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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


2024GA08      Phys.Rev. C 109, 024601 (2024)

Z.Gao, S.Liu, P.Wen, Z.Liao, Y.Yang, J.Su, Y.Wang, L.Zhu

Constraining the Woods-Saxon potential in fusion reactions based on the neural network

doi: 10.1103/PhysRevC.109.024601
Citations: PlumX Metrics


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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2024LI11      Phys.Rev. C 109, 024604 (2024)

Zh.Li, Z.Gao, L.Liu, Y.Wang, L.Zhu, Q.Li

Importance of physical information on the prediction of heavy-ion fusion cross sections with machine learning

doi: 10.1103/PhysRevC.109.024604
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2024WA03      Phys.Rev. C 109, 014621 (2024)

Y.H.Wang, D.Y.Pang, W.D.Chen, Y.P.Xu, W.L.Hai, R.Y.Chen

Nuclear radii from total reaction cross section measurements at intermediate energies with complex turning point corrections to the eikonal model

doi: 10.1103/PhysRevC.109.014621
Citations: PlumX Metrics


2024WA06      Phys.Rev. C 109, 015201 (2024)

Y.Wang, X.-J.Wen

Isospin asymmetric matter in uniform and nonuniform strong magnetic fields

doi: 10.1103/PhysRevC.109.015201
Citations: PlumX Metrics


2024WA07      Phys.Rev. C 109, 015202 (2024)

Y.-F.Wang, U.-G.Meissner, D.Ronchen, Ch.-W.Shen

Examination of the nature of the N* and Δ resonances via coupled-channels dynamics

doi: 10.1103/PhysRevC.109.015202
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2024WA09      Phys.Lett. B 849, 138449 (2024)

H.-K.Wang, H.Yang, M.L.Liu, Y.B.Wang, B.Jiang, Y.B.Qian

Ground-state inversion: The monopole-force governance in neutron mid-shell region

NUCLEAR STRUCTURE 117,119,121,123,125,127,129,131,133Sb; analyzed available data; deduced the evolution of single-proton states, the monopole force interaction, the ground-state inversion, the monopole force can sufficiently extend the present Hamiltonian to include the mid-shell region.

doi: 10.1016/j.physletb.2024.138449
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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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2024YA04      Phys.Rev.Lett. 132, 072502 (2024)

H.B.Yang, Z.G.Gan, Y.J.Li, M.L.Liu, S.Y.Xu, C.Liu, M.M.Zhang, Z.Y.Zhang, M.H.Huang, C.X.Yuan, S.Y.Wang, L.Ma, J.G.Wang, X.C.Han, A.Rohilla, S.Q.Zuo, X.Xiao, X.B.Zhang, L.Zhu, Z.F.Yue, Y.L.Tian, Y.S.Wang, C.L.Yang, Z.Zhao, X.Y.Huang, Z.C.Li, L.C.Sun, J.Y.Wang, H.R.Yang, Z.W.Lu, W.Q.Yang, X.H.Zhou, W.X.Huang, N.Wang, S.G.Zhou, Z.Z.Ren, H.S.Xu

Discovery of New Isotopes 160Os and 156W: Revealing Enhanced Stability of the N=82 Shell Closure on the Neutron-Deficient Side

NUCLEAR REACTIONS 106Cd(58Ni, 4n)160Os, E=335 MeV; measured reaction products; deduced new isotopes, σ. The Spectrometer for Heavy Atoms and Nuclear Structure (SHANS), the Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL), China.

RADIOACTIVITY 160Os(α), 156W(β+); measured decay products, Eα, Iα; deduced α-particles energies, Q-values, T1/2, α-decay reduced widths, N=82 shell closure toward the proton drip line. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.132.072502
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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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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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2023DA07      J.Phys.(London) G50, 045102 (2023)

X.R.Dai, Y.Y.Wang, D.Li, W.J.Zhao, Y.F.Han, X.Y.Han, K.H.Fang

Cross section measurements for 9Be(d, t)8Be reaction at the low-energy region (E ≤ 100 keV)

NUCLEAR REACTIONS 9Be(d, t), E=78-100 keV; measured reaction products; deduced thick-target yields, σ and uncertainties. The low-energy, high-current accelerators at Research Center for Electron Photon Science in Tohoku University.

doi: 10.1088/1361-6471/acb507
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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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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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2023LI05      Phys.Rev. C 107, 014307 (2023)

J.Lin, Y.K.Wang, C.Xu, Z.H.Li, H.Hua, S.Q.Zhang, D.W.Luo, H.Y.Wu, J.Meng, X.G.Wu, Y.Zheng, C.B.Li, T.X.Li, Z.Y.Huang, H.Cheng, C.Y.Guo, Z.X.Zhou, Z.Q.Chen, C.G.Wang

Possible coexistence of magnetic and antimagnetic rotations in 61Ni

NUCLEAR REACTIONS 54Cr(11B, 4n)61Ni, E=54 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 61Ni; deduced levels, J, π, asymmetric angular distributions from oriented states (ADO), dipole and quadrupole bands structures, configurations, high-spin states. Study provides evidence for possible coexistence of magnetic and antimagnetic rotations in the region around A=60. Comparison with calculations using the microscopic tilted axis cranking covariant density functional theory (TAC-CDFT). Detector array consisted of 6 HPGe with BGO anti-Compton suppressors, 1 clover HPGe detector 2 planar HPGe detectors at HI-13 Tandem Accelerator of the China Institute of Atomic Energy (CIAE).

doi: 10.1103/PhysRevC.107.014307
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2023LU04      Phys.Rev. C 108, 014302 (2023)

H.Y.Lu, Z.Liu, Z.H.Li, X.Wang, J.Li, H.Hua, H.Huang, W.Q.Zhang, Q.B.Zeng, X.H.Yu, T.H.Huang, M.D.Sun, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, F.S.Zhang

Reinvestigation of 222U in high-precision digital α-decay spectroscopy: Solution to the reduced decay-width anomaly

RADIOACTIVITY 222U(α) [from 186W(40Ar, 4n), E=80 MeV, followed by separation of fragments using SHANS separator at HRIFL-Lanzhou]; 218Th, 214Ra(α)[from 222U α decay chain]; measured Eα, Iα, evaporation residues (ER)-α correlations, T1/2 using DSSD detectors; deduced reduced α-decay width, and analyzed using NpNn scheme. 218Ac, 219Th, 220Pa(α); measured Eα, and T1/2. Systematics of reduced α-decay widths for g.s. to g.s. α transitions in even-even Z=84-92, N≥126 isotopes as function of NpNn. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.108.014302
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2023MA32      Phys.Rev. C 108, 014309 (2023)

Madhu, A.Y.Deo, K.Yadav, D.Sahoo, Y.Y.Wang, Y.K.Wang, J.Meng, S.Suman, S.K.Tandel, A.Sharma, I.Ahmed, K.Katre, K.Rojeeta Devi, S.Dutt, S.Kumar, Yashraj, S.Muralithar, R.P.Singh

Coexisting single-particle excitations and octupole correlations in the transitional nucleus 217Ra

NUCLEAR STRUCTURE 208Pb(12C, 3n)217Ra, E=68, 72, 80 MeV; measured Eγ, Iγ, X-rays, γγ-coin, γγ(θ). 217Ra; deduced levels, J, π δ, high-spin states, ratios of directional correlations of oriented states (DCO ratios), transition polarization asymmetry, linear polarization, cumulative T1/2 of the 2301- and 2394-keV states, configurations, bands structure and energy splittings. Comparison to theoretical calculations using reflection-asymmetric triaxial particle rotor model (RAT-PRM). From features of the simplex bands suggested that 217Ra exhibits an intermediate behavior between the extremes of spherical and octupole-deformed nuclei. Systematics of energy splittings and B(E1)/B(E2) ratios for 216Fr, 217Ra, 218Ac, 219Th, 232Th. Indian National Gamma Array (INGA) comprising of 13 Compton suppressed clover detectors and one low-energy photon spectrometer (LEPS) at 15UD Pelletron accelerator of Inter-University Accelerator Centre (New Delhi).

doi: 10.1103/PhysRevC.108.014309
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2023MA48      Phys.Rev. C 108, 044606 (2023)

C.-W.Ma, X.-X.Chen, X.-B.Wei, D.Peng, H.-L.Wei, Y.-T.Wang, J.Pu, K.-X.Cheng, Y.-F.Guo, C.-Y.Qiao

Systematic behavior of fragments in Bayesian neural network models for projectile fragmentation reactions

doi: 10.1103/PhysRevC.108.044606
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2023MU07      Phys.Rev. C 107, 035804 (2023)

M.Muller, F.Heim, Y.Wang, S.Wilden, A.Zilges

Determination of 170, 172Yb(α, n)173, 175Hf reaction cross sections in a stacked-target experiment

NUCLEAR REACTIONS 170Yb(α, n), E=14.5 MeV; 172Yb(α, n), E=17 MeV; measured Eγ, Iγ; deduced σ(E). Activation technique. Comparison with TALYS-1.95 calculations with various α optical model potentials (OMP) and other experimental data. Investigated the evolution of the α-OMP with the neutron-to-proton ratio. Cologne Clover Counting setup consisting of two clover-type high-purity germanium detectors in a face-to-face geometry. Irradiation of stacked targets at10 MV FN tandem accelerator (University of Cologne).

doi: 10.1103/PhysRevC.107.035804
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2023PE11      Phys.Rev. C 108, 014317 (2023)

C.M.Petrache, J.Uusitalo, A.D.Briscoe, C.M.Sullivan, D.T.Joss, H.Tann, O.Aktas, B.Alayed, M.A.M.Al-Aqeel, A.Astier, H.Badran, B.Cederwall, C.Delafosse, A.Ertoprak, Z.Favier, U.Forsberg, W.Gins, T.Grahn, P.T.Greenlees, X.T.He, J.Heery, J.Hilton, S.Kalantan, R.Li, P.M.Jodidar, R.Julin, S.Juutinen, M.Leino, M.C.Lewis, J.G.Li, Z.P.Li, M.Luoma, B.F.Lv, A.McCarter, S.Nathaniel, J.Ojala, R.D.Page, J.Pakarinen, P.Papadakis, E.Parr, J.Partanen, E.S.Paul, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, J.Smallcombe, J.Sorri, S.Szwec, L.J.Wang, Y.Wang, L.Waring, F.R.Xu, J.Zhang, Z.H.Zhang, K.K.Zheng, G.Zimba

High-K three-quasiparticle isomers in the proton-rich nucleus 129Nd

doi: 10.1103/PhysRevC.108.014317
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2023SH06      Astrophys.J. 945, 41 (2023)

Y.Shen, B.Guo, R.J.deBoer, E.Li, Z.Li, Y.Li, X.Tang, D.Pang, S.Adhikari, C.Basu, J.Su, S.Yan, Q.Fan, J.Liu, C.Chen, Z.Han, X.Li, G.Lian, T.Ma, W.Nan, W.Nan, Y.Wang, S.Zeng, H.Zhang, W.Liu

New Determination of the 12C(α, γ)16O Reaction Rate and Its Impact on the Black-hole Mass Gap

NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; measured reaction products. 16O; deduced σ(θ), the asymptotic normalization coefficient (ANC) for the 16O ground state (GS), astrophysical S-factor and the stellar rate. The HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE) in Beijing, China.

doi: 10.3847/1538-4357/acb7de
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2023WA05      Phys.Rev.Lett. 130, 092701 (2023)

L.H.Wang, J.Su, Y.P.Shen, J.J.He, M.Lugaro, B.Szanyi, A.I.Karakas, L.Y.Zhang, X.Y.Li, B.Guo, G.Lian, Z.H.Li, Y.B.Wang, L.H.Chen, B.Q.Cui, X.D.Tang, B.S.Gao, Q.Wu, L.T.Sun, S.Wang, Y.D.Sheng, Y.J.Chen, H.Zhang, Z.M.Li, L.Y.Song, X.Z.Jiang, W.Nan, W.K.Nan, L.Zhang, F.Q.Cao, T.Y.Jiao, L.H.Ru, J.P.Cheng, M.Wiescher, W.P.Liu

Measurement of the 18O(α, γ)22Ne Reaction Rate at JUNA and Its Impact on Probing the Origin of SiC Grains

NUCLEAR REACTIONS 18O(α, γ), E=470-787 keV; measured reaction products, Eγ, Iγ; deduced thick target yields, resonance energies and resonance strengths, total reaction rates. Comparison with available data. The Jinping Underground Nuclear Astrophysics experimental facility (JUNA).

doi: 10.1103/PhysRevLett.130.092701
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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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2023WA11      Appl.Radiat.Isot. 198, 110852 (2023)

Q.Wang, Y.Wang, Z.li, S.Niu, S.Si, Q.Wang, S.Zhang

Fission cross-section measurement for 135mXe and 135gXe in 238U reaction induced by 14MeV D-T neutrons

NUCLEAR REACTIONS 238U(n, X)135Xe/135I, E=14.1, 14.5, 14.7 MeV; measured reaction products, Eγ, Iγ; deduced independent fission σ. Comparison with available data. The K-400 high-current neutron generator platform of the Second Institute of the Chinese Academy of Engineering Physics.

doi: 10.1016/j.apradiso.2023.110852
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2023WA13      Phys.Rev. C 107, 064305 (2023)

H.K.Wang, Y.J.Li, Y.B.Wang, A.Jalili, Y.B.Qian

Spectroscopic factors and level spectra in neutron-rich Sn isotopes

NUCLEAR STRUCTURE 131,133,134,135,136,137Sn; calculated levels, J, π, spectroscopic factors, configurations. Shell-model calculations with Hamiltonian including core excitations and the intruder orbit i13/2 using codes NUSHELLX and KSHELL. Comparison to available experimental data.

doi: 10.1103/PhysRevC.107.064305
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2023WA16      Chin.Phys.C 47, 074103 (2023)

H.-K.Wang, A.Jalili, G.-X.Li, Y.-B.Wang

Monopole effects and high-spin levels in neutron-rich 132Te

NUCLEAR STRUCTURE 132Te; calculated energy levels, J, π using shell model calculations using the extended pairing plus multipole-multipole force model; deduced significant difference between experiment and theory in the high-spin level 17+, the monopole corrections and quadruple-quadruple force.

doi: 10.1088/1674-1137/accdc6
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2023WA23      Chin.Phys.C 47, 084101 (2023)

Y.-Z.Wang, F.-Z.Xing, J.-P.Cui, Y.-H.Gao, J.-Z.Gu

Roles of tensor force and pairing correlation in two-proton radioactivity of halo nuclei

RADIOACTIVITY 18Mg, 20Si(2p); calculated T1/2 using different Skyrme interactions, Q-values; deduced small effect of tensor force. The framework of spherical Skyrme-Hartree-Fock-Bogoliubov theory.

doi: 10.1088/1674-1137/acd680
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2023WA28      Appl.Radiat.Isot. 201, 110996 (2023)

Y.Wang, T.Sounalet, A.Guertin, E.Nigron, N.Michel, F.Haddad

Study of terbium production from enriched Gd targets via the reaction 155Gd(d, 2n)155Tb

NUCLEAR REACTIONS 155Gd(d, 2n), E=8.1-29.7 MeV; measured reaction products, Eγ, Iγ; deduced thick target yields, σ. Comparison with TALYS calculations. GIP ARRONAX cyclotron facility.

doi: 10.1016/j.apradiso.2023.110996
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2023WA37      Int.J.Mod.Phys. E32, 2340010 (2023)

Y.Wang, Sh.Zhang

Rotational spectroscopies of reflection-asymmetric nuclei within particle rotor model

NUCLEAR STRUCTURE 223Th, 78Br, 124Cs; analyzed available data; deduced the status of observations of the alternated parity bands in even-even nuclei and the parity doublet bands in odd-A and odd-odd nuclei for the A ∼ 220 mass region.

doi: 10.1142/S0218301323400104
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2023WU11      Nucl.Instrum.Methods Phys.Res. A1057, 168779 (2023)

H.Wu, X.Guan, G.Wu, H.Wang, Y.Wang, J.Du, L.Zhang, L.Gu

Experimental validation of a BNCT epithermal neutron flux detector using 55Mn(n, γ)56Mn reaction at an accelerator-based BNCT facility

NUCLEAR REACTIONS 55Mn(n, γ), E epithermal; measured reaction products, Eγ, Iγ; deduced induced radioactivity in the activated MnNi foil, epithermal neutron flux. GMX60 detector, the AB-BNCT facility developed by Lanzhou University by irradiating the detector in the neutron field.

doi: 10.1016/j.nima.2023.168779
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2023XU12      Int.J.Mod.Phys. E32, 2340007 (2023)

F.Xu, Y.Wang

Shell-model-like approach based on covariant density functional theory in 3D lattice space: Evolution of octupole shape in rotating 224Th

NUCLEAR STRUCTURE 224Th; calculated spin as functions of the rotational frequency by the cranking CDFT-SLAP in 3D lattice space with and without pairing correlations, quadrupole deformation parameters. Comparison with experimental data.

doi: 10.1142/S0218301323400074
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2023ZH26      Phys.Rev. C 107, 065801 (2023)

H.Zhang, J.Su, Z.H.Li, Y.J.Li, E.T.Li, C.Chen, J.J.He, Y.P.Shen, G.Lian, B.Guo, X.Y.Li, L.Y.Zhang, Y.D.Sheng, Y.J.Chen, L.H.Wang, L.Zhang, F.Q.Cao, W.Nan, W.K.Nan, G.X.Li, N.Song, B.Q.Cui, L.H.Chen, R.G.Ma, Z.C.Zhang, T.Y.Jiao, B.S.Gao, X.D.Tang, Q.Wu, J.Q.Li, L.T.Sun, S.Wang, S.Q.Yan, J.H.Liao, Y.B.Wang, S.Zeng, D.Nan, Q.W.Fan, W.P.Liu

Updated reaction rate of 25Mg(p, γ)26Al and its astrophysical implication

NUCLEAR REACTIONS 25Mg(p, γ), E=117-350 keV; measured Eγ, Iγ, sum of γ energies; deduced γ-ray branching ratios, resonances, resonance strengths, astrophysical reaction rate (T=0.01-2.0 GK), contribution of individual resonances to the reaction rate, ground-state and isomeric state contribution. Comaprison to other experimental data and NACRE compilation. Evaluated the impact of the obtained data on the 26Al yield in stellar environment (code MESA). BGO detector array in nearby 4π geometry composed of 8 identical segments at high-current 400 kV JUNA accelerator (China JinPing underground Laboratory).

doi: 10.1103/PhysRevC.107.065801
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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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2023ZO02      Astrophys.J.Suppl.Ser. 268, 56 (2023)

Y.P.Zou, J.S.Zhang, C.Henkel, D.Romano, Y.H.Zheng, Y.T.Yen, J.L.Chen, Y.X.Wang, Y.Zhao

A Systematic Observational Study on Galactic Interstellar Ratio 18O/17O. II. C18O and C17O J = 2-1 Data Analysis

doi: 10.3847/1538-4365/acee6b
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2022CH16      Chin.Phys.C 46, 024105 (2022)

K.-X.Cheng, C.Xu, C.n-W.Ma, J.Pu, Y.-T.Wang

Pauli blocking potential applied to heavy-ion fusion reactions

NUCLEAR REACTIONS 208Pb(16O, X), 58Ni(58Ni, X), E not given; calculated fusion hindrance phenomena at deep sub-barrier energies using the Pauli blocking potential between two colliding nuclei in the density overlapping region is applied to describe the heavy nuclei fusion process.

doi: 10.1088/1674-1137/ac3749
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2022CH21      Phys.Rev. C 105, 045806 (2022)

P.-C.Chu, Y.-N.Wang, X.-H.Li, H.Liu, J.-W.Zhang

Strange quark matter at finite temperature under magnetic fields with a quasiparticle model

doi: 10.1103/PhysRevC.105.045806
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2022CU01      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY 255,256,258,259,261,263Rf, 256,257,258,259Db, 270Db, 259,260,261Sg, 263Sg, 267,269,271Sg, 263Sg, 267,269,271Sg, 260,261Bh, 265,266,267Bh, 270,272,274Bh, 264,265,266Hs, 268,269,270Hs, 273,275Hs, 270Mt, 274,275,276Mt, 278Mt, 267Ds, 269,270,271Ds, 273Ds, 277,279,281Ds, 272Rg, 278,279,280,281,282Rg, 277Cn, 281,283Cn, 284,285Cn, 278Nh, 282,283,284,285,286Nh, 285,286,287,288,289Fl, 287Mc, 289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og(α); calculated T1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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2022CU02      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY 255,256,258,259,261,263Rf, 256,257,258,259,270Db, 259,260,261,263,267,269,271Sg, 260,261,265,266,267,270,272,274Bh, 264,265,266,268,269,270,273,275Hs, 270,274,275,276,278Mt, 267,269,270,271,273,277,279,281Ds, 272,278,279,280,281,282Rg, 277,281,283,284,285Cn, 278,282,284,285,286Nh, 285,286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 278,282,286,290,294,298,302,306Og, 281,285,289,293,297,301,305,309119, 286,290,294,298,302,306,310,289,293,297,301,305,309120(α); calculated T1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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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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2022KA31      Phys.Rev. C 106, 034323 (2022)

K.Katre, P.V.Madhusudhana Rao, R.Raut, A.Sharma, K.Suryanarayana, A.Tejaswi, M.Ratna Raju, D.Vijaya Lakshmi, T.Seshi Reddy, M.Kumar Raju, S.Jehangir, N.Rather, G.H.Bhat, N.Nazir, J.A.Sheikh, Y.P.Wang, J.T.Matta, A.D.Ayangeakaa, U.Garg, S.S.Ghugre, T.Trivedi, B.S.Naidu, R.Palit, S.Saha, S.Muralithar, R.P.Singh

Chiral-like doublet band structure and octupole correlations in 104Ag

NUCLEAR REACTIONS 76Ge(32S, 3np)104Ag, E=110 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), level T1/2 by DSAM using INGA array of 18 Compton suppressed clover detectors at the 14-UD BARC-TIFR Pelletron Facility. 104Ag; deduced high-spin levels, J, π, multipolarities, bands, B(M1), B(E2), B(E1), B(M1)/B(E1), B(M1)/B(E2), spherical configurations, moment of inertia plots, alignments; calculated potential energy surface in the (β-γ) deformation plane, octupole correlations, enhanced E1 transitions, chiral-like doublet band. Comparison with theoretical calculations using triaxial projected shell model (TPSM) and covariant density functional theory (CDFT).

doi: 10.1103/PhysRevC.106.034323
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2022LI05      Chin.Phys.C 46, 014104 (2022)

X.Li, Y.Wang, X.Guo, M.Chen, J.Liu, C.Xu

Comparative studies on nuclear elastic magnetic form factors between the relativistic and non-relativistic mean-field approaches

NUCLEAR STRUCTURE 11B, 17O, 27Al, 41Ca, 57Ti, 59Co, 115In, 132Sn; calculated magnetic form factors in the relativistic framework, deformation corrections, RMS charge radii, valence nucleon RMS radii, binding energies, density distributions.

doi: 10.1088/1674-1137/ac2f94
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2022LI25      Nucl.Phys. A1022, 122444 (2022)

Y.J.Li, Z.H.Li, Y.B.Wang, Y.P.Shen

The controversy 3/2+ state in 7Be and its effect on the 3He(α, γ)7Be reaction

NUCLEAR REACTIONS 3He(α, γ), E(cm)<5 MeV; analyzed available data;deduced S-factors, R-matrix fitting parameters, J, π, resonances, astrophysical reaction rates.

doi: 10.1016/j.nuclphysa.2022.122444
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2022LI28      Few-Body Systems 63, 43 (2022)

W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho

Progress of Underground Nuclear Astrophysics Experiment JUNA in China

NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.

doi: 10.1007/s00601-022-01735-3
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2022LI47      Phys.Rev. C 106, 025807 (2022)

X.Y.Li, B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, J.J.He, S.Q.Yan, Q.W.Fan, J.C.Liu, L.Gan, Z.Y.Han, E.T.Li, G.Lian, Y.P.Shen, Y.B.Wang, S.Zeng, W.P.Liu

Astrophysical 15N(n, γ)16N reaction rate from precision measurement of the 15N(d, p)16N angular distributions

NUCLEAR REACTIONS 15N(d, p), (d, d), E=15 MeV; measured particle spectra, σ(θ) using Q3D magnetic spectrograph at CIAE's HI-13 tandem accelerator facility. 16N; deduced levels, J, π, configurations, spectroscopic factors for ground and first three excited states. DWBA and ADWA analysis. 15N(n, γ), T=0.01-10 GK; deduced astrophysical reaction rates; calculated σ(E). Comparison with previous experimental results, and with OXBASH shell-model predictions.

doi: 10.1103/PhysRevC.106.025807
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2022LI59      Phys.Rev. C 106, 054605 (2022)

J.Liu, Y.Wang, Y.Gao, P.Danielewicz, C.Xu, Z.Ren

Exploring the sensitivity of charge-exchange (p, n) reactions to the neutron density distribution

NUCLEAR REACTIONS 48Ca(p, p), 48Ca, 208Pb(p, n), E=35, 45 MeV;208Pb(n, n), E=30.4, 40 MeV; calculated σ(θ). Distorted-wave Born approximation (DWBA) method with complex folding and the hybrid folding models generated potentials. Calibration of the calculated potentials to PREX-II data. Comparison to experimental data.

NUCLEAR STRUCTURE 48Ca, 208Pb; calculated binding energies per nucleon, charge rms radii, neutron skin thickness. 208Pb; calculated ground-state neutron and proton densities. Calculations within Skyrme-Hartree-Fock (SHF) and the relativistic mean-field (RMF) frameworks. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.054605
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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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2022LU01      Phys.Rev. C 105, 024305 (2022)

D.W.Luo, C.Xu, Y.K.Wang, Z.H.Li, R.A.Bark, S.Q.Zhang, H.Hua, S.Y.Wang, J.Peng, X.Q.Li, H.Y.Wu, X.Wang, C.G.Wu, Q.T.Li, J.Lin, Y.Jin, W.Z.Xu, L.Mu, J.Meng, F.R.Xu, Y.L.Ye, D.X.Jiang, P.Jones, E.A.Lawrie, P.Papka, M.F.Nkalanga, T.D.Bucher, M.V.Chisapi, L.Msebi, S.Jongile, S.Ntshangase, B.R.Zikhali, S.H.Mthembu, T.Seakamela, M.A.Sithole, O.Shirihda, A.A.Aava, L.Mdletshe, K.L.Malatji, S.Mhlongo, L.Makhathini

Collective structures in 62Cu

NUCLEAR REACTIONS 54Cr(12C, 3np), E=67 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 62Cu; deduced levels, J, π, high-spin levels, B(M1)/B(E2), configurations, γγ(linear polarization). Comparison with calculations using the self-consistent tilted axis cranking covariant density functional theory (TAC-C DFT). Comparison with level structures in 60,64Ca. AFRODITE array at the iThemba LABS accelerator facility.

doi: 10.1103/PhysRevC.105.024305
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2022MA39      Chin.Phys.C 46, 074104 (2022)

C.-W.Ma, X.-B.Wei, X.-X.Chen, D.Peng, Y.-T.Wang, J.Pu, K.-X.Cheng, Y.-F.Guo, H.-L.Wei

Precise machine learning models for fragment production in projectile fragmentation reactions using Bayesian neural networks

doi: 10.1088/1674-1137/ac5efb
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2022MA45      Phys.Rev. C 106, 064316 (2022)

L.Ma, H.B.Yang, Z.Y.Zhang, J.C.Pei, M.H.Huang, M.M.Zhang, C.Y.Qiao, X.J.Bao, Y.L.Tian, C.L.Yang, Y.S.Wang, Z.Zhao, X.Y.Huang, S.Y.Xu, W.X.Huang, Z.Liu, X.H.Zhou, Z.G.Gan

Attempts to produce new americium isotopes near N=126

NUCLEAR REACTIONS 191,193Ir(40Ar, xn)231Am*/233Am*, E=190-204 MeV; measured reaction products, Eα, (recoils)α-α-α correlated events, using SHANS gas-filled recoil separator, 16 position-sensitive Si-strip detectors (PSSDs) for evaporation residues, and eight side silicon detectors (SSDs) for α particles at the HRIFL-Lanzhou facility. 226,227,228Am; no evidence found for the detection of these nuclides, with upper limits of cross sections determined for the production of the compound nuclei of 231Am and 233Am; discussed nonobservation of new americium isotopes in terms of reduced survival probabilities of compound nuclei 231Am and 233Am due to their low fission barriers at high excitations.

NUCLEAR STRUCTURE 226,227,228,229Am; calculated excitation functions for the production of these nuclides in 191,193Ir(40Ar, xn) using the statistical model code HIVAP. 230,231,232,233,234,235,236Am; evaluated shell correction energies and fission barriers from FRDM2012, KTUY2005, and WS2010. 226U, 227Np, 231,233Am; calculated fission barrier heights as functions of excitation energy and quadrupole deformation parameter β2 using microscopic finite-temperature Skyrme Hartree-Fock+BCS theory.

doi: 10.1103/PhysRevC.106.034316
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2022PE09      J.Phys.(London) G49, 085102 (2022)

D.Peng, H.-L.Wei, X.-X.Chen, X.-B.Wei, Y.-T.Wang, J.Pu, K.-X.Cheng, C.-W.Ma

Bayesian evaluation of residual production cross sections in proton-induced nuclear spallation reactions

NUCLEAR REACTIONS 1H(36Ar, X), (40Ar, X), (40Ca, X), (56Fe, X), (93Nb, X), (93Zr, X), (107Pd, X), (90Sr, X), (136Xe, X), (137Cs, X), (138Ba, X), (197Au, X), E<2.6 GeV/nucleon; analyzed available data; deduced accurate and complete energy-dependent residual σ using a simplified EPAX formula (sEPAX), the Bayesian neural network (BNN) technique.

doi: 10.1088/1361-6471/ac7069
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2022PO02      Phys.Rev. C 105, L041301 (2022)

W.S.Porter, B.Ashrafkhani, J.Bergmann, C.Brown, T.Brunner, J.D.Cardona, D.Curien, I.Dedes, T.Dickel, J.Dudek, E.Dunling, G.Gwinner, Z.Hockenbery, J.D.Holt, C.Hornung, C.Izzo, A.Jacobs, A.Javaji, B.Kootte, G.Kripko-Koncz, E.M.Lykiardopoulou, T.Miyagi, I.Mukul, T.Murbock, W.R.Plass, M.P.Reiter, J.Ringuette, C.Scheidenberger, R.Silwal, C.Walls, H.L.Wang, Y.Wang, J.Yang, J.Dilling, A.A.Kwiatkowski

Mapping the N=40 island of inversion: Precision mass measurements of neutron-rich Fe isotopes

ATOMIC MASSES 63,64,65,65m,66,67,68,69,69m,70Fe; measured time-of-flight; deduced mass excess, S(2n), pairing gap. Systematics of S(2n) values for Z=24–28 isotope chains. Compared to mean-field calculations employing recent Woods-Saxon Hamiltonian and results from the multishell valence-space in-medium similarity renormalization group (VS-IMSRG). Comparison to recommended values from AME2020. TITAN (TRIUMF’s Ion Trap for Atomic and Nuclear science) Multiple-Reflection Time-of- Flight Mass Spectrometer.

doi: 10.1103/PhysRevC.105.L041301
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2022SU23      Phys.Rev. C 106, 034614 (2022)

Y.Z.Sun, S.T.Wang, Y.P.Xu, D.Y.Pang, J.G.Li, C.X.Yuan, L.F.Wan, Y.Qiao, Y.Q.Wang, X.Y.Chen

Spectroscopic strength reduction of intermediate-energy single-proton removal from oxygen isotopes

NUCLEAR STRUCTURE C(13O, p), E=397 MeV/nucleon;C(14O, p), E=305, 349 MeV/nucleon;C(15O, p), E=308 MeV/nucleon;C(16O, p), E=450 MeV/nucleon;C(17O, p), E=629 MeV/nucleon;C(18O, p), E=573 MeV/nucleon;C(19O, p), E=635 MeV/nucleon;C(20O, p), E=415 MeV/nucleon;C(22O, p), E=414 MeV/nucleon; calculated inclusive single-proton removal σ, shell-model spectroscopic factors, reduction factors of the spectroscopic factors with the experimental data. Glauber reaction model calculations performed with MOMDIS code. Comparison to experimental data obtained at GSI and ETF(Lanzhou, China).

doi: 10.1103/PhysRevC.106.034614
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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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2022WA12      Phys.Rev. C 105, 044316 (2022)

Y.Y.Wang, Q.B.Chen, S.Q.Zhang

Interpretation of enhanced electric dipole transitions in 73Br by the reflection-asymmetric triaxial particle rotor model

NUCLEAR STRUCTURE 73Br; calculated potential energy surface, levels, J, π, B(E2), B(E1), positive and negative parity bands structures, proton single-particle levels. Investigated octupole correlations. Reflection-asymmetric triaxial version of particle rotor model (RAT-PRM). Comparison to experimental data.

doi: 10.1103/PhysRevC.105.044316
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2022WA13      Phys.Lett. B 830, 137154 (2022)

Y.F.Wang, X.Y.Zhang, Z.M.Niu, Z.P.Li

Study of nuclear low-lying excitation spectra with the Bayesian neural network approach

NUCLEAR STRUCTURE 20,22,24,26,28,30,32,34,36,38,40Mg, 36,38,40,42,44,46,48,50,52,54Ca, 72,74,76,78,80,82,84,86,88,90,92,94,96,98Kr, 130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162Sm, 182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216Pb; analyzed available data; deduced energies, J, π of the low-lying spectra in Bayesian neural network (BNN) approach.

doi: 10.1016/j.physletb.2022.137154
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2022WA15      Phys.Rev. C 105, 054311 (2022)

Y.K.Wang, P.W.Zhao, J.Meng

Configuration-interaction projected density functional theory: Effects of four-quasiparticle configurations and time-odd interactions

NUCLEAR STRUCTURE 60Fe; calculated levels, J, π, B(E2), kinematic moment of inertia, yrast band structure, neutron and proton quasiparticle energy levels. Four-quasiparticle configurations and time-odd interactions investigated in the framework of configuration-interaction projected density functional theory (CI-PDFT). Comparison to experimental data.

doi: 10.1103/PhysRevC.105.054311
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2022WA18      Phys.Lett. B 831, 137198 (2022)

Y.-Z.Wang, S.Zhang, Y.-G.Ma

System dependence of away-side broadening and α-clustering light nuclei structure effect in dihadron azimuthal correlations

NUCLEAR REACTIONS 16O(16O, X), 10B(10B, X), 40Ca(40Ca, X), 96Zr(96Zr, X), 197Au(197Au, X), E=6.73 TeV; analyzed available data; deduced dihadron azimuthal correlation, the momentum dependence of away-side broadening parameters.

doi: 10.1016/j.physletb.2022.137198
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2022WA30      Phys.Lett. B 833, 137337 (2022)

H.-K.Wang, Z.-H.Li, Y.-B.Wang, B.Jiang

High-spin levels, β- decay and monopole effects in A = 128 hole nuclei near 132Sn

RADIOACTIVITY 128Pd, 128Ag, 128Cd, 128In(β-); calculated log ft, high-spin energy levels, J, π with large-scale shell-model calculations with the extended pairing plus multipole-multipole force model 128Sn; deduced monopole effects, impact on T1/2 by monopole corrections acting on the configuration of final states, a spin-trap isomer feeding. Comparison with available data.

doi: 10.1016/j.physletb.2022.137337
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2022WA37      Phys.Rev. C 106, 044610 (2022)

Y.Wang, for the A1 and MAGIX Collaborations

Low-Q2 elastic electron-proton scattering using a gas jet target

NUCLEAR REACTIONS 1H(e, e'), E=315 MeV; measured Eβ, Iβ, angular distributions; deduced proton electric form factor. Comparison to other experimental results. Cryogenic supersonic gas jet target in the A1 three-spectrometer facility at the Mainz Microtron.

doi: 10.1103/PhysRevC.106.044610
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2022XI08      Nucl.Phys. A1028, 122528 (2022)

F.Xing, H.Qi, J.Cui, Y.Gao, Y.Wang, J.Gu, G.Yong

An improved Gamow-like formula for α-decay half-lives

RADIOACTIVITY 214,215,216,217,218U, 219,220,221,222,223,224Np, 221,222,223,224,225,226,227Pu, 224,225,226,227,228Am, 231,232Cm, 233,234,235,236,237,238,239,240,241,242Bk, 234,235,236Cf, 237,238,239Es, 239,240,241,242,243,244Fm, 241,242,243Md, 246,247,248,249,250No, 249,250,251Lr, 251,252,253,254Rf, 253,254,255Db, 256,257,258Sg, 258,259,260,261,262,263Bh, 261,262Hs, 263,264,265Mt, 261,262,263,264,265,266Ds, 266,267,268,269,270,271,272,273Rg, 270,271,272,273,274,275,276Cn, 272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290Nh, 278,279,280,281,282,283,284,285,286,287,288,289,290,291Fl, 281,282,283,284,285,286,287,288,289,290,291,292Mc, 283,284,285,286,287,288,289Lv, 285,286,287,288,289,290,291,292Ts, 288,289,290,291,292,293Og, 295Og, 290,291,292,293,294,295,296119, 291,292,293,294,295,296,297,298,299,300120, 287,288,289,290,291Og, 283,284Lv, 279,280,281Fl, 275,276Cn, 271,272,273Ds, 294120, 268,269Hs, 264,265Sg, 281Fl(α); calculated T1/2; deduced an improved Gamow-like (IMGL) formula parameters. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122528
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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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2022ZH07      Phys.Rev. C 105, 024328 (2022)

H.B.Zhou, Z.Y.Li, Z.G.Gan, Z.Y.Zhang, H.Yao, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, X.H.Zhou, J.L.Tian

Modeling the fusion process with a modified Woods-Saxon potential in 40Ar-induced fusion reactions

NUCLEAR REACTIONS 176Hf(40Ar, 2np)212Ac, (40Ar, 3np)213Ac, (40Ar, 2nα)209Ra, (40Ar, 3nα)210Ra, E=183, 190 MeV; measured reaction products, Eα, Iα; deduced σ(E), theory evaluation factors. Observed α peaks from decays of 211,212,213,213Ra, 214,215Ac. Comparison to density-constrained time-dependent Hartree-Fock theory calculations. Beam from Sector-Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL). 165Ho(40Ar, 4n), E(cm)=130-160 MeV; 169Tm(40Ar, 4n), E(cm)=130-170 MeV; 174Yb(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 175Lu(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 176Hf(40Ar, 4n), (40Ar, 5n), E(cm)=135-165 MeV; 181Ta(40Ar, 4n), E(cm)=130-160 MeV; analyzed σ(E) from 1984VE09.

doi: 10.1103/PhysRevC.105.024328
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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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2022ZH69      Eur.Phys.J. A 58, 200 (2022)

T.G.Zhang, L.R.Dai, X.J.Cai, L.N.Chen, Y.H.Wang

A study of hidden-color channel on the strangeness-1 dibaryon

doi: 10.1140/epja/s10050-022-00857-w
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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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2021CH03      Phys.Rev. C 103, 014613 (2021)

K.Cheng, C.Xu, C.Ma, J.Pu, Y.Wang

Density variation effects in α + 208Pb and 16O + 208Pb fusion reactions

NUCLEAR REACTIONS 208Pb(α, X), E=15.6, 23.5 MeV; calculated width parameter and corresponding central density of α particles versus distance between the center of mass of two nuclei, potentials of M3Y + Pauli and M3Y + Pauli + DVE. 208Pb(16O, X), E=75.65, 109.52 and 65.85 MeV; calculated density distributions of 208Pb, 16O, and α cluster at E(16O)=75.65 MeV, total potentials M3Y + Pauli with and without DVE for E(16O)=109.52 and 65.85 MeV; deduced influence of density variation of α particles and α-cluster nucleus 16O on cross sections and potentials. 208Pb(16O, X), E=64-88 MeV; calculated fusion σ(E) using coupled-channels (CC) with M3Y + Pauli and M3Y + Pauli + DVE potentials. Comparison with experimental data.

doi: 10.1103/PhysRevC.103.014613
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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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2021FA05      Appl.Radiat.Isot. 172, 109669 (2021)

Y.Fan, Q.Li, Y.Wang, Y.Zhao, X.Zhang, H.Jia, Y.Chang, S.Liu, X.Ai, S.Wang

Assessment of a compton-suppressed spectrometer for measurement of radioactive xenon isotopes

RADIOACTIVITY 133Xe(β-), 127Xe(EC); measured decay products, Eγ, Iγ; deduced γ-ray energies and relative intensities.

doi: 10.1016/j.apradiso.2021.109669
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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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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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2021LI50      Phys.Rev. C 104, 034608 (2021)

F.Li, Y.Wang, Z.Gao, P.Li, H.Lu, Q.Li, C.Y.Tsang, M.B.Tsang

Application of machine learning in the determination of impact parameter in the 132Sn + 124Sn system

NUCLEAR REACTIONS 124Sn(132Sn, X), E=270 MeV/nucleon; analyzed experimental data for charged-particle spectra or other simulated events from RIBF-RIKEN facility to extract impact parameters using the ultrarelativistic quantum molecular dynamics (UrQMD) model, and three machine learning algorithms of artificial neural network (ANN), convolutional neural network (CNN), and light gradient boosting machine (LightGBM).

doi: 10.1103/PhysRevC.104.034608
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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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2021MA66      Phys.Rev. C 104, 044310 (2021)

L.Ma, Z.Y.Zhang, H.B.Yang, M.H.Huang, M.M.Zhang, Y.L.Tian, C.L.Yang, Y.S.Wang, Z.Zhao, W.X.Huang, Z.Liu, X.H.Zhou, Z.G.Gan

α-decay properties of 220Pa

RADIOACTIVITY 220,220mPa(α)[from 187Re(40Ar, 3nα), E=198.7 MeV]; 216Ac(α)[from 220Pa(α)]; measured Eα, Iα, half-lives of decays of 220,220mPa using position-sensitive 16-strip detectors (PSSDs) at the Sector-Focusing Cyclotron and SHANS recoil separator of HIRF-Lanzhou. 220Pa, 216Ac; deduced levels, J, π, Q(α), reduced α-width, new isomer in 220Pa. Comparison with previous experimental data. Systematics of reduced α widths of N=129, Z=84-93 isotones.

doi: 10.1103/PhysRevC.104.044310
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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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2021RA31      Phys.Rev. C 104, 064316 (2021)

S.Rajbanshi, R.Palit, R.Raut, Y.Y.Wang, Z.X.Ren, J.Meng, Q.B.Chen, S.Ali, H.Pai, F.S.Babra, R.Banik, S.Bhattacharya, S.Bhattacharyya, P.Dey, S.Malik, G.Mukherjee, Md.S.R.Laskar, S.Nandi, R.Santra, T.Trivedi, S.S.Ghugre, A.Goswami

Evidence of octupole correlation in 79Se

NUCLEAR REACTIONS 76Ge(9Be, 2nα)79Se, E≈31 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(θ)(ADO ratios), γγ(linear polarization), T1/2 of levels by DSAM using INGA array of 14 Compton-suppressed clover detectors at the TIFR Pelletron Linac Facility. 79Se; deduced high-spin levels, J, π, multipolarities, multipole mixing ratios, B(M1), B(E2), B(E1)/B(E2) ratios, intrinsic dipole moments, octupole correlation; calculated potential energy surface in (β20, β30) plane based on the covariant density functional theory. Comparison of measured transition probabilities with reflection asymmetric triaxial particle rotor model (RAT-PRM) calculations.

doi: 10.1103/PhysRevC.104.064316
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2021SH23      Phys.Rev. C 103, L061301 (2021)

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

β-delayed two-proton decay of 27S at the proton-drip line

RADIOACTIVITY 27S(β+2p)[from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility, and implanted into three W1-type double-sided silicon strip detectors (DSSDs)]; measured reaction products, E(p), I(p), pp-coin, p(θ), half-life of 27S decay using Si detectors surrounded by HPGe detectors; deduced branching ratio of β+2p decay, identified as a two-proton transition, dominantly sequential, via the isobaric-analog state (IAS) in 27P to the ground state of 25Al.

doi: 10.1103/PhysRevC.103.L061301
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2021WA06      Phys.Rev. C 103, L011301 (2021)

Y.B.Wang, for the BRIF Collaboration

Direct observation of the exotic β - γ - α decay mode in the Tz = 1 nucleus 20Na

RADIOACTIVITY 20Na(EC), (β+), (β+α)[pure intense ISOL beam of 20Na from 24Mg(p, nα), E=100 MeV from Beijing HI-13 tandem accelerator]; measured decay products, Eβ+, Eγ, Iγ, Eα, Iα, γγ- and αγ-coin at the Beijing Radioactive Ion-beam facility. 20Ne; deduced levels, J, π, isospin, EC and β+ feedings, logft, B(F), B(GT). 16O; deduced levels, J, π, β+-delayed α sequences. Comparison with shell model calculation with USDB interaction.

doi: 10.1103/PhysRevC.103.L011301
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2021WA29      Chin.Phys.C 45, 044111 (2021)

Y.Wang, F.Xing, Y.Xiao, J.Gu

An improved semi-empirical relationship for cluster radioactivity

RADIOACTIVITY 212,214Po, 236,238Pu, 222,224,226Ra, 228,230Th, 230,232,234,236U, 242Cm, 213Po, 215At, 221Fr, 221,223Ra, 225Ac, 231Pa, 233,235U(α), 226Th(14C), (18O), 232Th, 230,236U(24Ne), 232Th, 236U(26Ne), 232,233,235U(28Mg), 237Np(30Mg), 240Pu, 241Am(34Si); calculated preformation factors P of the cluster radioactivity and α-decay, T1/2. Comparison with available data.

doi: 10.1088/1674-1137/abe112
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2021WA35      Phys.Rev. C 104, 014318 (2021)

Y.Y.Wang

Parity doublet bands in 223Th within reflection-asymmetric triaxial particle rotor model

NUCLEAR STRUCTURE 223Th; calculated level energies, staggering parameters, parity splitting, B(E1)/B(E2) and B(M1)/B(E2) ratios, main components of intrinsic wave functions for the positive- and negative-parity doublet structures using reflection-asymmetric triaxial particle rotor model (RAT-PRM). Comparison with experimental data.

doi: 10.1103/PhysRevC.104.014318
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2021WA36      Phys.Rev. C 104, 014320 (2021)

Y.K.Wang, P.W.Zhao, J.Meng

Nuclear matrix elements of neutrinoless double-β decay in the triaxial projected shell model

NUCLEAR STRUCTURE 76Ge, 76Se; 82Se, 82Kr; 100Mo, 100Ru; 130Te, 130Xe; 150Nd, 150Sm; calculated levels, J for the low-lying positive-parity states, B(E2) for the first 2+ states, occupancies of single-particle orbits for neutrons and protons using triaxial projected shell model, potential-energy curves of 0+ states as functions of the triaxial deformation parameters for 76Ge, 82Se, 100Mo, 130Te, 150Nd. Comparison with experimental data.

RADIOACTIVITY 76Ge, 82Se, 100Mo, 130Te, 150Nd(2β-); calculated nuclear matrix elements (NMEs) for 0νββ decay mode, NME contours as functions of triaxial deformation parameters using triaxial projected shell model (TPSM) and triaxial projected Hartree-Fock-Bogoliubov model (TPHFB). Comparison with calculations using relativistic and nonrelativistic density functional theory (DFT), interacting boson model (IBM), PHFB, quasiparticle random-phase approximation (QRPA), and shell-model (SM).

doi: 10.1103/PhysRevC.104.014320
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2021XI06      Chin.Phys.C 45, 124105 (2021)

F.Xing, J.Cui, Y.Wang, J.Gu

Two-proton radioactivity of ground and excited states within a unified fission model

RADIOACTIVITY 6Be, 12O, 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); 5Be, 6,7B, 8C, 10N, 11O, 13,14F, 15Ne, 17Na, 22Si, 24P, 26S, 28,29Cl, 29,30Ar, 31,32K, 33,34Ca, 45Sc, 35,37Sc, 37,38,39Ti, 39,40V, 41,42Cr, 43,44Mn, 47Co, 49Ni, 52Cu, 55Zn, 56,57,58Ga, 58,59Ge, 60,61,62As, 63,64Se, 65,66Br, 68Kr, 81Mo, 85Ru, 108Xe(2p); analyzed available data; calculated T1/2. Comparison with the AME2020 table, available data.

doi: 10.1088/1674-1137/ac2425
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2021YA29      Astrophys.J. 919, 84 (2021)

S.Q.Yan, X.Y.Li, K.Nishio, M.Lugaro, Z.H.Li, H.Makii, M.Pignatari, Y.B.Wang, R.Orlandi, K.Hirose

The 59Fe(n, γ)60Fe Cross Section from the Surrogate Ratio Method and Its Effect on the 60Fe Nucleosynthesis

NUCLEAR REACTIONS 56,58Fe(18O, 16O), E=103 MeV; measured reaction products, Eγ, Iγ; deduced σ, Maxwellian-averaged σ. Comparison with TALYS calculations.

doi: 10.3847/1538-4357/ac12ce
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2021YA31      Phys.Rev. C 104, 054312 (2021)

Y.L.Yang, Y.K.Wang, P.W.Zhao, Z.P.Li

Nuclear landscape in a mapped collective Hamiltonian from covariant density functional theory

NUCLEAR STRUCTURE Z=8-104 (even Z), N=6-258 (even N); calculated binding energies with and without dynamical correlation energies, Dynamical correlation energies, quadrupole deformations β, triaxial deformation γ, S(2n), S(2p), neutron and proton Fermi surfaces, charge radii, neutron, proton and matter root-mean-square radii for even-even nuclei. Relativistic Hartree-Bogoliubov theory with the PCPK1 energy density functional, and the beyond-mean-field dynamical correlation energies from microscopically mapped five-dimensional collective Hamiltonian (5DCH). 112Ru; calculated pairing energies and the zero-point energies in two calculations. The detailed results for a large number of nuclides are given in the Supplemental Material. Comparison of S(2n) and S(2p) with AME2016 values.

doi: 10.1103/PhysRevC.104.054312
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2021ZH22      Phys.Rev.Lett. 126, 152502 (2021)

Z.Y.Zhang, H.B.Yang, M.H.Huang, Z.G.Gan, C.X.Yuan, C.Qi, A.N.Andreyev, M.L.Liu, L.Ma, M.M.Zhang, Y.L.Tian, Y.S.Wang, J.G.Wang, C.L.Yang, G.S.Li, Y.H.Qiang, 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, Z.Z.Ren, S.G.Zhou

New α-Emitting Isotope 214U and Abnormal Enhancement of α-Particle Clustering in Lightest Uranium Isotopes

RADIOACTIVITY 214,216,218U(α) [from 180,182W(36Ar, 4n), 184W(40Ca, 2nα), E<200 MeV]; measured decay products, Eα, Iα; deduced α-decay Q-values and reduced widths, T1/2, abnormal enhancement by the strong monopole interaction between the valence protons and neutrons. Comparison withavailable data, calculations.

doi: 10.1103/PhysRevLett.126.152502
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2021ZH24      Phys.Rev. C 103, 044314 (2021)

H.B.Zhou, Z.G.Gan, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Li, C.X.Yuan, S.Huang, X.J.Sun, H.Y.Peng, L.Ou, X.H.Zhou

Lifetime measurement for the isomeric state in 213Th

NUCLEAR REACTIONS 176Hf(40Ar, xn)213Th/214Th/215Th, E=183, 190 MeV beam from Sector-Focusing Cyclotron of HIRFL-Lanzhou facility, followed by the separation of evaporation residues (ERs) by the SHANS separator and implanted in three position-sensitive silicon strip detectors (PSSDs); measured position, time, and energy of the ERs, Eα, Iα, Eγ, Iγ, (ER)α-, (ER)γ- and (ER)αγ-correlated events. Enriched target. 213,214,215Th; deduced levels, J, π, isomers, half-lives of the isomers in 213,214,215Th. Comparison with previous experimental results for isomer half-lives. Systematics of 13/2+ isomers in N=123 isotones 207Po, 209Rn, 211Ra and 213Th.

RADIOACTIVITY 209,210,211,213Ra, 212,213,215Ac, 211,212,213,214,215,216Th(α)[from 176,177,178,179,180Hf(40Ar, xnyp), E=183, 190 MeV, enriched 176Hf with small abundance of other Hf isotopes]; measured Eα, Iα, αγ-correlations.

doi: 10.1103/PhysRevC.103.044314
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2021ZH54      Phys.Lett. B 822, 136645 (2021)

K.K.Zheng, C.M.Petrache, Z.H.Zhang, P.W.Zhao, Y.K.Wang, A.Astier, B.F.Lv, P.T.Greenlees, T.Grahn, R.Julin, S.Juutinen, M.Luoma, J.Ojala, J.Pakarinen, J.Partanen, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, H.Tann, J.Uusitalo, G.Zimba, B.Cederwall, O.Aktas, A.Ertoprak, W.Zhang, S.Guo, M.L.Liu, I.Kuti, B.M.Nyako, D.Sohler, J.Timar, C.Andreoiu, M.Doncel, D.T.Joss, R.D.Page

Evidence of oblate-prolate shape coexistence in the strongly-deformed nucleus 119Cs

NUCLEAR REACTIONS 58Ni(64Zn, 3p), E=255 MeV; measured reaction products, Eγ, Iγ, γ-γ-γ-coin.; deduced γ-ray energies, J, π, partial level scheme, bands, oblate-prolate shape coexistence, level T1/2. Comparison with the particle-number conserving cranked shell model and two dimensional tilted axis cranking covariant density functional theory. JUROGAM 3+MARA setup at the Accelerator Laboratory of the University of Jyvaskyla, Finland.

doi: 10.1016/j.physletb.2021.136645
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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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2020BA10      Eur.Phys.J. A 56, 26 (2020)

S.N.Basilev, Yu.P.Bushuev, O.P.Gavrishchuk, V.V.Glagolev, D.A.Kirillov, N.V.Kostayeva, A.D.Kovalenko, K.S.Legostaeva, A.N.Livanov, I.A.Philippov, N.M.Piskunov, A.A.Povtoreiko, P.A.Rukoyatkin, R.A.Shindin, A.V.Shipunov, A.V.Shutov, I.M.Sitnik, V.M.Slepnev, I.V.Slepnev, A.V.Terletskiy, K.Hamilton, R.Montgomery, J.R.M.Annand, D.Marchand, Y.Wang, E.Tomasi-Gustafsson, C.F.Perdrisat, V.Punjabi, G.Martinska, J.Urban, J.Musinsky

Measurement of neutron and proton analyzing powers on C, CH, CH2 and Cu targets in the momentum region 3-4.2 GeV/c

doi: 10.1140/epja/s10050-020-00032-z
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2020CA06      Chin.Phys.C 44, 031001 (2020)

J.Cao, G.-y.Huang, Y.-F.Li, Y.Wang, L.-J.Wen, Z.-z.Xing, Z.-h.Zhao, S.Zhou

Towards the meV limit of the effective neutrino mass in neutrinoless double-beta decays

RADIOACTIVITY 130Te, 136Xe(2β-); analyzed available data; deduced Majorana neutrino mass limits.

doi: 10.1088/1674-1137/44/3/031001
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2020CA09      Chin.Phys.C 44, 031001 (2020)

J.Cao, G.-yu.Huang, Y.-F.Li, Y.Wang, L.-J.Wen, Z.-z.Xing, Z.-h.Zhao, S.Zhou

Towards the meV limit of the effective neutrino mass in neutrinoless double-beta decays

RADIOACTIVITY 136Xe(2β-); analyzed available data; deduced importance of neutrino Majorana mass sensitivity in future experiments.

doi: 10.1088/1674-1137/44/3/031001
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2020CU01      Phys.Rev. C 101, 014301 (2020), Erratum Phys.Rev. C 104, 029902 (2021)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Two-proton radioactivity within a generalized liquid drop model

RADIOACTIVITY 6Be, 12O, 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); calculated half-lives for 2p decay mode using generalized liquid drop model (GLDM) and compared with experimental half-lives, and other theoretical calculations. 22Si, 26S, 34Ca, 38,39Ti, 42Cr, 49Ni, 55Zn, 58,59,60Ge, 64Se(2p); predicted half-lives using GLDM for 2p radioactivity.

doi: 10.1103/PhysRevC.101.014301
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2020EP03      Phys.Rev. D 102, 012006 (2020)

C.S.Epstein, R.Johnston, S.Lee, J.C.Bernauer, R.Corliss, K.Dow, P.Fisher, I.Friscic, D.Hasell, R.G.Milner, P.Moran, S.G.Steadman, Y.Wang, J.Dodge, E.Ihloff, J.Kelsey, C.Vidal, C.M.Cooke

Measurement of Moller scattering at 2.5 MeV

NUCLEAR REACTIONS C(E, E'), E=2.5 MeV; measured reaction products, Eβ, Iβ; deduced σ(θ). Comparison with GEANT4 simulations.

doi: 10.1103/PhysRevD.102.012006
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2020GA03      Phys.Rev. C 101, 014612 (2020)

L.Gan, H.B.Sun, Z.H.Li, S.P.Hu, Y.J.Li, J.Su, B.Guo, S.Q.Yan, Y.B.Wang, S.Zeng, Z.Y.Han, X.Y.Li, D.H.Li, T.L.Ma, Y.P.Shen, Y.Su, E.T.Li, W.P.Liu

Experimental study of the spectroscopic factors of 116-125Sn

NUCLEAR REACTIONS 116,118,120,122,124Sn(p, d), E=18.0 MeV; 116,118,120,122,124Sn(d, p), E=12.0 MeV; measured E(p), I(p), E(d), I(d), σ(θ) using the high-precision Q3D magnetic spectrograph at the CIAE-Beijing HI-13 tandem accelerator. 115,117,119,121,123,125Sn; deduced levels, L-transfers, J, π, spectroscopic factors (SFs). DWBA analysis of σ(θ) data and extraction of the neutron spectroscopic factors using two different sets of systematic optical potential parameters. Comparison with previous experimental data. Proposed a linear formula to relate SFs with S(n).

doi: 10.1103/PhysRevC.101.014612
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2020GU16      Phys.Lett. B 807, 135572 (2020)

S.Guo, C.M.Petrache, D.Mengoni, Y.H.Qiang, Y.P.Wang, Y.Y.Wang, J.Meng, Y.K.Wang, S.Q.Zhang, P.W.Zhao, A.Astier, J.G.Wang, H.L.Fan, E.Dupont, B.F.Lv, D.Bazzacco, A.Boso, A.Goasduff, F.Recchia, D.Testov, F.Galtarossa, G.Jaworski, D.R.Napoli, S.Riccetto, M.Siciliano, J.J.Valiente-Dobon, M.L.Liu, G.S.Li, X.H.Zhou, Y.H.Zhang, C.Andreoiu, F.H.Garcia, K.Ortner, K.Whitmore, A.Atac Nyberg, T.Back, B.Cederwall, E.A.Lawrie, I.Kuti, D.Sohler, T.Marchlewski, J.Srebrny, A.Tucholski

Evidence for pseudospin-chiral quartet bands in the presence of octupole correlations

NUCLEAR STRUCTURE 131Ba; analyzed available data; calculated B(E1), three pairs of nearly degenerate doublet bands using the reflection-asymmetric triaxial particle rotor model.

doi: 10.1016/j.physletb.2020.135572
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2020HA27      Phys.Rev. C 102, 024625 (2020)

H.Haba, F.Fan, D.Kaji, Y.Kasamatsu, H.Kikunaga, Y.Komori, N.Kondo, H.Kudo, K.Morimoto, K.Morita, M.Murakami, K.Nishio, J.P.Omtvedt, K.Ooe, Z.Qin, D.Sato, N.Sato, T.K.Sato, Y.Shigekawa, A.Shinohara, M.Takeyama, T.Tanaka, A.Toyoshima, K.Tsukada, Y.Wakabayashi, Y.Wang, S.Wulff, S.Yamaki, S.Yano, Y.Yasuda, T.Yokokita

Production of 266Bh in the 248Cm(23Na, 5n)266Bh reaction and its decay properties

RADIOACTIVITY 266,267Bh(α)[from 248Cm(23Na, 5n), (23Na, 4n), E=125.9, 130.6, 135.3 MeV]; 262Db(α), (SF)[from 266Bh α decay]; 263Db(EC), (α), (SF)[from 267Bh α decay]; 263Rf(SF)[from 263Db EC decay]; 258Lr(α), (EC)[from 262Db α decay]; 259Lr(α), (SF)[from 263Db α decay]; 258No(SF)[from 258Lr(EC); measured Eα, αα-, ααα- and α(SF)-correlations for 32 observed events using rotating wheel apparatus MANON and gas-jet transport system coupled to gas-filled recoil ion separator GARIS at RIKEN; deduced decay times, half-lives, decay branching ratios, production cross sections for 266Bh and 267Bh. Comparison with previous experimental results for half-lives and branching ratios for decay modes.

NUCLEAR REACTIONS 248Cm(23Na, 5n), (23Na, 4n), E=125.9, 130.6, 135.3 MeV; measured reaction products, σ(E) at RIKEN. Comparison with HIVAP calculations, and with previous experimental results.

doi: 10.1103/PhysRevC.102.024625
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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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