A.Tarasovicova, M.G.Tarzila, G.F.Tassielli, A.Tauro, A.Tavira Garcia, G.Tejeda Munoz, A.Telesca, L.Terlizzi, C.Terrevoli, S.Thakur, D.Thomas, A.Tikhonov, N.Tiltmann, A.R.Timmins, M.Tkacik, T.Tkacik, A.Toia, R.Tokumoto, K.Tomohiro, N.Topilskaya, M.Toppi, T.Tork, P.V.Torres, V.V.Torres, A.G.Torres Ramos, A.Trifiro, A.S.Triolo, S.Tripathy, T.Tripathy, S.Trogolo, V.Trubnikov, W.H.Trzaska, T.P.Trzcinski, A.Tumkin, R.Turrisi, T.S.Tveter, K.Ullaland, B.Ulukutlu, A.Uras, G.L.Usai, M.Vala, N.Valle, L.V.R.van Doremalen, M.van Leeuwen, C.A.van Veen, R.J.G.van Weelden, P.Vande Vyvre, D.Varga, Z.Varga, M.Vasileiou, A.Vasiliev, O.Vazquez Doce, O.Vazquez Rueda, V.Vechernin, E.Vercellin, S.Vergara Limon, R.Verma, L.Vermunt, R.Vertesi, M.Verweij, L.Vickovic, Z.Vilakazi, O.Villalobos Baillie, A.Villani, A.Vinogradov, T.Virgili, M.M.O.Virta, V.Vislavicius, A.Vodopyanov, B.Volkel, M.A.Volkl, K.Voloshin, S.A.Voloshin, G.Volpe, B.von Haller, I.Vorobyev, N.Vozniuk, J.Vrlakova, J.Wan, C.Wang, D.Wang, Y.Wang, Y.Wang, A.Wegrzynek, F.T.Weiglhofer, S.C.Wenzel, J.P.Wessels, J.Wiechula, J.Wikne, G.Wilk, J.Wilkinson, G.A.Willems, B.Windelband, M.Winn, J.R.Wright, W.Wu, Y.Wu, R.Xu, A.Yadav, A.K.Yadav, S.Yalcin, Y.Yamaguchi, S.Yang, S.Yano, Z.Yin, I.-K.Yoo, J.H.Yoon, H.Yu, S.Yuan, A.Yuncu, V.Zaccolo, C.Zampolli, F.Zanone, N.Zardoshti, A.Zarochentsev, P.Zavada, N.Zaviyalov, M.Zhalov, B.Zhang, C.Zhang, L.Zhang, S.Zhang, X.Zhang, Y.Zhang, Z.Zhang, M.Zhao, V.Zherebchevskii, Y.Zhi, D.Zhou, Y.Zhou, J.Zhu, Y.Zhu, S.C.Zugravel, N.Zurlo

System-size dependence of the hadronic rescattering effect at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.109.014911
Citations: PlumX Metrics


2024CH12      Phys.Rev. C 109, L021604 (2024)

X.Chen, J.Yang, Y.Cui, K.Zhao, Zh.Li, Y.Zhang

Novel Pauli blocking method in quantum molecular dynamics type models

doi: 10.1103/PhysRevC.109.L021604
Citations: PlumX Metrics


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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2024GA07      Phys.Rev. C 109, 024307 (2024)

T.J.Gao, J.-B.Lu, Y.Ma, Y.Zhang, S.Q.Zhang, H.D.Wang, J.-Q.Liu, P.-Y.Yang, Zh.Ren, Ch.-Q.Li, Q.B.Chen, Z.C.Gao, J.Li, K.Y.Ma, G.Dong

Evidence for possible multiple chiral doublet bands with identical configuration in the odd-odd nucleus 126Cs

doi: 10.1103/PhysRevC.109.024307
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2024GU05      Eur.Phys.J. A 60, 36 (2024)

D.Guo, X.He, P.Li, Zh.Qin, Ch.Hu, B.Wang, Y.Zhou, K.Zheng, Y.Zhang, X.Wei, H.Yang, D.Hu, M.Shao, L.Duan, Y.Yu, Zh.Sun, Y.Wang, Q.Li, Zh.Xiao

Studies of nuclear equation of state with the HIRFL-CSR external-target experiment

doi: 10.1140/epja/s10050-024-01245-2
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2024LI17      Phys.Rev. C 109, 034310 (2024)

C.B.Li, Y.Zheng, T.X.Li, X.G.Wu, H.Y.Wu, M.Zheng, Z.H.Zhao, Y.Q.Li, R.Hong, Z.Y.He, J.Z.Li, J.L.Wang, C.Y.Guo, Z.X.Zhou, L.Ni, G.S.Li, X.H.Zhou, B.Guo, S.Y.Wang, M.L.Liu, Y.H.Zhang, C.Y.He, F.L.Liu, S.Wang, L.H.Zhu

Lifetime measurements of the first 2+ states in 116, 118Te

doi: 10.1103/PhysRevC.109.034310
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Data from this article have been entered in the XUNDL database. For more information, click here.


2024PA10      Phys.Lett. B 848, 138340 (2024)

F.Pan, Y.Zhang, L.Dai, J.P.Draayer, D.Kekejian

A multi-shell extension of the interacting boson model

NUCLEAR STRUCTURE 152Sm; calculated strength distributions, energy levels, J, π, B(Eλ), electric quadrupole moments with a multi-shell extension of the IBM for even-even nuclei that includes multiple excitations. Comparison with available data.

doi: 10.1016/j.physletb.2023.138340
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2024SU04      Chin.Phys.C 48, 034002 (2024)

M.Z.Sun, Y.Yu, X.P.Wang, M.Wang, J.G.Li, Y.H.Zhang, K.Blaum, Z.Y.Chen, R.J.Chen, H.Y.Deng, C.Y.Fu, W.W.Ge, W.J.Huang, H.Y.Jiao, H.H.Li, H.F.Li, Y.F.Luo, T.Liao, Yu.A.Litvinov, M.Si, P.Shuai, J.Y.Shi, Q.Wang, Y.M.Xing, X.Xu, H.S.Xu, F.R.Xu, Q.Yuan, T.Yamaguchi, X.L.Yan, J.C.Yang, Y.J.Yuan, X.H.Zhou, X.Zhou, M.Zhang, Q.Zeng

Ground-state mass of 22Al and test of state-of-the-art ab initio calculations

NUCLEAR STRUCTURE 22Al, 22F; calculated test of the state-of-the-art ab initio valence-space in-medium similarity renormalization group calculations with four sets of interactions derived from the chiral effective field theory using excitation energies and mirror energy differences.

doi: 10.1088/1674-1137/ad1a0a
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2024WA04      Phys.Rev. C 109, 014624 (2024)

K.Wang, Y.Y.Yang, Jin Lei, A.M.Moro, V.Guimaraes, J.G.Li, F.F.Duan, Z.Y.Sun, G.Yang, D.Y.Pang, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Liu, J.L.Lou, H.J.Ong, B.F.Lv, S.Guo, M.Kumar Raju, X.H.Wang, R.H.Li, X.X.Xu, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Elastic scattering and breakup reactions of the mirror nuclei 12B and 12N on 208Pb using ab initio structure inputs

doi: 10.1103/PhysRevC.109.014624
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2024YA05      Chin.Phys.C 48, 034001 (2024)

G.Yang, F.-F.Duan, K.Wang, Y.-Y.Yang, Zh.-Y.Sun, V.Guimaraes, D.-Y.Pang, W.-D.Chen, L.Jin, Sh.-W.Xu, J.-B.Ma, P.Ma, Zh.Bai, L.-H.Wang, Q.Liu, H.-J.Ong, B.-F.Lv, S.Guo, M.K.Raju, X.-H.Wang, R.-H.Li, Y.-H.Zhang, X.-H.Zhou, Zh.-G.Hu, H.-Sh.Xu

Elastic scattering of 13C and 14C isotopes on a 208Pb target at energies of approximately five times the Coulomb barriers

NUCLEAR REACTIONS 208Pb(13C, 13C), E=340 MeV; 208Pb(14C, 14C), E=294, 342 MeV; measured reaction products; deduced σ(θ) within the optical model and continuum-discretized coupled-channels (CDCC) framework. Comparison with available data. The Heavy-Ion Research Facility in Lanzhou (HIRFL), the National Laboratory of Heavy Ion Research of the Institute of Modern Physics.

doi: 10.1088/1674-1137/ad1678
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2024YA08      Phys.Rev.Lett. 132, 152502 (2024)

X.Yan, Zh.Cheng, A.Abdukerim, Z.Bo, W.Chen, X.Chen, Ch.Cheng, X.Cui, Y.Fan, D.Fang, Ch.Fu, M.Fu, L.Geng, K.Giboni, L.Gu, X.Guo, Ch.Han, K.Han, Ch.He, J.He, D.Huang, Y.Huang, J.Huang, Zh.Huang, R.Hou, Y.Hou, X.Ji, Y.Ju, Ch.Li, J.Li, M.Li, Sh.Li, T.Li, Q.Lin, J.Liu, X.Lu, C.Lu, L.Luo, Y.Luo, W.Ma, Y.Ma, Y.Mao, Y.Meng, X.Ning, B.Pang, N.Qi, Zh.Qian, X.Ren, N.Shaheed, X.Shang, X.Shao, G.Shen, L.Si, W.Sun, A.Tan, Y.Tao, A.Wang, M.Wang, Q.Wang, Sh.Wang, S.Wang, W.Wang, X.Wang, Zh.Wang, Y.Wei, M.Wu, W.Wu, J.Xia, M.Xiao, X.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, Y.Yao, Ch.Yu, Y.Yuan, Zh.Yuan, X.Zeng, D.Zhang, M.Zhang, P.Zhang, Sh.Zhang, Sh.Zhang, T.Zhang, W.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou, Y.Zhou, Y.Zhou, for the PandaX Collaboration

Searching for Two-Neutrino and Neutrinoless Double Beta Decay of 134Xe with the PandaX-4T Experiment

RADIOACTIVITY 134Xe(2β-); measured decay products, Eβ, Iβ; deduced two-neutrino and neutrinoless T1/2 limits. Comparison with available data. The cylindrical active volume PandaX-4T dual-phase TPC.

doi: 10.1103/PhysRevLett.132.152502
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2024ZH05      Phys.Rev. C 109, 014622 (2024)

M.-H.Zhang, Y.-H.Zhang, Y.Zou, Ch.Wang, L.Zhu, F.-Sh.Zhang

Predictions of synthesizing elements with Z=119 and 120 in fusion reactions

doi: 10.1103/PhysRevC.109.014622
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2024ZH11      Phys.Rev. C 109, 024902 (2024)

Y.Zhang, P.Ru

Squeezed correlations of bosons with nonzero widths for expanding sources

doi: 10.1103/PhysRevC.109.024902
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2024ZH16      Eur.Phys.J. A 60, (2024)

Y.-X.Zhang, S.Zhang, Y.-G.Ma

Signatures of an α + core structure in 44Ti + 44Ti collisions at √ σNN = 5.02 TeV by a multiphase transport model

doi: 10.1140/epja/s10050-024-01290-x
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2023AK05      Phys.Lett. B 845, 138128 (2023)

T.Akaishi, H.Asano, X.Chen, A.Clozza, C.Curceanu, R.Del Grande, C.Guaraldo, C.Han, T.Hashimoto, M.Iliescu, K.Inoue, S.Ishimoto, K.Itahashi, M.Iwasaki, Y.Ma, M.Miliucci, R.Murayama, H.Noumi, H.Ohnishi, S.Okada, H.Outa, K.Piscicchia, A.Sakaguchi, F.Sakuma, M.Sato, A.Scordo, K.Shirotori, D.Sirghi, F.Sirghi, S.Suzuki, K.Tanida, T.Toda, M.Tokuda, T.Yamaga, X.Yuan, P.Zhang, Y.Zhang, H.Zhang

Precise lifetime measurement of 4ΛH hypernucleus using in-flight 4He(K-, π0)4ΛH reaction

RADIOACTIVITY 4H(π-) [from 4He(K-, π0), E not given]; measured decay products, Eγ, Iγ; deduced hypernucleus T1/2. Comparison with available data. Experiment (J-PARC E73).

doi: 10.1016/j.physletb.2023.138128
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2023AN14      Sci. Rep. 13, 12657 (2023)

Z.An, W.Qiu, W.Jiang, G.Yang, X.Li, Z.Liao, Z.Zhuang, X.Zhang, S.Chen, C.Guo, E.Xiao, X.Fang, X.Li, H.Wang, X.Hu, Bi.Jiang, W.Shen, J.Wang, J.Ren, X.Ruan, D.Wang, S.-Y.Zhang, W.Luo, Z.Zhu, H.Lan, Z.Cao, X.Ma, Y.Liu, P.Wang, Y.Yang, P.Su, X.Deng, W.He, Y.Ma, C.Ma, Y.Wang, P.He, R.Tang, T.Zhou, J.Wang, H.Yi, Y.Zhang, Y.Chen, R.Fan, K.Gao, Q.Li, K.Sun, Z.Tan, M.Gu, H.Jing, J.Tang

Measurement of the 181Ta(n, γ) cross sections up to stellar s-process temperatures at the CSNS Back-n

NUCLEAR REACTIONS 181Ta(n, γ), E=0.001-800 keV; measured reaction products, En, In, TOF; deduced σ, resonance parameters using the R-Matrix code SAMMY, Maxwellian average cross sections (MACS). Comparison with available data. The back-streaming white neutron facility (Back-n) of China spallation neutron source (CSNS).

doi: 10.1038/s41598-023-39603-7
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2023BA40      Eur.Phys.J. A 59, 284 (2023); Erratum Eur.Phys.J. A 60, 23 (2024)

X.H.Bai, Z.Wei, K.Wu, S.Y.Zhang, P.Q.Zhang, Y.N.Han, M.Li, J.Y.Wang, Z.Y.Wei, Z.E.Yao, J.R.Wang, Y.Zhang

Physical design of a high-intensity compact D–D/D–T neutron generator based on the internal antenna RF ion source

NUCLEAR REACTIONS 2,3H(d, n), E=200 keV; measured reaction products, En, In; deduced neutron yields.

doi: 10.1140/epja/s10050-023-01177-3
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2023CH44      Phys.Rev. C 108, 034613 (2023)

X.Chen, L.Li, Y.Cui, J.Yang, Z.Li, Y.Zhang

Bayesian reconstruction of impact parameter distributions from two observables for intermediate energy heavy ion collisions

doi: 10.1103/PhysRevC.108.034613
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2023GA15      Phys.Rev. C 107, 064618 (2023)

Z.Gao, X.Zhang, Y.Zhang, Y.Ju, L.Chen, H.Ge, F.Ma, Z.Chen, W.Yang

Benchmarking geant4 nuclear models for light fragments of 80.5 MeV/u carbon ions bombarding heavy-metal targets

NUCLEAR REACTIONS W(12C, p), (12C, d), (12C, t), (12C, 3He), (12C, α), E=80.5 MeV/nucleon; Cu, Au, Pb(12C, p), (12C, α), E=80.5 MeV/nucleon; calculated σ(θ, E), angular distributions of outgoing particles. Simulation of experimental setup from Nucl. Instrum. Methods Phys. Res. B 514, 15 (2022) using G4BinaryLightIonReaction, G4QMDReaction and INCL++ models. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.064618
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2023GA21      J.Radioanal.Nucl.Chem. 332, 3037 (2023)

X.Gao, P.Zhang, J.Li, W.Mao, Z.Guo, J.Li, Y.Zhang, J.Chen, L.Sheng, M.Lin

Production of 99Mo via photoneutron reaction using a 50 MeV electron linear accelerator

NUCLEAR REACTIONS 100Mo(γ, n), E<50 MeV; calculated yields using FLUKA program; deduced guidance on the size of W conversion and molybdenum targets, as well as the selection of molybdenum species.

doi: 10.1007/s10967-023-09003-2
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2023GA25      Astrophys.J. 957, L36 (2023)

S.Gandhi, S.de Regt, I.Snellen, Y.Zhang, B.Rugers, N.van Leur, Q.Bosschaart

JWST Measurements of 13C, 18O, and 17O in the Atmosphere of Super-Jupiter VHS 1256 b

ATOMIC MASSES 13C, 17,18O; measured frequencies; deduced the ratio of abundances.

doi: 10.3847/2041-8213/ad07e2
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2023HE16      Eur.Phys.J. C 83, 1092 (2023)

Z.He, M.Li, W.Bu, C.Xiao, X.Wei, Y.Yang, Z.Qin, S.He, T.Qiu, P.Ma, C.Lu, L.Duan, B.Hu, Y.Zhang, H.Yang

Development of a semi-cylindrical time projection chamber prototype for (3He, t) charge exchange reaction experiment

NUCLEAR REACTIONS 13,17C(3He, t), E ∼ 450 MeV; analyzed available data; deduced rough σ estimate.

doi: 10.1140/epjc/s10052-023-12170-x
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2023HU02      J.Phys.(London) G50, 025107 (2023)

B.-Y.Hu, Y.Zhang, G.-X.Na, S.-N.Wang, W.Teng

Quadrupole and octupole states in 152Sm using the proton-neutron interacting boson model

NUCLEAR STRUCTURE 152Sm; calculated energy levels, J, π, B(E2), B(E1), B(E3), B(M1) using the proton-neutron interacting boson model (IBM-2) in terms of the SU(3) basis. Comparison with available data.

doi: 10.1088/1361-6471/acb282
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2023HU18      Phys.Rev. C 108, 034301 (2023)

W.J.Huang, X.Zhou, Y.H.Zhang, M.Wang, Yu.A.Litvinov, K.Blaum

Ground-state mass of the odd-odd n = z nuclide 70Br

doi: 10.1103/PhysRevC.108.034301
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2023HU22      Phys.Rev. C 108, 054907 (2023)

Q.Hu, G.Y.Tian, R.Wada, X.Q.Liu, W.P.Lin, H.Zheng, Y.P.Zhang, Z.Q.Chen, R.Han, M.R.Huang

Semirelativistic antisymmetrized molecular dynamics for the production of energetic neutrons in intermediate-energy heavy-ion reactions

doi: 10.1103/PhysRevC.108.054907
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2023HU23      Eur.Phys.J. A 59, 265 (2023)

D.Y.Huo, Z.Wei, K.Wu, C.Han, Y.X.Wang, Y.N.Han, Z.E.Yao, Y.Zhang, J.R.Wang, X.D.Su

Evaluation of pre-neutron-emission mass distributions in induced fission of typical actinides based on Monte Carlo dropout neural network

NUCLEAR REACTIONS 232Th, 235,238U, 237Np, 239Pu(n, F), E<45 MeV; analyzed available data; deduced pre-neutron-emission mass distribution wi th the Monte Carlo dropout neural network (MC-Dropout NN) method.

doi: 10.1140/epja/s10050-023-01189-z
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2023LA10      Chin.Phys.C 47, 094001 (2023)

C.Lan, Y.Niu, Y.Wei, F.Lu, X.Yang, R.Xu, Y.Zhang, Y.Ge, J.Wang, G.Jiang

Measurement of the (n, 2n) reaction cross-sections of iodine and cesium induced by D-T neutrons with covariance analysis

NUCLEAR REACTIONS 127I, 137Cs, 93Nb(n, 2n), E=13.83-14.79 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS-1.95 and EMPIRE-3.2.3 calculations. The K-400 neutron generator at the China Academy of Engineering Physics.

doi: 10.1088/1674-1137/ace313
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2023LI03      Phys.Rev. C 107, 014302 (2023)

H.H.Li, Q.Yuan, J.G.Li, M.R.Xie, S.Zhang, Y.H.Zhang, X.X.Xu, N.Michel, F.R.Xu, W.Zuo

Investigation of isospin-symmetry breaking in mirror energy difference and nuclear mass with ab initio calculations

NUCLEAR STRUCTURE 21,23Al, 23Ne, 21,22O, 22,23Si, 23F, 27P, 27Mg, 46Ti, 46V, 46Cr; calculated levels, J, π. 18,19Ne, 19Na, 20,21Na, 22,23,24,25Al, 27Si, 29S, 33Ar; calculated mirror energy difference in the mirror nuclei states. A=17-75; calculated coefficient "b" of the isobaric multiplet mass equation. Ab initio valence-space in-medium similarity renormalization group (VS-IMSRG) method. Comparison to experimental data and AME2020.

doi: 10.1103/PhysRevC.107.014302
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2023LI17      Int.J.Mod.Phys. E32, 2330002 (2023)

J.-J.Li, N.Tang, Y.-H.Zhang, M.-H.Zhang, C.Wang, X.-R.Zhang, L.Zhu, F.-S.Zhang

Progress on production cross-sections of unknown nuclei in fusion evaporation reactions and multinucleon transfer reactions

NUCLEAR REACTIONS 232Th(204Hg, X), E(cm)=678.1 MeV; 249Bk(238U, X), E(cm)=823.4 MeV; 248Cm(238U, X), E(cm)=824.9 MeV; calculated σ in fusion evaporation (FE) reactions and multinucleon transfer (MNT) reactions.

doi: 10.1142/S0218301323300023
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2023ME12      Phys.Rev. C 108, 034602 (2023)

B.Mei, Y.Guan, N.Zeng, Z.Mai, J.Tu, T.Yu, S.Wang, X.Zhang, P.Ma, X.Xu, X.Tu, Y.Sun, Z.Sun, S.Tang, Y.Yu, F.Fang, D.Yan, S.Jin, Y.Zhao, S.Ma, Y.Zhang

Isotopic cross sections in fragmentation reactions of 12, 14C, 14, 16N, and 16O projectiles on a carbon target

doi: 10.1103/PhysRevC.108.034602
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2023ME14      New Journal of Physics 25, 093026 (2023)

T.Meng, M.X.Ma, B.Tu, P.Ma, Y.W.Zhang, L.Liu, J.Xiao, K.Yao, Y.Zou, Y.Wu, J.G.Wang, B.Wei

Study of single electron capture in O6+ + He collisions

NUCLEAR REACTIONS He(O, X), E=2.63-37.5 keV/nucleon; measured reaction products; deduced the total and l-solved state-selective single EC σ. Comparison with calculations.

doi: 10.1088/1367-2630/acf1c3
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2023WA08      Phys.Rev. C 107, L041601 (2023)

Y.Wang, F.Guan, X.Diao, M.Wan, Y.Qin, Z.Qin, Q.Wu, D.Guo, D.Si, S.Xiao, B.Zhang, Y.Zhang, B.Tian, X.Wei, H.Yang, P.Ma, R.J.Hu, L.Duan, F.Duan, Q.Hu, J.Ma, S.Xu, Z.Bai, Y.Yang, J.Wang, W.Liu, W.Su, X.Wei, C.-W.Ma, X.Li, H.Wang, F.Wang, Y.Zhang, M.Warda, A.Dobrowolski, B.Nerlo-Pomorska, K.Pomorski, L.Ou, Z.Xiao

Observing the ping-pong modality of the isospin degree of freedom in cluster emission from heavy-ion reactions

NUCLEAR REACTIONS 208Pb(86Kr, X), E=25 MeV/nucleon; measured reaction products, A=3 isobars in coincidence with the intermediate mass fragments of A=6-11; deduced velocity spectra of 3H and 3He, yields ratios of 3H/3He correlate reversely to the neutron-to-proton ratio N/Z of the intermediate mass fragments. Comparison with ImQMD transport model. Yield ratio 3H/3He exhibits evident anticorrelation with the N/Z of the latter, suggesting the ping-pong modality of the N/Z of the emitted particles. Anti-correlation shows dependence on the slope of the symmetry energy at saturation density. Compact Spectrometer for Heavy IoN Experiment (CSHINE) at the final focal plane of the Radioactive Ion Beam Line at Lanzhou (RIBLL-I).

doi: 10.1103/PhysRevC.107.L041601
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2023WA10      Phys.Rev.Lett. 130, 192501 (2023)

M.Wang, Y.H.Zhang, X.Zhou, X.H.Zhou, H.S.Xu, M.L.Liu, J.G.Li, Y.F.Niu, W.J.Huang, Q.Yuan, S.Zhang, F.R.Xu, Y.A.Litvinov, K.Blaum, Z.Meisel, R.F.Casten, R.B.Cakirli, R.J.Chen, H.Y.Deng, C.Y.Fu, W.W.Ge, H.F.Li, T.Liao, S.A.Litvinov, P.Shuai, J.Y.Shi, Y.N.Song, M.Z.Sun, Q.Wang, Y.M.Xing, X.Xu, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, M.Zhang

Mass Measurement of Upper fp-Shell N = Z - 2 and N = Z - 1 Nuclei and the Importance of Three-Nucleon Force along the N = Z Line

ATOMIC MASSES 58Zn, 60Ga, 62Ge, 64As, 66Se, 70Kr, 61Ga, 63Ge, 65As, 67Se, 71Kr, 75Sr; measured time-of-flight (TOF); deduced mass excess (ME). A novel method of isochronous mass spectrometry, the Heavy Ion Research Facility in Lanzhou (HIRFL).

doi: 10.1103/PhysRevLett.130.192501
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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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2023XI01      Phys.Rev. C 107, 014304 (2023)

Y.M.Xing, C.X.Yuan, M.Wang, Y.H.Zhang, X.H.Zhou, Yu.A.Litvinov, K.Blaum, H.S.Xu, T.Bao, R.J.Chen, C.Y.Fu, B.S.Gao, W.W.Ge, J.J.He, W.J.Huang, T.Liao, J.G.Li, H.F.Li, S.Litvinov, S.Naimi, P.Shuai, M.Z.Sun, Q.Wang, X.Xu, F.R.Xu, T.Yamaguchi, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, M.Zhang, X.Zhou

Isochronous mass measurements of neutron-deficient nuclei from 112Sn projectile fragmentation

ATOMIC MASSES 69As, 73Br, 75Kr, 79Sr, 81Y, 87Mo, 87mMo, 91Ru, 91mRu, 93Rh, 93mRh, 95Pd, 95mPd, 103Sn; measured revolution times of stored ions, ToF; deduced mass excesses. 27Al, 29Si, 31P, 33S, 35Cl, 37Ar, 39,40K, 41,42Ca, 43,43mSc, 46Ti, 47,48V, 50,49Cr, 51,52,52mMn, 51m,53,54Fe, 55,56,57Co, 57,58,59Ni, 59,60,61Cu, 62,63Zn, 63,65Ga, 65,66Ge, 67,68,69,70Se, 71Br, 73,74Kr, 75,76,77Rb, 77,78Sr, 82Zr, 84Nb, 86Mo, 90Ru, 94Pd, 97,97mAg, 99Cd, 101,101mIn; analyzed masses by comparing to previously measured values and AME2020 evaluation. 87Mo, 91Ru, 93Rh, 95Pd; deduced isomer ratios, isomeric states and assigned J, π values as 1/2- from systematics. 91mRu; deduced mass excess based on the precise measured value for 90Mo. 104Sb, 107Te, 108I, 111Xe, 112Cs; deduced mass excess based on measured mass excess value for 103Sn and literature Q values for α- and p-decays. Systematics of 1/2- isomers in Zr, Mo, Ru, Pd and Cd isotopes and comparison to shell-model calculations. Comparison to AME2020 and NUBASE2020. Isochronous mass spectrometry at the Cooler Storage Ring in Lanzhou of the fragments from 9Be(112Sn, X), E=400.88 MeV/nucleon reaction.

NUCLEAR REACTIONS 9Be(112Sn, X), E=400.88 MeV/nucleon; measured reaction products, number of produced fragments. 87,87mMo, 91,91mRu, 93,93mRh, 95,95mPd; deduced isomeric ratios.

doi: 10.1103/PhysRevC.107.014304
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2023YA14      Universe 9, 206 (2023)

J.Yang, X.Chen, Y.Cui, Z.Li, Y.Zhang

Probing the Neutron Skin of Unstable Nuclei with Heavy-Ion Collisions

NUCLEAR REACTIONS 124Sn(124Sn, X), (132Sn, X), E=200 MeV; calculated peripheral collisions; deduced σ of projectile-like residues correlations with the neutron skin of the system.

doi: 10.3390/universe9050206
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2023ZH06      Phys.Lett. B 838, 137716 (2023)

Y.Zhang, Y.-X.Luo, Q.Liu, J.-Y.Guo

Pseudospin symmetry in resonant states in deformed nuclei

NUCLEAR STRUCTURE 170Yb; calculated pseudospin symmetry (PSS) in resonant states in deformed nuclei by solving the Dirac equation in the complex-momentum representation for a potential with quadrupole deformation at the first order obtained from relativistic mean-field (RMF) calculations.

doi: 10.1016/j.physletb.2023.137716
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2023ZH09      Phys.Rev. C 107, 024604 (2023)

Y.-H.Zhang, J.-J.Li, N.Tang, X.-R.Zhang, Z.Liu, F.-S.Zhang

Production cross sections of new neutron-rich isotopes with Z=92-106 in the multinucleon transfer reaction 197Au + 232Th

NUCLEAR REACTIONS 232Th(197Au, X)258Es/259Es/260Es/261Es/262Es/260Fm/261Fm/262Fm/263Fm/261Md/262Md/263Md/264Md/265Md/261No/263No/264No/265No/266No/267No/263Lr/265Lr/267Lr/268Lr/264Rf/266Rf/268Rf/269Rf/270Rf/264Db/265Db/269Db/271Db/267Sg/268Sg/270Sg/272Sg/273Sg, E(cm)=690.69;232Th(197Au, X)243U/244U/245U/246U/247U/248U/249U/246Np/247Np/248Np/249Np/250Np/251Np/252Np/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/256Am/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/252Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/257Cf/258Cf/259Cf/260Cf/261Cf/258Es/259Es/260Es/261Es/262Es, E(cm)=756.47 MeV; calculated production σ. 232Th(197Au, X), E=690.7, 723.6, 756.5 MeV;232Th(186W, X), E=681, 2 MeV;232Th(238U, X), E=823.8; calculated final isotopic production σ for U, Np, Pu, Am, Cm, Bk, Cf, Es, Fm, Md, No, Lr, Rf, Db and Sg isotopes, calculated driving potentials, potential energy surfaces. 232Th(197Au, X), E=690.7, 723.6, 756.5, 789.4 MeV; interaction time as a function of the impact parameter. 249Cf(136Xe, X), E(cm)=567 MeV; calculated final production σ for Pu, Am, Cm, Bk, Cf, Es isotopes. Calculations performed within the framework of dinuclear system (DNS) model with a decay model GEMINI++. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.024604
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2023ZH10      Eur.Phys.J. A 59, 27 (2023)

M.Zhang, X.Zhou, M.Wang, Y.H.Zhang, Yu.A.Litvinov, H.S.Xu, R.J.Chen, H.Y.Deng, C.Y.Fu, W.W.Ge, H.F.Li, T.Liao, S.A.Litvinov, P.Shuai, J.Y.Shi, R.S.Sidhu, Y.N.Song, M.Z.Sun, S.Suzuki, Q.Wang, Y.M.Xing, X.Xu, T.Yamaguchi, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, X.H.Zhou

Bρ-defined isochronous mass spectrometry and mass measurements of 58Ni fragments

ATOMIC MASSES 23Al, 25Si, 27P, 31Cl, 33Ar, 35K, 37Ca, 41Ti, 43V, 45Cr, 47Mn, 49Fe, 51Co, 53Ni, 55Cu, 43Ti, 44,44mV, 46Cr, 48Mn, 50,51Fe, 52,52mCo, 54Ni, 56Cu, 24,24mAl, 44,44mV, 52,52mCo; measured revolution time spectrum, frequencies; deduced masses, energy differences between the ground states and isomers. The experimental cooler-storage ring CSRe in Lanzhou.

doi: 10.1140/epja/s10050-023-00928-6
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2023ZH19      Eur.Phys.J. A 59, 72 (2023)

Y.-X.Zhang, S.Zhang, Y.-G.Ma

Deuteron production mechanism via azimuthal correlation for p-p and p-Pb collisions at LHC energy with the AMPT model

doi: 10.1140/epja/s10050-023-00980-2
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2023ZH29      Eur.Phys.J. A 59, 101 (2023)

S.Y.Zhang, X.Yang, Y.X.Wang, X.H.Bai, K.Wu, J.Ma, Z.E.Yao, Y.Zhang, Z.Y.Deng, L.Wu, G.T.Gao, T.Z.Jiang, C.Bao, Y.B.Nie, Y.Y.Ding, J.R.Wang, Z.Wei

Measurement of neutron source characterization of the compact D-D neutron generator with unfolding algorithm

doi: 10.1140/epja/s10050-023-01007-6
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2023ZH34      Phys.Rev. C 108, 014614 (2023)

J.T.Zhang, P.Ma, Y.Huang, X.L.Tu, P.Sarriguren, Z.P.Li, Y.Kuang, W.Horiuchi, T.Inakura, L.Xayavong, Y.Sun, K.Kaneko, X.Q.Liu, K.Yue, C.J.Shao, Q.Zeng, B.Mei, P.Egelhof, Yu.A.Litvinov, M.Wang, Y.H.Zhang, X.H.Zhou, Z.Y.Sun

Matter radius of 78Kr from proton elastic scattering at 153 MeV

NUCLEAR REACTIONS 1H(78Kr, p), E=152 MeV/nucleon; measured Ep, Ip; deduced σ(θ). 78Kr; deduced point-matter radius, neutron skin thickness. Glauber model analysis. Comparison of the obtained σ to FRESCO calculations with the phenomenological OMP parameters (KD03). Collision in Cooler Storage Ring of the Heavy Ion Research Facility in Lanzhou (HIRFL-CSR) with molecular hydrogen-gas target. MICRON double-sided Si-strip detector (DSSD) used to measure the recoil protons.

doi: 10.1103/PhysRevC.108.014614
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2023ZH48      Phys.Rev. C 108, 064316 (2023)

S.Zhang, F.R.Xu, J.G.Li, B.S.Hu, Z.H.Cheng, N.Michel, Y.Z.Ma, Q.Yuan, Y.H.Zhang

Ab initio descriptions of A=16 mirror nuclei with resonance and continuum coupling

doi: 10.1103/PhysRevC.108.064316
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2023ZH49      Eur.Phys.J. A 59, 296 (2023)

Y.Zhang, Q.Liu

Shear viscous transport dynamics simulations of parton matter in AMPT model

doi: 10.1140/epja/s10050-023-01218-x
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2022DE12      Phys.Rev. C 105, 064613 (2022)

X.G.Deng, P.Danielewicz, Y.G.Ma, H.Lin, Y.X.Zhang

Impact of fragment formation on shear viscosity in the nuclear liquid-gas phase transition region

doi: 10.1103/PhysRevC.105.064613
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2022DU05      Phys.Rev. C 105, 034602 (2022)

F.F.Duan, Y.Y.Yang, J.Lei, K.Wang, Z.Y.Sun, D.Y.Pang, J.S.Wang, X.Liu, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Hu, Z.H.Gao, X.X.Xu, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, G.Yang, S.Y.Jin, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Elastic scattering and breakup reactions of neutron-rich nucleus 11Be on 208Pb at 210 MeV

NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, 10Be), E=210 MeV; measured reaction products; deduced σ(θ), σ. Comparison with CDCC calculations and experimental results for other reaction systems including tightly- and weakly-bound projectiles impinging on medium to heavy mass targets. Beam by Heavy-Ion Research Facility in Lanzhou (HIRFL, China).

doi: 10.1103/PhysRevC.105.034602
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2022GA07      Nucl.Instrum.Methods Phys.Res. B514, 15 (2022)

Z.Gao, X.Zhang, Y.Ju, L.Chen, H.L.Ge, Y.Zhang, F.Ma, H.Zhang, G.Shi, Z.Chen, R.Han, G.Tian, F.Shi, B.Liu, X.Zhang

Nuclear reaction measurements of 80.5 MeV/u 12C beam bombarding on C, Cu, W, Au, Pb targets

NUCLEAR REACTIONS C, Cu, W, 197Au, Pb(12C, X), E=80.5 MeV/nucleon; measured reaction products; deduced σ(θ, E). Institute of Modern Physics, Chinese Academy of Sciences.

doi: 10.1016/j.nimb.2022.01.003
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2022GO11      Eur.Phys.J. C 82, 945 (2022)

I.Goldman, R.N.Mohapatra, S.Nussinov, Y.Zhang

Constraints on neutron-mirror-neutron oscillation from neutron star cooling

NUCLEAR STRUCTURE 1NN; analyzed available data; deduced constraints on neutron-mirror-neutron oscillation.

doi: 10.1140/epjc/s10052-022-10917-6
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2022GU04      Phys.Lett. B 828, 137010 (2022)

S.Guo, X.H.Zhou, C.M.Petrache, E.A.Lawrie, S.H.Mthembu, Y.D.Fang, H.Y.Wu, H.L.Wang, H.Y.Meng, G.S.Li, Y.H.Qiang, J.G.Wang, M.L.Liu, Y.Zheng, B.Ding, W.Q.Zhang, A.Rohilla, K.R.Muhki, Y.Y.Yang, H.J.Ong, J.B.Ma, S.W.Xu, Z.Bai, H.L.Fan, J.F.Huang, J.H.Li, J.H.Xu, B.F.Lv, W.Hua, Z.G.Gan, Y.H.Zhang

Probing the nature of the conjectured low-spin wobbling bands in atomic nuclei

NUCLEAR REACTIONS 175Lu(18O, 6n)187Au, E=108 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, partial level scheme, B(M1)/B(E2), polarization, mixing ratios, low-spin wobbling bands. The Heavy Ion Research Facility in Lanzhou (HIRFL), China.

doi: 10.1016/j.physletb.2022.137010
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2022GU07      Phys.Rev.Lett. 128, 242502 (2022)

S.Guo, B.Ding, X.H.Zhou, Y.B.Wu, J.G.Wang, S.W.Xu, Y.D.Fang, C.M.Petrache, E.A.Lawrie, Y.H.Qiang, Y.Y.Yang, H.J.Ong, J.B.Ma, J.L.Chen, F.Fang, Y.H.Yu, B.F.Lv, F.F.Zeng, Q.B.Zeng, H.Huang, Z.H.Jia, C.X.Jia, W.Liang, Y.Li, N.W.Huang, L.J.Liu, Y.Zheng, W.Q.Zhang, A.Rohilla, Z.Bai, S.L.Jin, K.Wang, F.F.Duan, G.Yang, J.H.Li, J.H.Xu, G.S.Li, M.L.Liu, Z.Liu, Z.G.Gan, M.Wang, Y.H.Zhang

Probing 93mMo Isomer Depletion with an Isomer Beam

RADIOACTIVITY 93Mo(IT) [from 12C(86Kr, 5n), E=559 MeV]; measured decay products, Eγ, Iγ; deduced γ-ray energies and relative intensities, lack of isomer depletion, excitation probability. Comparison with available data. Nuclear excitation by electron capture (NEEC).

doi: 10.1103/PhysRevLett.128.242502
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2022HE08      Phys.Rev. C 105, 044332 (2022)

B.C.He, S.Y.Zhang, L.Li, Y.A.Luo, Y.Zhang, F.Pan, J.P.Draayer

Even-even Nd isotopes in an SD-pair shell model

NUCLEAR STRUCTURE 144,146,148,150,152,154,156Nd; calculated levels, J, π, B(E2). Nucleon pair shell model truncated to SD collective pair subspace (SDPSM). Comparison to experimental data.

doi: 10.1103/PhysRevC.105.044332
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2022HL01      Phys.Rev. C 106, 024319 (2022)

M.Q.Hlatshwayo, Y.Zhang, H.Wibowo, R.LaRose, D.Lacroix, E.Litvinova

Simulating excited states of the Lipkin model on a quantum computer

doi: 10.1103/PhysRevC.106.024319
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2022HU03      J.Phys.(London) G49, 25104 (2022)

J.Hu, Y.Zhang, H.Shen

The Ξ-nuclear potential constrained by recent Ξ-hypernuclei experiments

NUCLEAR STRUCTURE 15C, 14N; analyzed available data; deduced nuclear potential in the quark mean-field (QMF) model.

doi: 10.1088/1361-6471/ac4469
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2022JI03      Chin.Phys.C 46, 014003 (2022)

S.-Y.Jin, Y.-Z.Sun, S.-T.Wang, Z.-Y.Sun, X.-H.Zhang, Z.-Q.Chen, B.Mei, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.B.Ma, X.-M.Liu, R.Han

Fragmentation of stable and neutron-rich 12-16C into boron fragments at approximately 240 MeV/nucleon

NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X)10Be/13B/B, E=240 MeV/nucleon; measured reaction products; deduced σ. Comparison with EPAX3, modified EPAX2, FRACS, NUCFRG2, INCL++, JQMD, and JQMD-2.0 calculations. The ETF of the Institute of Modern Physics, Chinese Academy of Sciences.

doi: 10.1088/1674-1137/ac2ed5
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2022LI03      J.Phys.(London) G49, 25106 (2022)

J.Li, G.Zhang, X.Zhang, Y.Zhang, Z.Liu and F.-S.Zhang

Production of unknown neutron-rich transuranium isotopes 245-249Np, 248-251Pu, 248-254Am, and 252-254Cm in multinucleon transfer reactions

NUCLEAR REACTIONS 238U, 248Cm(238U, X), E(cm)=800 MeV; 249Bk(238U, X), E not given; analyzed available data. 245,246,247,248Np, 248,249,250,251Pu, 248,249,250,251Am, 252,253,254,255Cm; calculated production σ in multinucleon transfer (MNT) reactions using the dinuclear system model with GEMINI code.

doi: 10.1088/1361-6471/ac44ad
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2022LI04      Phys.Lett. B 824, 136829 (2022)

Q.Liu, Y.Zhang, J.-Y.Guo

Pseudospin symmetry in resonant states and its dependence on the shape of potential

NUCLEAR STRUCTURE 132Sn; calculated single-particle levels for neutrons, single particle levels for the pseudospin doublets, wavefunctions of the pseudospin doublets, energies and widths as a function of every potential parameter for the single-particle states, pseudospin energy and width splittings. Dirac equation with a Woods-Saxon potential.

doi: 10.1016/j.physletb.2021.136829
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2022LI30      Phys.Rev. C 105, 064904 (2022)

X.Li, M.Xu, Y.Zhang, Z.Li, Y.Zhou, J.Fu, Y.Wu

Investigations into the characteristics and influences of nonequilibrium evolution

doi: 10.1103/PhysRevC.105.064904
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2022LI39      Phys.Rev. C 106, 014606 (2022)

J.-J.Li, N.Tang, Y.-H.Zhang, X.-R.Zhang, G.Zhang, F.-S.Zhang

Theoretical study on the production of neutron-rich transuranium nuclei with radioactive beams in multinucleon transfer reactions

NUCLEAR REACTIONS 248Cm(136Xe, X)229Pu/230Pu/231Pu/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/233Am/234Am/235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/261Es/262Es , E(cm)=533 MeV; 249Cf(136Xe, X)229Pu/230Pu/231Pu/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/230Am/231Am/232Am/233Am/234Am/235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/233Cm/234Cm/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/236Bk/237Bk/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/237Cf/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/240Es/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es, E(cm)=526 MeV; 238U(92Kr, X)/229Np/230Np/231Np/232Np/233Np/234Np/235Np/236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf, E(cm)=357 MeV; 238U(132Sn, X), 230Np/231Np/232Np/233Np/234Np/235Np/236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np/245Np/246Np/247Np/248Np/249Np/250Np/251Np/252Np/253Np/254Np/255Np/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/255Pu/256Pu/257Pu/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/256Am/257Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/259Cm/260Cm/261Cm/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/261Bk/262Bk/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cm/258Cm/259Cm/260Cm/261Cm/262Cm/263Cm/264Cm, E(cm)=478, 521, 564 MeV; 238U(144Xe, X), 236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np//245Np/246Np/247Np/248Np/249Np/250Np/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/265Bk/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cm/258Cm/259Cm/260Cm/261Cm/262Cm, E(cm)=511 MeV; calculated σ of the isotopes production, driving potential during the transfer of nucleons. Dinuclear system model (DNS) calculations performed with GEMINI++ code. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.014606
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2022LI42      Chin.Phys.C 46, 064001 (2022)

H.-F.Li, X.Xu, M.Wang, Y.-H.Zhang, C.-Y.Fu, W.-J.Huang

On the masses of A = 54 isospin septet and the isobaric multiplet mass equation

NUCLEAR STRUCTURE 52Ni, 54Zn; analyzed available data; deduced the ground-state mass excess of 54Zn. Comparison with the prediction of the quadratic form of the isobaric multiplet mass equation (IMME).

doi: 10.1088/1674-1137/ac5600
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2022LI67      Phys.Rev. C 106, 064316 (2022)

E.Litvinova, Y.Zhang

Microscopic response theory for strongly coupled superfluid fermionic systems

doi: 10.1103/PhysRevC.106.064316
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2022LI72      Phys.Rev. C 106, 065804 (2022)

X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, D.X.Wang, S.Y.Zhang, G.L.Yang, X.K.Li, Z.D.An, J.J.He, W.Luo, X.G.Cao, L.L.Song, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, Y.D.Liu, C.W.Ma, Y.T.Wang, J.Su, L.Y.Zhang, Y.X.Yang, S.Feng, W.B.Liu, W.Q.Su, S.Jin, K.J.Chen

Experimental determination of the neutron resonance peak of 162Er at 67.8 eV

NUCLEAR REACTIONS 162Er(n, γ), E=20-100 eV; measured Eγ, Iγ; deduced neutron-capture yield, resonances, decay widths. Resonance parameters at 67.8 eV are extracted for the first time. R-matrix analysis. Comparison to other experimental results and ENDF/B-VIII.0 data. 4 C6D6 detectors. Neutron beam from Back-n Facility of the CSNS.

doi: 10.1103/PhysRevC.106.065804
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2022ME07      Phys.Rev. C 105, 064604 (2022)

B.Mei, J.Tu, X.Zhang, S.Wang, Y.Guan, Z.Mai, N.Zeng, X.Tu, Z.Sun, S.Tang, Y.Yu, F.Fang, D.Yan, S.Jin, Y.Zhao, S.Ma, Y.Zhang

New experimental evidence for universal odd-even staggering in fragmentation cross sections

NUCLEAR REACTIONS 27Al, 16,17,18O(78Kr, X), E=300 MeV/nucleon; measured reaction products, Bρ, time of flight, ΔE; deduced production yields, odd-even staggering (OES) in fragmentation reaction for Z=5-45 with N-Z from 1–9. Systematics of odd-even staggering magnitudes for 78Kr+Al2O3, 78Kr+Be, 84Kr+112,124Sn and 86Kr+Be/Ta. Fragmentation on Al2O3 target at RIBLL2 separator at the Heavy-Ion Research Facility in Lanzhou (HIRFL).

doi: 10.1103/PhysRevC.105.064604
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2022RE08      Phys.Rev. A 106, 012805 (2022)

B.Ren, P.Ma, Y.Zhang, L.Wei, J.Han, Z.Xia, J.Wang, T.Meng, W.Yu, Y.Zou, C.-L.Yang, B.Wei

Dissociation mechanism of C2H42+ induced by 18-keV/u Ne8+ impact: Symmetric and isomeric cleavage of the C-C bond

NUCLEAR REACTIONS C, H(Ne, X), E=18 keV/nucleon; measured reaction products; deduced kinetic-energy release (KER) distributions, C-C bond cleavage dissociation of ethylene dication. Comparison with calculations. The COLTRIMS setup at Fudan University.

doi: 10.1103/PhysRevA.106.012805
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2022SI05      Phys.Rev. C 105, 024907 (2022)

F.Si, Y.Zhang

Statistical uncertainty estimation of higher-order cumulants with finite efficiency and its application in heavy-ion collisions

doi: 10.1103/PhysRevC.105.024907
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2022WA03      Phys.Lett. B 825, 136856 (2022)

Y.Wang, F.Guan, Q.Wu, X.Diao, Y.Huang, L.M.Lyu, Y.Qin, Z.Qin, D.Si, Z.Bai, F.Duan, L.Duan, Z.Gao, Q.Hu, R.J.Hu, G.Jin, S.Jin, J.Ma, P.Ma, J.Wang, P.Wang, Y.Wang, X.Wei, H.Yang, Y.Yang, G.Yu, Y.Yu, Y.Zhang, Q.Zhou, Y.Zhang, C.Ma, X.Hu, H.Wang, Y.Cui, J.Tian, Z.Xiao

The emission order of hydrogen isotopes via correlation functions in 30 MeV/u Ar+Au reactions

NUCLEAR REACTIONS 197Au(40Ar, X)1H/2H/3H, E=30 MeV/nucleon; measured reaction products, Ep, Ip; deduced correlation functions, emission rates. The Compact Spectrometer for Heavy IoN Experiment (CSHINE), the Heavy Ion Research Facility at Lanzhou (HIRFL).

doi: 10.1016/j.physletb.2021.136856
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2022WA39      Phys.Rev. C 106, L051301 (2022)

M.Wang, M.Zhang, X.Zhou, Y.H.Zhang, Yu.A.Litvinov, H.S.Xu, R.J.Chen, H.Y.Deng, C.Y.Fu, W.W.Ge, H.F.Li, T.Liao, S.A.Litvinov, P.Shuai, J.Y.Shi, M.Si, R.S.Sidhu, Y.N.Song, M.Z.Sun, S.Suzuki, Q.Wang, Y.M.Xing, X.Xu, T.Yamaguchi, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, X.H.Zhou

Bρ-defined isochronous mass spectrometry: An approach for high-precision mass measurements of short-lived nuclei

ATOMIC MASSES 44,44mV, 46Cr, 48Mn, 50,51Fe, 52,52mCo, 54Ni, 56Cu, 43Ti; measured velocity and revolution time of stored ions; deduced mass excess. 52Co; deduced S(p). Introduced technique for broadband high-precision mass spectrometry based on simultaneous determinations of revolution time and velocity of short-lived stored ions at the cooler storage ring CSRe in Lanzhou.Comparison to AME2020 values and other experimental results.

RADIOACTIVITY 46Cr, 50Fe, 54Ni(EC); deduced Q values, ft using the values of mass excess obtained in this paper.

doi: 10.1103/PhysRevC.106.L051301
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2022WA43      Phys.Rev. C 106, 064325 (2022)

X.D.Wang, B.Qi, C.Liu, A.Rohilla, Y.Zhang

Restored symmetries for the observed excited alternating-parity band in even-even nuclei

NUCLEAR STRUCTURE 148Ce; calculated levels, J, π, bands structure, high-spin states, energies of states as functions of triaxial parameter, transi tion strengths ratios for the ground and excited alternating-parity bands - B(E1)/B(E2), B(E2)/B(E2), probability distribution of the total angular momentum. Comparison to experimental results.

doi: 10.1103/PhysRevC.106.064325
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2022WU15      Chin.Phys.C 46, 104101 (2022)

Y.-Q.Wu, W.Teng, X.-J.Hou, G.-X.Na, Y.Zhang, B.-C.He, Y.-A.Luo

Spectral fluctuations in the interacting boson model

doi: 10.1088/1674-1137/ac76a5
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2022XU06      Phys.Lett. B 833, 137287 (2022), Priv.Comm.

W.Z.Xu, S.Y.Wang, C.Liu, X.G.Wu, R.J.Guo, B.Qi, J.Zhao, A.Rohilla, H.Jia, G.S.Li, Y.Zheng, C.B.Li, X.C.Han, L.Mu, X.Xiao, S.Wang, D.P.Sun, Z.Q.Li, Y.M.Zhang, C.L.Wang, Y.Li

Interplay between nuclear chiral and reflection symmetry breakings revealed by the lifetime measurements in 76Br

NUCLEAR REACTIONS 68Zn(12C, 3np)76Br, E=66 MeV; measured reaction products, Eγ, Iγ, γγ-coin, γγ(θ)(ADO). 76Br; deduced γ-ray energies and relative intensities, high-spin levels, J, π, multipolarities, B(M1), B(E2), bands, chirality, level T1/2. Comparison with triaxial particle rotor model (TPRM), and multidimensional-constrained covariant density function (MDC-CDFT) calculations. The Doppler-shift attenuation method (DSAM), one LEPS detector and nine Compton-suppressed HPGe detectors. HI-13 Tandem Accelerator of the China Institute of Atomic Energy (CIAE).

doi: 10.1016/j.physletb.2022.137287
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2022XU12      Chin.Phys.C 46, 111001 (2022)

Xi.-D.Xu, Y.-Z.Sun, S.-T.Wang, B.Mei, S.-Y.Jin, X.-H.Zhang, Z.-Y.Sun, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.-B.Ma

Isotopic production cross sections of fragmentation residues produced by 18O ions on a carbon target near 260 MeV/nucleon

NUCLEAR REACTIONS C(18O, X)14N/15C/12C/12B/13B/10B, E=260 MeV/nucleon; measured reaction products, TOF; deduced isotopic σ. Comparison with available data. The HIRFL facility in Lanzhou (China).

doi: 10.1088/1674-1137/ac827c
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2022YA15      Phys.Rev. C 105, L051302 (2022)

H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, C.X.Yuan, Y.F.Niu, C.L.Yang, Y.L.Tian, L.Guo, Y.S.Wang, J.G.Wang, H.B.Zhou, X.J.Wen, H.R.Yang, X.H.Zhou, Y.H.Zhang, W.X.Huang, Z.Liu, S.G.Zhou, Z.Z.Ren, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, D.I.Solovyev

New isotope 207Th and odd-even staggering in α-decay energies for nuclei with Z > 82 and N < 126

RADIOACTIVITY 207Th(α)[from 176Hf(36Ar, 5n), E=197-199 MeV]; 208Th(α)[from 176Hf(36Ar, 4n), E=197-199 MeV]; 203Ra, 199Rn, 195Po(α)[from 207Th α-decay chain]; 204Ra, 200Rn, 196Po(α)[from 208Th α-decay chain]; measured evaporation residues (ERs), Eα, and ER-α1234 correlated α-decay chain from the decays of 207Th and208Th. 207,208Th; deduced α-decay T1/2, production σ. Z=84-92, N=102-126; discussed systematics of experimental and theoretically calculated (by relativistic Hartree-Fock-Bogoliubov and large-scale shell-model approaches) odd-even staggering (OES) of Q(α), Q(proton) and Q(neutron). Position-sensitive silicon strip detectors (PSSDs), non-position sensitive Si detectors, and SHANS gas-filled recoil separator at the sector focusing cyclotron facility of HIRFL, Lanzhou.

doi: 10.1103/PhysRevC.105.L051302
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2022YA27      Phys.Rev. C 106, 064311 (2022)

H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, C.L.Yang, Y.L.Tian, Y.S.Wang, H.B.Zhou, X.J.Wen, J.G.Wang, Z.Zhao, S.Y.Xu, L.X.Chen, X.Y.Huang, C.X.Yuan, Y.F.Niu, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, S.G.Zhou, Z.Z.Ren, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, D.I.Solovyev

Examining the impact of α-decay energies on the odd-even staggering in half-lives: α-decay spectroscopy of 207-209Ac

RADIOACTIVITY 207,208,208m,209Ac(α)[from 176Hf(36Ar, X), E=197-199 MeV]; measured evaporation residues (ER), Eα, Iα, αα-coin, (ER)αα-coin; deduced T1/2, Q values, decay branches. 204mFr(IT) [from 208Ac(α)]; deduced T1/2, isomer level energy, tentative J and π for the newly found 80-keV isomer. 204Fr(α)[from 208,208mAc(α)]; deduced T1/2. Found new α-decay branching 208Ac and assigned to the transition from ground state to the excited (2+, 4+) state. Comparison to the calculations performed in the framework of Wentzel-Kramers-Brillouin approximation. Spectrometer for Heavy Atoms and Nuclear Structure (SHANS) at Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL).

doi: 10.1103/PhysRevC.106.064311
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2022ZH10      Prog.Theor.Exp.Phys. 2022, 023D01 (2022)

Y.Zhang, H.Sagawa, E.Hiyama

Prediction of exotic hyperon halos in neutron-rich Zr hypernuclei

NUCLEAR STRUCTURE 90,91,92Zr, 114,115,116Zr, 136,137,138Zr; calculated neutron single-particle energies and potentials in the hypernuclei, occupation probabilities with the Skyrme HFB model. Comparison with available data.

doi: 10.1093/ptep/ptac004
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2022ZH19      Phys.Rev. C 105, 044326 (2022)

Y.Zhang, A.Bjelcic, T.Niksic, E.Litvinova, P.Ring, P.Schuck

Many-body approach to superfluid nuclei in axial geometry

NUCLEAR STRUCTURE 28Si; calculated single-particle energies, Nilsson diagram, strength of the neutron states, low-energy isoscalar strength functions for varying quadrupole deformation, deformation parameters. 250Cf; calculated deformation parameters. 249,251Cf; calculated single-quasiparticle neutron states. Finite amplitude quasiparticle random phase approximation method. Comparison to experimental data.

doi: 10.1103/PhysRevC.105.044326
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2022ZH42      Phys.Rev. C 106, 014625 (2022)

Y.-H.Zhang, G.Zhang, J.-J.Li, Z.Liu, A.V.Yeremin, F.-S.Zhang

Production cross sections of 243-248No isotopes in fusion reactions

NUCLEAR REACTIONS 208Pb(48Ca, X), E(cm)=165-220 MeV; 238U(20Ne, X), E(cm)=95-14 MeV; 242Pu(16O, X), E(cm)=80-130 MeV; 232Th(26Mg, X), E(cm)=110-160 MeV; 208Pb(48Ca, 2n), E(cm)=170-245 MeV; 208Pb(48Ca, 3n), E(cm)=180-258 MeV; 208Pb(48Ca, 4n), E(cm)=190-275 MeV; 208Pb(48Ca, 5n), E(cm)=200-280 MeV; 208Pb(40Ca, 2n), E(cm)=160-190 MeV; 208Pb(40Ca, 3n), E(cm)=170-200 MeV; 208Pb(40Ca, 4n), E(cm)=175-215 MeV; 208Pb(40Ca, 5n), E(cm)=200-220 MeV; 208Pb(44Ca, 2n), E(cm)=170-200 MeV; 208Pb(44Ca, 3n), E(cm)=175-210 MeV; 208Pb(44Ca, 4n), E(cm)=175-215 MeV; 208Pb(44Ca, 5n), E(cm)=180-225 MeV; 233U(20Ne, 4n), E(cm)=90-135 MeV; 233U(20Ne, 5n), E(cm)=105-140 MeV; 233U(20Ne, n), E(cm)=115-140 MeV; 235U(20Ne, 4n), E(cm)=90-135 MeV; 235U(20Ne, 5n), E(cm)=100-140 MeV; 235U(20Ne, n), E(cm)=110-140 MeV; 238U(20Ne, 4n), E(cm)=90-135 MeV; 238U(20Ne, 5n), E(cm)=95-140 MeV; 238U(20Ne, n), E(cm)=105-140 MeV; calculated σ(E), time evolution of binding energies and root-mean-square charge radii for 48Ca and 208Pb, excitation functions, static barrier in collision, evolution density profile for heads-on collision, production σ for new isotopes - 243,244,245,246,247,248No.Improved quantum molecular dynamical model (ImQMD) incorporated with a statistical model and the dinuclear system (DNS) model calculations. Comparison to available experimental data.

doi: 10.1103/PhysRevC.106.014625
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2022ZH45      Phys.Rev. C 106, 024305 (2022)

M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Zhang, Z.G.Gan, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, J.G.Wang, C.X.Yuan, C.Qi, A.N.Andreyev, X.Y.Huang, S.Y.Xu, Z.Zhao, L.X.Chen, J.Y.Wang, M.L.Liu, Y.H.Qiang, G.S.Li, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Y.F.Niu, L.Guo, Z.Z.Ren, S.G.Zhou

Fine structure in the α decay of the 8+ isomer in 216, 218U

RADIOACTIVITY 216,216m,218,218mU(α)[218U from 182W(40Ar, 4n), E=190 MeV, 184W(40Ca, 2nα), E=206 MeV, 216U from 180W(40Ar, 4n), E=191 MeV]; measured evaporation residues (EVRs), Eα, Iα, (EVR)α12-correlations, T1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. 216,216m,218,218mU; deduced T1/2, Q-values, α-branching ratio, α-decay hindrance factors. 204Rn, 208,210Ra, 212,214Th(α)[from 216,218U α-decay chains]; measured Eα, T1/2. 212Th; deduced level, J, π, identification of the first 2+ state. 215Ra, 212,213,216Ac, 211,212,213,214,216,216m,217Th, 216,217,217m,218Pa, 217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.106.024305
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2022ZH60      Nature(London) 610, 656 (2022)

L.Zhang, J.He, R.J.deBoer, M.Wiescher, A.Heger, D.Kahl, J.Su, D.Odell, Y.Chen, X.Li, J.Wang, L.Zhang, F.Cao, H.Zhang, Z.Zhang, X.Jiang, L.Wang, Z.Li, L.Song, H.Zhao, L.Sun, Q.Wu, J.Li, B.Cui, L.Chen, R.Ma, E.Li, G.Lian, Y.D.Sheng, Z.Li, B.Guo, X.Zhou, Y.Zhang, H.Xu, J.Cheng, W.Liu

Measurement of 19F(p, γ)20Ne reaction suggests CNO breakout in first stars

NUCLEAR REACTIONS 19F(p, γ), E(cm)<400 keV; measured reaction products, Eγ, Iγ; deduced yields, S-factor, resonance strengths, astrophysical reaction rates. Comparison with available data. The Jinping Underground Nuclear Astrophysics Experiment (JUNA).

doi: 10.1038/s41586-022-05230-x
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2022ZH62      Phys.Rev. C 106, L051303 (2022)

Y.Zhang, Y.Bao, H.Shen, J.Hu

Resolving the spurious-state problem in the Dirac equation with the finite-difference method

NUCLEAR STRUCTURE 132Sn; calculated neutron energy levels, neutron wave functions. Solved spurious-state problem appearing while solving Dirac equations with finite-difference method, by replacing the central difference formula with the asymmetric difference formula.

doi: 10.1103/PhysRevC.106.L051303
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2022ZH77      Sci. Rep. 12, 19264 (2022)

X.Zhou, J.Wei, Ru.Cheng, Y.Zhang, Y.Chen, C.Liang, X.Zhang, Y.Zhao

Au L-shell x-ray emission induced by 154.3-423.9 MeV/u C6+ ions

NUCLEAR REACTIONS 197Au(12C, X), E=154.3-423.9 MeV/nucleon; measured reaction products, X-rays; deduced L-shell X-ray spectra, relative intensity ratios, production σ. Comparison with calculations. The cancer therapy termina l at the national laboratory of Heavy Ion Research Facility in Lanzhou (HIRFL) in the Institute of Modern Physics, Chinese Academic of Science (IMP, CAS).

doi: 10.1038/s41598-022-23830-5
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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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2021CA31      Phys.Rev. C 104, 065502 (2021)

M.Cadeddu, N.Cargioli, F.Dordei, C.Giunti, Y.F.Li, E.Picciau, C.A.Ternes, Y.Y.Zhang

New insights into nuclear physics and weak mixing angle using electroweak probes

NUCLEAR REACTIONS 133Cs, 127I(ν, ν), E=2-100 MeV; analyzed coherent elastic neutrino-nucleus scattering data in cesium-iodide crystal from the COHERENT experiment, and from atomic parity violation (APV) experiment. 133Cs, 127I; deduced most precise neutron rms radii, and the neutron skin values, independent low-energy weak mixing angle with uncertainty and compared with standard model prediction. 127I, 133Cs, 208Pb; calculated rms proton and neutron point and physical radii and the neutron skins using nonrelativistic Skyrme-Hartree-Fock (SHF) and relativistic mean-field (RMF) nuclear models, point neutron skin predictions for 208Pb and 133Cs according to different models and comparisons with data from PREX-I, PREX-II, and COHERENT+APV experiments.

doi: 10.1103/PhysRevC.104.065502
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2021CH17      Phys.Rev. C 103, L031302 (2021)

J.Chen, S.M.Wang, H.T.Fortune, J.L.Lou, Y.L.Ye, Z.H.Li, N.Michel, J.G.Li, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, D.Y.Pang, F.R.Xu, W.Zuo, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, H.J.Ong, E.Ideguchi, Y.Ayyad, K.Hatanaka, D.T.Tran, D.Bazin, J.Lee, Y.N.Zhang, J.Wu, H.N.Liu, C.Wen, T.Yamamoto, M.Tanaka, T.Suzuki

Observation of the near-threshold intruder 0- resonance in 12Be

NUCLEAR REACTIONS 2H(11Be, p)12Be, E=26.9 MeV/nucleon; measured E(p), I(p), σ(θ) using two parallel-plate avalanche counters (PPACs), and a set of annular double-sided silicon detectors (ADSSDs) at the RCNP, Osaka University. 12Be; deduced missing-mass spectra of 12Be unbound states, levels, J, π, a 0- resonance just above S(n), decay width. DWBA analysis. Comparison with Gamow coupled-channel and Gamow shell-model calculations.

doi: 10.1103/PhysRevC.103.L031302
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2021CH19      Phys.Rev.Lett. 126, 132501 (2021)

R.J.Charity, T.B.Webb, J.M.Elson, D.E.M.Hoff, C.D.Pruitt, L.G.Sobotka, K.W.Brown, G.Cerizza, J.Estee, W.G.Lynch, J.Manfredi, P.Morfouace, C.Santamaria, S.Sweany, C.Y.Tsang, M.B.Tsang, Y.Zhang, K.Zhu, S.A.Kuvin, D.McNeel, J.Smith, A.H.Wuosmaa, Z.Chajecki

Observation of the Exotic Isotope 13F Located Four Neutrons beyond the Proton Drip Line

NUCLEAR REACTIONS 9Be(13O, 13F), E=69.5 MeV/nucleon; measured reaction products, Ep, Ip. 13F, 12O, 11N, 10C, 9B, 8Be; deduced 13F resonance parameters, energy levels, J, π, level decays via initial proton emissions.

doi: 10.1103/PhysRevLett.126.132501
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2021CH39      Chin.Phys.C 48, 084101 (2021)

Y.-J.Chen, Y.-Y.Liu, L.-L.Liu, F.-Y.Wang, Y.-X.Zhang

Understanding the isoscaling relationship in the fissioning system with evaluated data

NUCLEAR REACTIONS 233,235U(n, F), E<20 MeV; analyzed available data; deduced isoscaling parameters in the fissioning systems. ENDF/B-VIII.0 and JEFF-3.3 evaluated libraries.

doi: 10.1088/1674-1137/ac0035
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2021CH46      J.Radioanal.Nucl.Chem. 329, 1393 (2021)

C.Chu, G.Hu, X.Guo, Q.Liu, W.Li, F.Hao, Q.Xiang, J.Zeng, Y.Zhang

Half-life determination of 88Kr based on rapid Kr-Xe separation

RADIOACTIVITY 88Kr(β-) [from U(n, F), E thermal]; measured decay products, Eγ, Iγ; deduced γ-ray energies, T1/2 and uncertainties. Comparison with available data.

doi: 10.1007/s10967-021-07881-y
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2021CO10      Phys.Rev. C 104, 024603 (2021)

M.Colonna, Y.-X.Zhang, Y.-J.Wang, D.Cozma, P.Danielewicz, C.M.Ko, A.Ono, M.B.Tsang, R.Wang, H.Wolter, J.Xu, Z.Zhang, L.-W.Chen, H.-G.Cheng, H.Elfner, Z.-Q.Feng, M.Kim, Y.Kim, S.Jeon, C.-H.Lee, B.-A.Li, Q.-F.Li, Z.-X.Li, S.Mallik, D.Oliinychenko, J.Su, T.Song, A.Sorensen, F.-S.Zhang

Comparison of heavy-ion transport simulations: Mean-field dynamics in a box

doi: 10.1103/PhysRevC.104.024603
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2021DE24      Eur.Phys.J. A 57, 242 (2021)

X.G.Deng, Y.G.Ma, Y.X.Zhang

Green-Kubo formula for Boltzmann and Fermi-Dirac statistics

doi: 10.1140/epja/s10050-021-00550-4
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2021DI06      Nucl.Phys. A1014, 122237 (2021)

X.Ding, J.Hu, Y.Zhang, H.Shen

Neutron drop trapped in axially deformed external fields

NUCLEAR STRUCTURE N=28; calculated energy levels, J, π using an axially symmetric harmonic oscillator (ASHO) potential within the Skyrme HFB model.

doi: 10.1016/j.nuclphysa.2021.122237
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2021DI09      Phys.Rev. C 104, 064304 (2021)

B.Ding, C.M.Petrache, S.Guo, E.A.Lawrie, I.Wakudyanaye, Z.H.Zhang, H.L.Wang, H.Y.Meng, D.Mengoni, Y.H.Qiang, J.G.Wang, C.Andreoiu, A.Astier, A.Avaa, T.Back, R.A.Bark, D.Bazzacco, A.Boso, T.D.Bucher, B.Cederwall, M.V.Chisapi, H.L.Fan, F.Galtarossa, F.H.Garcia, A.Goasduff, G.Jaworski, P.Jones, I.Kuti, J.J.Lawrie, G.S.Li, R.Li, M.L.Liu, Z.Liu, B.Lomberg, B.F.Lv, T.Marchlewski, L.Mdletshe, L.Msebi, S.H.Mthembu, D.R.Napoli, A.Netshiya, M.F.Nkalanga, J.N.Orce, K.Ortner, F.Recchia, S.Riccetto, A.Rohilla, T.W.Seakamela, M.Siciliano, M.A.Sithole, D.Sohler, J.Srebrny, D.Testov, A.Tucholski, J.J.Valiente-Dobon, F.Wentzel, K.Whitmore, Y.H.Zhang, K.K.Zheng, X.H.Zhou, B.R.Zikhali

Signature splitting of the g7/2 [404] 7/2+ bands in 131Ba and 133Ce

NUCLEAR REACTIONS 122Sn(13C, 4nγ)131Ba, E=65 MeV from XTU Tandem accelerator at LNL-Legnaro; 125Te(12C, 4nγ)133Ce, E=57 MeV from separated sector cyclotron of iThemba LABS; measured Eγ, Iγ, γγ-coin, γγ(θ) using GALILEO array of 25 Compton-suppressed HPGe detectors, EUCLIDES silicon ball for charged particles and the Neutron Wall array for neutrons for 131Ba at Legnaro, and AFRODITE array of eight Compton-suppressed clover detectors for 133Ce at iThemba LABS. 131Ba, 133Ce; deduced high-spin levels, multipolarities, J, π, bands, quasiparticle alignments, dynamical moments of inertia, signature splittings and configurations. Comparison with cranked shell model and quasiparticle-plus-triaxial-rotor model calculations.

doi: 10.1103/PhysRevC.104.064304
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2021DO07      J.Phys.(London) G48, 045103 (2021)

W.-T.Dong, Y.Zhang, B.-C.He, F.Pan, Y.-A.Luo, J.P.Draayer, S.Karampagia

Statistical analysis of the excited-state quantum phase transitions in the interacting boson model

doi: 10.1088/1361-6471/abdd8c
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2021JI16      Symmetry 13, 2278 (2021)

H.Jian, Y.Gao, F.Dai, J.Liu, X.Xu, C.Yuan, K.Kaneko, Y.Sun, P.Liang, G.Shi, L.Sun, L.Xayavong, C.Lin, J.Lee, Z.Li, Y.Yang, P.Li, R.Fan, S.Zha, H.Zhu, J.Li, Q.Gao, Z.Zhang, R.Chen, J.Wang, D.Wang, H.Wu, K.Wang, Y.Lam, F.Duan, P.Ma, Z.Gao, Q.Hu, Z.Bai, J.Ma, J.Wang, F.Zhong, C.Wu, D.Luo, Y.Jiang, Y.Liu, D.Hou, R.Li, N.Ma, W.Ma, G.Yu, D.Patel, S.Jin, Y.Wang, Y.Yu, Q.Zhou, P.Wang, L.Hu, X.Wang, H.L.Zang, Q.Zhao, L.Yang, P.Wen, F.Yang, H.Jia, G.Zhang, M.Pan, X.Wang, H.Sun, M.Wang, Z.Hu, X.Zhou, Y.Zhang, H.Xu, M.Liu, H.-J.Ong, W.Yang

β-Delayed γ Emissions of 26P and Its Mirror Asymmetry

RADIOACTIVITY 26P(β+), (EC) [from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation using RIBBL1 at HRIBF, Lanzhou facility]; measured Eγ, Iγ, βγ-coin, T1/2 of 26P decay. 26Si; deduced levels, J, π, β++ϵ feedings, logft, mirror asymmetry parameter from comparison with the ϵ decay of mirror nucleus 26Na to 26Mg, mirror-energy differences (MEDs), and halo structure in 26P. Comparison with shell-model calculations.

NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P/27S, E=80.6 MeV/nucleon; measured reaction products, particle-identification (PID) plot of ΔE vs TOF for the ions separated using RIBBL1 separator at HRIBF, Lanzhou facility.

doi: 10.3390/sym13122278
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2021KA39      Phys.Lett. B 822, 136681 (2021)

M.Kaneko, T.Murakami, T.Isobe, M.Kurata-Nishimura, A.Ono, N.Ikeno, J.Barney, G.Cerizza, J.Estee, G.Jhang, J.W.Lee, W.G.Lynch, C.Santamaria, C.Y.Tsang, M.B.Tsang, R.Wang, D.S.Ahn, L.Atar, T.Aumann, H.Baba, K.Boretzky, J.Brzychczyk, N.Chiga, N.Fukuda, I.Gasparic, B.Hong, A.Horvat, T.Ichihara, K.Ieki, N.Inabe, Y.J.Kim, T.Kobayashi, Y.Kondo, P.Lasko, H.S.Lee, Y.Leifels, J.Lukasik, J.Manfredi, A.B.McIntosh, P.Morfouace, T.Nakamura, N.Nakatsuka, S.Nishimura, R.Olsen, H.Otsu, P.Pawlowski, K.Pelczar, D.Rossi, H.Sakurai, H.Sato, H.Scheit, R.Shane, Y.Shimizu, H.Simon, T.Sumikama, D.Suzuki, H.Suzuki, H.Takeda, S.Tangwancharoen, Y.Togano, H.Tornqvist, Z.Xiao, S.J.Yennello, J.Yurkon, Y.Zhang

Rapidity distributions of Z=1 isotopes and the nuclear symmetry energy from Sn+Sn collisions with radioactive beams at 270 MeV/nucleon

NUCLEAR REACTIONS 124Sn(132Sn, X), 112Sn(108Sn, X), E=270 MeV/nucleon; measured reaction products. 1,2,3H; deduced rapidity distributions of hydrogen isotopes emitted from central collisions. Comparison with antisymmetrized molecular dynamics (AMD) calculations. RIKEN-RIBF facility.

doi: 10.1016/j.physletb.2021.136681
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2021LI01      Phys.Rev. C 103, 014616 (2021)

Y.Liu, Y.Wang, Y.Cui, C.-J.Xia, Z.Li, Y.Chen, Q.Li, Y.Zhang

Insights into the pion production mechanism and the symmetry energy at high density

doi: 10.1103/PhysRevC.103.014616
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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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2021LI56      Phys.Rev. C 104, 044303 (2021)

E.Litvinova, Y.Zhang

Many-body theory for quasiparticle states in superfluid fermionic systems

doi: 10.1103/PhysRevC.104.044303
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2021LI61      Phys.Rev. C 104, 054302 (2021)

X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, X.G.Cao, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, J.C.Wang, D.X.Wang, S.Y.Zhang, Y.D.Liu, X.Ma, C.W.Ma, Y.T.Wang, Z.D.An, J.J.He, J.Su, L.Y.Zhang, Y.X.Yang, W.B.Liu, W.Q.Su

New experimental measurement of natEr(n, γ) cross sections between 1 and 100 eV

NUCLEAR REACTIONS 162,164,166,167,168,170Er, 12,13C, 197Au(n, γ), E=0.001-100 keV; measured E(n), I(n), Eγ, Iγ using C6D6 liquid scintillator and a silicon monitor and natural Er, C and Au targets at the China spallation neutron source (CSNS) facility; deduced neutron-capture σ(E), capture yields as function of E(n), neutron resonances in Er isotopes in the 1-100 eV region. 162,164,166,167,168Er; deduced energies of 43 neutron resonances (nine for 162Er, five for 164Er, three for 166Er, 25 for 167Er, one for 168Er), cross sections, widths Γγ and Γn by R-matrix analysis. Comparison with previous experimental data, and with data in evaluated databases ENDF/B-VIII.0, ENDF/B-VII.1, JENDL-4.0, and ROSFOND-2010.

doi: 10.1103/PhysRevC.104.054302
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2021MA39      Phys.Rev. C 103, L061302 (2021)

W.H.Ma, D.Patel, Y.Y.Yang, J.S.Wang, Y.Kanada-En'yo, R.F.Chen, J.Lubian, Y.L.Ye, Z.H.Yang, Z.Z.Ren, S.Mukherjee, J.B.Ma, S.L.Jin, P.Ma, J.X.Li, Y.S.Song, Q.Hu, Z.Bai, M.R.Huang, X.Q.Liu, Y.J.Zhou, J.Chen, Z.H.Gao, F.F.Duan, S.Y.Jin, S.W.Xu, G.M.Yu, G.Z.Shi, Q.Wang, T.F.Wang, X.Y.Ju, Z.G.Hu, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan

Observation of 6He + t cluster states in 9Li

NUCLEAR REACTIONS 208Pb(9Li, X), E=32.7 MeV/nucleon, [secondary 9Li beam from 9Be(12C, X), E=53.7 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility]; measured reaction products and outgoing charged particles, angular distributions of charged particles using Si telescope and CsI(Tl) scintillator array. 9Li; deduced resonant states, relative energy spectrum of 6He+t cluster states from the decay of 9Li resonances, differential breakup cross-section, isoscalar monopole transition matrix element M(IS0) and monopole strength B(IS0), energy-weighted sum rule (EWSR) for the transferred angular momentum. DWBA and CDCC analysis of angular distributions, and GCM calculations for the cluster states in 9Li. Relevance to differences between the triton and α clusters, and impact of these differences on the formation of nuclei containing triton clusters.

doi: 10.1103/PhysRevC.103.L061302
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2021MA60      Prog.Part.Nucl.Phys. 121, 103911 (2021)

C.-W.Ma, H.-L.Wei, X.-Q.Liu, J.Su, H.Zheng, W.P.Lin, Y.-X.Zhang

Nuclear fragments in projectile fragmentation reactions

doi: 10.1016/j.ppnp.2021.103911
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2021MA84      J.Phys.(London) G48, 125107 (2021)

A.J.Majarshin, Y.-A.Luo, F.Pan, H.T.Fortune, Y.Zhang, J.P.Draayer

Quantum phase transitions and band mixing in 135Ba

NUCLEAR STRUCTURE 134,135Ba; calculated variation of some excitation energy levels, energy differences and ratios in odd systems, B(E2), energy spectra. Comparison with available data.

doi: 10.1088/1361-6471/ac2fb1
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2021ME13      Chin.Phys.C 45, 054001 (2021)

B.Mei, D.L.Balabanski, W.Hua, Y.-H.Zhang, X.-H.Zhou, C.-X.Yuan, J.Su

Fusion reactions around the barrier for Be+238U

NUCLEAR REACTIONS 238U(9Be, 5n)242Cm, E=35-70 MeV; measured reaction products, Eα, Iα; deduced σ. Comparison with model calculations through two different codes, namely HIVAP2 and KEWPIE2, using two methods (i.e., WKB and EBD) for the capture probability.

doi: 10.1088/1674-1137/abe36c
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