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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

2024AP01      Eur.Phys.J. C 84, 138 (2024)

E.Aprile, K.Abe, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, M.Bazyk, L.Bellagamba, R.Biondi, A.Bismark, E.J.Brookes, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, J.M.R.Cardoso, D.Cichon, A.P.Cimental Chavez, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, J.P.Cussonneau, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, M.Flierman, W.Fulgione, C.Fuselli, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Glade-Beucke, L.Grandi, J.Grigat, H.Guan, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, N.F.Hood, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, A.Molinario, S.Moriyama, K.Mora, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, Q.Pellegrini, R.Peres, C.Peters, J.Pienaar, M.Pierre, G.Plante, T.R.Pollmann, J.Qi, J.Qin, D.Ramirez Garcia, N.Sarcevic, J.Shi, R.Singh, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, V.H.S.Wu, Y.Xing, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu, XENON collaboration

Design and performance of the field cage for the XENONnT experiment

doi: 10.1140/epjc/s10052-023-12296-y
Citations: PlumX Metrics

2024DA02      Phys.Rev. C 109, 014322 (2024)

S.Das, S.Bhattacharyya, S.Bhattacharya, S.Chakraborty, S.Shukla, P.C.Srivastava, R.Banik, S.Nandi, G.Mukherjee, I.Bala, S.S.Bhattacharjee, S.Das Gupta, A.Dhal, D.Mondal, S.Muralithar, R.Raut, A.Sharma, R.P.Singh, V.Srivastava

High-spin level structure of ²⁰⁹Rn

doi: 10.1103/PhysRevC.109.014322
Citations: PlumX Metrics

2024NA05      Nucl.Sci.Eng. 198, 771 (2024)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron–Induced Fission of ²³⁸Pu

NUCLEAR REACTIONS ²³⁸Pu(n, F), E ∼ 1.9 MeV; measured reaction products, Eγ, Iγ. ⁷⁸Ge, ^83,84Se, ^84,86Br, ^85,87,88,89Kr, ^89,90Rb, ^91,92,93,94Sr, ^{91,92,93,94,95}Y, ^95,97Zr, ^99,101Mo, ^{101,102,104,105}Tc, ^105,107,108Ru, ^105,109Rh, ^111,112,113Ag, ^115,117Cd, ^{123,125,127,128,129,130}Sn, ^{127,129,130,131}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135}I, ^135,137,138Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ¹⁴²La, ^{140,141,143,145,146}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^151,153Pm, ^{153,155,156,157}Sm; deduced cumulative and independent yields, nubar. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2023.2224274
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2024NA06      Appl.Radiat.Isot. 208, 111304 (2024)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Independent isomeric yield ratios of fission products in the epi-cadmium neutron induced fission of ²³³U

NUCLEAR REACTIONS ²³³U(n, F)¹²⁸Sb/¹³⁰Sb/¹³²Sb/¹³¹Te/¹³³Te/¹³⁴I/¹³⁶I/¹³⁵Xe/¹³⁸Cs, E ∼ 1.9 MeV; measured reaction products, Eγ, Iγ; deduced independent isomeric yield ratios (IR), root mean square fragment angular momenta. Comparison with available data. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1016/j.apradiso.2024.111304
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2024RA07      Phys.Rev. C 109, 024318 (2024)

R.Rahaman, A.Bisoi, A.Das, Y.Sapkota, A.Gupta, S.Ray, S.Sarkar, Yashraj, A.Sharma, Bh.Rohila, I.Ahmed, K.Katre, S.Dutt, S.Kumar, R.P.Singh, R.Kumar, S.Muralithar

Spectroscopic study of ⁴⁰K

doi: 10.1103/PhysRevC.109.024318
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2024RA11      J.Phys.(London) G51, 035104 (2024)

A.K.Rana, S.Sihotra, H.P.Sharma, V.Singh, G.H.Bhat, S.Jehangir, J.A.Sheikh, N.Rather, Kuldeep, N.Singh, R.K.Bhowmik, R.Kumar, R.P.Singh, S.Muralithar, P.Chauhan, D.S.Verma, T.Trivedi, S.Kumar, R.Palit, D.Mehta

Level structures of ⁹⁶Tc and their microscopic description

NUCLEAR REACTIONS ⁷⁵As(²⁸Si, 3n4p)⁹⁶Tc, E=120 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, energy level, J, π, partial level scheme, high-spin states, DCO and IPDCO ratios, multipolarities. Comparison with the framework of triaxial projected shell model calculations. The 15UD Pelletron accelerator facility at inter university accelerator centre (IUAC), New Delhi.

doi: 10.1088/1361-6471/ad1f2e
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2024SH08      Eur.Phys.J. A 60, (2024)

N.Sharma, Dh.Singh, A.Mahato, R.K.Sahoo, L.Chhura, P.K.Giri, Sn.B.Linda, H.Kumar, S.A.Tali, M.A.Ansari, R.Ali, S.Kumar, I.Ahmed, Yashraj, R.Kumar, K.S.Golda, S.Muralithar, R.P.Singh

Evidence of compound nucleus theory in the population of incompletely fused composite system ¹⁶⁰Dy*

NUCLEAR REACTIONS ¹⁴⁶Nd(¹⁸O, X)¹⁶¹Er/¹⁵⁹Er/¹⁵⁸Er/¹⁶¹Ho/¹⁵⁹Ho/¹⁵⁷Dy/¹⁵⁵Dy, E=68-102 MeV; measured reaction products, Eγ, Iγ. ¹⁶⁰Dy; deduced production σ, T_1/2. Comparison with available data and the predictions of statistical model code PACE-4 based on compound nucleus theory. 15UD Pelletron heavy ion accelerator facility of Inter-University Accelerator Centre (IUAC), New Delhi, India.

doi: 10.1140/epja/s10050-024-01293-8
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2024SH14      J.Radioanal.Nucl.Chem. 333, 1541 (2024)

N.Sharma, Dh.Singh, A.Mahato, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.A.Ansari, I.Ahmed, S.Kumar, Yashraj, R.Kumar, K.S.Golda, S.Muralithar, R.P.Singh

Role of incomplete fusion in production of ¹⁵⁵Tb

NUCLEAR REACTIONS ¹⁴⁶Nd(¹⁶O, X)¹⁵⁵Tb, E=3-7 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ. Comparison with PACE 4 calculations. General Purpose Scattering Chamber (GPSC) of Inter University Accelerator Centr e (IUAC), New Delhi, India.

doi: 10.1007/s10967-023-09111-z
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2023AP04      Phys.Rev. D 108, 072015 (2023)

E.Aprile, K.Abe, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, M.Bazyk, L.Bellagamba, R.Biondi, A.Bismark, E.J.Brookes, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, J.M.R.Cardoso, A.P.Cimental Chavez, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, M.Flierman, W.Fulgione, C.Fuselli, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Glade-Beucke, L.Grandi, J.Grigat, H.Guan, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, N.F.Hood, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, D.G.Layos Carlos, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, A.Molinario, S.Moriyama, K.Moraa, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, Q.Pellegrini, R.Peres, C.Peters, J.Pienaar, M.Pierre, G.Plante, T.R.Pollmann, J.Qi, J.Qin, D.Ramirez Garcia, J.Shi, R.Singh, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, V.H.S.Wu, Y.Xing, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu

Search for events in XENON1T associated with gravitational waves

doi: 10.1103/PhysRevD.108.072015
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2023CH32      J.Phys.(London) G50, 075106 (2023)

S.Chakraborty, H.P.Sharma, S.Jehangir, S.S.Tiwary, C.Majumder, A.K.Gupta, G.H.Bhat, J.A.Sheikh, N.Rather, P.Banerjee, S.Ganguly, S.Rai, Pragati, S.Muralithar, R.P.Singh, S.S.Bhattacharjee, S.Kumar, Mayank, A.Kumar, R.Palit

Three-quasineutron γ-band in ¹²⁷Xe

NUCLEAR REACTIONS ¹²²Sn(⁹Be, 4n), E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, J, π, partial level scheme, structures of negative parity multi-quasiparticle states, new negative parity bands. Comparison with the triaxial projected shell model (TPSM) approach. The Indian National Gamma Array (INGA), the 15UD pelletron accelerator facility at Inter-University Accelerator Centre (IUAC), New Delhi.

doi: 10.1088/1361-6471/acd86a
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2023CH36      Nucl.Phys. A1037, 122706 (2023)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, A.K.Gupta, P.Banerjee, S.Ganguly, S.Rai, Pragati, Mayank, S.Kumar, A.Kumar, R.Palit, S.S.Bhattacharjee, R.P.Singh, S.Muralithar

Incipient reflection asymmetry in ¹²⁷Xe

NUCLEAR REACTIONS ¹²²Sn(⁹Be, Xn)¹²⁷Xe/¹²⁶Xe/¹²⁸Xe, E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, J, π, partial level scheme, B(E1)/B(E2). 15UD palletron accelerator of Inter-University Accelerator Centre (IUAC), New Delhi.

doi: 10.1016/j.nuclphysa.2023.122706
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2023MA05      Phys.Rev. C 107, 014601 (2023)

A.Mahato, D.Singh, N.Sharma, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, A.Ali, M.Afzal Ansari, N.K.Deb, N.P.M.Sathik, S.Kumar, R.Kumar, S.Muralithar, R.P.Singh

Disentangling fractional momentum transfer in the ¹⁹F + ¹⁵⁴Sm system

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁹F, 5n)¹⁶⁸Lu, (¹⁹F, 6n)¹⁶⁷Lu, (¹⁹F, 5np)¹⁶⁷Yb, (¹⁹F, 3nα)¹⁶⁶Tm, (¹⁹F, 4nα)¹⁶⁵Tm, (¹⁹F, 5nα)¹⁶⁴Tm, (¹⁹F, 3n2α)¹⁶²Ho, (¹⁹F, 4n2α)¹⁶¹Ho, E=107 MeV; measured reaction products, evaporation residues (ERs), Eγ, Iγ; deduced ERs yields as a function of range in stopping medium, forward recoil range distributions (FRRDs) for the evaporation residues, range integrated σ, relative contributions of complete and incomplete fusion, mean ranges in stopping medium. Discussed linear momentum transfer from the projectile to target accounting also for projectile breakup α+¹⁵N and 2α+¹¹B. Activation technique. Beam from 15UD Pelletron accelerator facility at Inter University Accelerator Center (IUAC, India). ERs were collected with a stack of 26 aluminium catcher foils of different thicknesses placed immediately after the target. The decay of ERs on the catcher foils measured with HPGe detector.

doi: 10.1103/PhysRevC.107.014601
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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 T_1/2 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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2023MU10      Phys.Rev. C 107, 054310 (2023)

A.Mukherjee, S.Bhattacharya, T.Trivedi, S.Tiwari, R.P.Singh, S.Muralithar, Yashraj, K.Katre, R.Kumar, R.Palit, S.Chakraborty, S.Jehangir, N.Nazir, S.P.Rouoof, G.H.Bhat, J.A.Sheikh, N.Rather, R.Raut, S.S.Ghugre, S.Ali, S.Rajbanshi, S.Nag, S.S.Tiwary, A.Sharma, S.Kumar, S.Yadav, A.K.Jain

Evidence of transverse wobbling motion in ¹⁵¹Eu

NUCLEAR REACTIONS ¹⁴⁸Nd(⁷Li, 4n)¹⁵¹Eu, E=30 MeV; measured Eγ, Iγ, γγ-coin γγ(θ). ¹⁵¹Eu; deduced levels, J, π, high-spin states, directional correlation of oriented states (DCO) ratio, polarization asymmetries, mixing ratios, δ, rotational bands structure, B(E2_in)/B(E2_out), B(M1_in)/B(E2_out). Comparison to triaxial projected shell model calculations. Evidences of presence of transverse wobbling in ¹⁵¹Eu. Systematics of wobbling excitation energies for ¹⁵¹Eu, ¹³⁵Pr, ¹³³Ba, ¹⁸³Au, ¹⁸⁷Au, ¹³³La and ¹²⁷Xe. Indian National Gamma Array (INGA) consisting of 16 Compton suppressed clover detectors and 2 ancillary LEPS detectors at 15 UD pelletron (IUAC, New Delhi).

doi: 10.1103/PhysRevC.107.054310
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2023NA03      Nucl.Sci.Eng. 197, 25 (2023)

H.Naik, R.J.Singh, W.Jang

Post-Neutron Fission Product Yield Distribution in the Spontaneous Fission of ²⁴⁴Cm

RADIOACTIVITY ²⁴⁴Cm(SF); measured decay products, Eγ, Iγ. ⁸⁵Kr, ^87,88Kr, ^88,89Rb, ^91,92Sr, ⁹¹Y, ^93,94Y, ⁹⁵Zr, ⁹⁷Zr, ⁹⁹Mo, ¹⁰¹Mo, ¹⁰¹Tc, ^104,105Tc, ¹⁰³Ru, ¹⁰⁵Ru, ¹⁰⁸Ru, ¹⁰⁵Rh, ¹⁰⁹Rh, ^111,112,113Ag, ¹¹⁵Cd, ¹²⁷Sb, ^{129,130,131,132,133}Sb, ¹²⁸Sn, ¹³¹I, ^133,134I, ^{131,132,133,134}Te, ¹³⁵Xe, ^137,138Xe, ^138,139Cs, ^{139,140,141,142}Ba, ¹⁴¹Ce, ^143,144Ce, ¹⁴⁶Ce, ¹⁴⁶Pr, ^147,149,151Nd, ¹⁵¹Pm, ^155,156Sm; deduced post-neutron fission product yield distributions, parameters. Comparison with available data.

doi: 10.1080/00295639.2022.2103345
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33185.

2023NA10      Nucl.Sci.Eng. 197, 485 (2023)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-Neutron Mass Yield Distribution in the Thermal Neutron-Induced Fission of ²³⁵U

NUCLEAR REACTIONS ²³⁵U(n, F)⁷⁸As/⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁸Rb/⁸⁹Kr/⁸⁹Rb/⁹⁰Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Y/⁹⁵Y/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰¹Tc/¹⁰²Tc/¹⁰³Ru/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁷Ru/¹⁰⁸Ru/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹²⁹Sb/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Te/¹³³I/¹³⁴Te/¹³⁵I/¹³⁵Xe/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵²Nd/¹⁵³Pm/¹⁵³Sm/¹⁵⁵Sm, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent yields. Comparison with available data. The reactors CIRUS and APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2022.2133947
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2023NA13      Nucl.Sci.Eng. 197, 1133 (2023)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-Neutron Mass Yield Distribution in the Thermal Neutron Induced Fission of ²³³U

NUCLEAR REACTIONS ²³³U(n, F), E thermal; measured reaction products, Eγ, Iγ. Z=77-155; deduced cumulative, independent fission yields, mass chain yields. Comparison with available data. Two different reactor facilities at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2022.2142433
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2023NA14      Appl.Radiat.Isot. 197, 110804 (2023)

H.Naik, R.J.Singh, S.P.Dange

Charge distribution of light mass fission products in the thermal neutron induced fission of ²³³U, ²³⁵U and ²³⁹Pu

NUCLEAR REACTIONS ^233,235U, ²³⁹Pu(n, F), E thermal; measured reaction products, Eγ, Iγ. ^77,78Ga, ^79,80,83,84Ge, ^81,83,84As, ^{83,84,85,87,88}Se, ^{86,87,88,89,90}Br, ^{86,87,88,89,90,91,92,93,94,95}Kr, ^89,91Rb, ^91,92,93,94Sr, ^95,99Y, ^97,99,102Zr, ^101,104,105Mo, ^{103,104,105,106}Tc, ^104,105Nb, ^{105,107,108,109}Ru, ¹¹²Pd; deduced fractional cumulative yields, charge distribution parameters. The reactor CIRUS at Bhabha Atomic Research Centre (BARC), India, the reactor APSARA at BARC, India.

doi: 10.1016/j.apradiso.2023.110804
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2023NA17      Nucl.Sci.Eng. 197, 1265 (2023)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²²⁹Th

NUCLEAR REACTIONS ²²⁹Th(n, F)⁷⁷Ge/⁷⁸Ge/⁸³Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Rb/⁹¹Sr/⁹²Sr/⁹³Sr/⁹³Y/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰³Ru/¹⁰⁵Ru/¹⁰⁷Rh/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²⁷Sb/¹²⁸Sb/¹²⁹Sb/¹³¹I/¹³²Te/¹³³Te/¹³⁴Te/¹³³I/¹³⁴I/¹³⁵I/¹³⁸Xe/¹³⁸Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²La/¹⁴³Ce/¹⁴⁴Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Pm, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced post-neutron mass yields, cumulative product yields. The Standard I and Standard II asymmetric modes of fission. The highly enriched uranium–fueled light water–moderated swimming pool reactor APSARA.

doi: 10.1080/00295639.2022.2150029
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2023NA18      Nucl.Sci.Eng. 197, 1279 (2023)

H.Naik, R.J.Singh, W.Jang, S.P.Dange

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴⁵Cm

NUCLEAR REACTIONS ²⁴⁵Cm(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹³Sr/⁹³Y/⁹⁴Y/⁹⁵Y/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰²Tc/¹⁰³Ru/¹⁰⁵Rh/¹⁰⁷Ru/¹⁰⁷Rh/¹⁰⁸Ru/¹¹¹Ag/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹²⁹Sb/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹³⁴I/¹³⁴Te/¹³⁵I/¹³⁵Xe/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Pm/¹⁵³Pm/¹⁵³Sm/¹⁵⁶Sm/¹⁵⁷Eu/¹⁵⁸Eu/¹⁶¹Gd, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced relative and absolute cumulative and mass chain yields, comparison of mass yield distributions was made between the epi-cadmium and thermal neutron–induced fission to examine the role of excitation energy on the nuclear structure effect and P/V ratio. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2022.2153577
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2023NA29      Nucl.Sci.Eng. 197, 3110 (2023)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴¹Pu

NUCLEAR REACTIONS ²⁴¹Pu(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹⁰Rb/⁹¹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰¹Tc/¹⁰²Tc/¹⁰³Ru/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁵Rh/¹⁰⁷Ru/¹⁰⁷Rh/¹⁰⁸Ru/¹⁰⁹Rh/¹¹¹Ag/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁷Sb/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹²⁴Te/¹³⁴I/¹³⁵I/¹³⁵Xe/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Cs/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵²Nd/¹⁵³Pm/¹⁵³Sm/¹⁵⁵Sm/¹⁵⁶Sm/¹⁵⁷Eu, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced cumulative yields. Comparison with ENDF/B-VIII.0, JEFF-3.3 evaluated libraries. The reactor APSARA at the Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2023.2190725
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2023NA31      Eur.Phys.J. A 59, 230 (2023)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Charge distribution studies in the epi-cadmium neutron induced fission of ²⁴⁵Cm

NUCLEAR REACTIONS ²⁴⁵Cm(n, F)⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁹¹Sr/⁹²Sr/⁹³Sr/⁹⁵Y/⁹⁷Zr/¹⁰⁵Tc/¹⁰⁷Ru/¹⁰⁸Ru/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹²⁹Sb/¹³⁰Sb/¹³¹Sb/¹³³Sb/¹³¹Te/¹³²Te/¹³³Te/¹³⁴Te/¹³⁴I/¹³⁵I/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴²Ba/¹⁴⁴La/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁸Ce, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced fission yields, fractional cumulative yields (FCY) and charge distribution parameters, isotopic yield distribution. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1140/epja/s10050-023-01136-y
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2023PA23      Chin.Phys.C 47, 084002 (2023)

A.Pandey, R.Bhushan, A.Rohilla, C.Majumder, H.P.Sharma, S.Chakraborty, R.P.Singh, S.Muralithar, Yashraj, K.Katre, B.Rohila, Subodh, A.Kumar, I.M.Govil, S.Jehangir, N.Rather, G.H.Bhati, A.A.Wani, J.A.Sheikh, S.K.Chamoli

Revisiting band structures in ¹¹⁸Xe nucleus via in-beam γ-ray spectroscopy

NUCLEAR REACTIONS ⁹³Nb(²⁸Si, 2np), E=115 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, J, π, partial level scheme, DCO ratios, B(E1), B(E1)/B(E2), high-spin states. Comparison with Triaxial projected shell model (TPSM). The 15 UD pelletron accelerator facility at IUAC, New Delhi.

doi: 10.1088/1674-1137/acd83d
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2023SI03      Phys.Rev. C 107, 024911 (2023)

R.Singh, Y.Bailung, S.K.Kundu, A.Roy

Jet fragmentation via azimuthal angular correlations of electrons from heavy flavor decay in pp, p-Pb, and Pb-Pb collisions using PYTHIA8 + Angantyr calculations

doi: 10.1103/PhysRevC.107.024911
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2023SI04      Phys.Rev. C 107, 025206 (2023)

R.Singh, S.Khade, A.Roy

Jet fragmentation via azimuthal angular correlations of heavy flavors in pp collisions at √ s = 7 TeV

doi: 10.1103/PhysRevC.107.025206
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2023SI09      Phys.Rev. C 107, 054607 (2023)

R.K.Singh, N.L.Singh, M.Mehta, R.Chauhan, H.Kumawat, R.Makwana, S.V.Suryanarayana, B.K.Nayak, H.Naik, J.Varmuza, K.Katovsky

Experimental and theoretical study of the ⁶⁵Cu(n, p)⁶⁵Ni reaction cross section from reaction threshold up to 25 MeV

NUCLEAR REACTIONS ⁶⁵Cu(n, p), E=13.52, 16.86, 19.89 MeV; measured Eγ, Iγ; deduced σ(Ε) relative to standard ²⁷Al(n, α) cross-section. Comparison to other experimental data, TALYS and EMPIRE calculations, and evaluated values from ENDF/B-VIII.0, JEFF-3.3, JENDL-4.0/HE, CENDL-3.2, TENDL-2019, and FENDL-3.2 libraries. HPGe-based activation measurement at 14UD BARC-TIFR Pelletron facility (Mumbai, India).

doi: 10.1103/PhysRevC.107.054607
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2023SI14      Nucl.Phys. A1035, 122656 (2023)

R.Singh, M.Shokri, S.M.A.Tabatabaee Mehr

Relativistic hydrodynamics with spin in the presence of electromagnetic fields

doi: 10.1016/j.nuclphysa.2023.122656
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2023SI19      Appl.Radiat.Isot. 200, 110949 (2023)

R.K.Singh, N.L.Singh, M.Mehta, R.Chauhan, S.V.Suryanarayana, R.Makwana, B.K.Nayak, H.Naik, J.Varmuza, K.Katovsky

Activation cross section for the (n, 2n) and (n, p) reactions on ¹⁰³Rh, ⁴⁸Ti and ⁵²Cr from reaction threshold up to 25 MeV energy region

NUCLEAR REACTIONS ¹⁰³Rh(n, 2n), E<25 MeV; measured reaction products, Eγ, Iγ. ⁵²Cr, ⁴⁸Ti, ¹⁰³Rh; deduced σ, nuclear level densities, optical potential. Comparison with TALYS and EMPIRE codes calculations, FENDL-3.2b, CENDL-3.2, JENDL-5.0, and ENDF/B-VIII.0 libraries. The 14UD BARC-TIFR Pelletron facility in Mumbai, India.

doi: 10.1016/j.apradiso.2023.110949
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2023YA12      Phys.Rev. C 107, 054303 (2023)

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

High-spin spectroscopy in ²⁰⁷At: Evidence of a 29/2⁺ isomeric state

NUCLEAR REACTIONS ¹⁹⁸Pt(¹⁴N, 5n)²⁰⁷At, E=80-87 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization) using INGA array of 13 Compton-suppressed HPGe detectors at the 15-UD tandem accelerator of the IUAC-New Delhi facility. Deduced high-spin levels, J, π, bands, multipolarities, new high-spin isomer, and configurations. Comparison with large-scale shell model calculations using KHM3Y effective interaction. Systematics of energies low-lying states in ^{116,118,120,122,126}At and ^{116,118,120,122,126}Po, and B(E3) in At isotopes. Systematics of energies of 13/2+ states in ^{199,201,203,205,207}At.

doi: 10.1103/PhysRevC.107.054303
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2023YA20      Nucl.Phys. A1036, 122685 (2023)

Yashraj, U.S.Ghosh, I.Ahmed, R.Kumar, R.P.Singh

Shell model based description of single-particle and collective excitations in ⁶⁶Zn

NUCLEAR STRUCTURE ⁶⁵Zn; calculated energy levels, J, π, kinematic moment of inertia in model space using two different interactions jj44bpn and jun45pn. Comparison with available data.

doi: 10.1016/j.nuclphysa.2023.122685
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2022BH04      Phys.Rev. C 106, 044312 (2022)

S.Bhattacharya, T.Trivedi, A.Mukherjee, D.Negi, R.P.Singh, S.Muralithar, S.Jehangir, G.H.Bhat, N.Nazir, J.A.Sheikh, N.Rather, R.Palit, S.Nag, S.Rajbanshi, S.Chakraborty, S.Kumar, M.Kumar Raju, V.V.Parkar, D.Choudhury, R.Kumar, R.K.Bhowmik, S.C.Pancholi, A.K.Jain

Evidence for prolate-oblate shape coexistence in the odd-A ⁷³₃₅Br₃₈ nucleus

NUCLEAR REACTIONS ⁵⁰Cr(²⁸Si, pα)⁷³Br, E=90 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), ⁷³Br; deduced levels, J, π, high-spin states states, bands structure, δ, T_1/2 of 9/2⁺ excited state, polarization asymmetry, DCO and ADO ratios. Comparison to Projected shell model (PSM) calculations and other experimental data. Systematics of monopole transition strength in ⁷³Br, calculated from the semiempirical approach with neighboring Se, Br, and Kr. Evidences provided for the prolate-oblate shape coexistence at low excitation energy. INGA array at IUAC, New Delhi.

doi: 10.1103/PhysRevC.106.044312
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2022CH50      Phys.Rev. C 106, 044329 (2022)

S.Chatterjee, B.Mondal, A.Ghosh, D.Arora, S.Das, S.Samanta, R.Raut, S.S.Ghugre, P.C.Srivastava, A.K.Sinha, U.Garg, H.K.Singh, Neelam, K.Rojeeta Devi, A.Sharma, S.S.Bhattacharjee, R.Garg, I.Bala, R.P.Singh, S.Muralithar

Single-particle configurations of the excited states of ²⁰³Po

NUCLEAR REACTIONS ¹⁹⁴Pt(¹³C, 4n), (¹³C, 3n), E=74 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). ²⁰³Po; deduced levels, J, π, polarization asymmetry, ratio of angular distribution from oriented nuclei, linear polarisation of the transitions, δ, T_1/2 of 2789-keV state, high-spin states. ²⁰⁴Po; deduced T_1/2 of 3387-keV state. Comparison to other experimental data and large basis shell-model calculation using the KHH7B Hamiltonian. Indian National Gamma Array (INGA) consisting of 18 Compton suppressed HPGe clover detectors at 15UD Pelletron accelerator facility (IUAC, New Delhi).

doi: 10.1103/PhysRevC.106.044329
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2022DE09      Phys.Rev. C 105, 044307 (2022)

P.Dey, D.Negi, R.Palit, P.C.Srivastava, Md.S.R.Laskar, B.Das, F.S.Babra, S.Bhattacharya, B.Das, K.Rojeeta Devi, R.Gala, U.Garg, S.S.Ghugre, E.Ideguchi, S.Kumar, A.Kundu, G.Mukherjee, S.Muralithar, S.Nag, S.Nandi, Neelam, M.K.Raja, R.Raut, R.Santra, A.Sharma, S.Sihotra, A.K.Singh, R.P.Singh, T.Trivedi

Experimental investigation of high-spin states in ⁹⁰Zr

NUCLEAR REACTIONS ⁸²Se(¹³C, 5n), E=60 MeV; measured Eγ, Iγ, γγγ-coin, γ(θ). ⁹⁰Zr; deduced levels, J, π, DCO ratios, polarization asymmetry, multipolarity, high-spin states, bands structure, configurations. Comparison to shell-model calculations with the GWBXG effective interaction. Indian National Gamma Array (INGA) at TIFR-BARC Pelletron Linac Facility.

doi: 10.1103/PhysRevC.105.044307
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2022JO02      Phys.Rev. C 105, 034615 (2022)

C.Joshi, H.Kumawat, V.V.Parkar, D.Dutta, S.V.Suryanarayana, V.Jha, R.K.Singh, N.L.Singh, S.Kailas

Inclusive α production for the ⁶Li + ⁵¹V system

NUCLEAR REACTIONS ⁵¹V(⁶Li, X), E=14, 20, 23, 26 MeV; measured charged particles, Eα, Iα, deuteron spectra, angular distributions; deduced σ(θ) for α production, σ(E) for α and deuteron production, direct and compound contribution to the α production; calculated σ(E) of complete fusion, α production by compound nuclear reactions, noncapture breakup, 1n transfer, 1p transfer, 1d transfer and total direct α production. Statistical calculations of compound reactions and total fusion are done with PACE code. FRESCO (CDCC and CRC) used for transfer reactions calculations. Comparison with experimental data of α productions with ⁶Li beam on ⁵⁸Ni, ¹¹⁸Sn, ¹²⁰Sn, ⁵⁹Co, ⁶⁵Cu, ⁹⁰Zr, ¹⁵⁹Tb, ²⁰⁸Pb, ²⁰⁹Bi targets. BARC-TIFR Pelletron-Linac facility.

doi: 10.1103/PhysRevC.105.034615
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2022JO03      Eur.Phys.J. A 58, 40 (2022)

C.Joshi, H.Kumawat, R.K.Singh, N.L.Singh, D.Patel, B.K.Nayak, J.Acharya, A.Parihari, K.Rani, S.D.Sharma, G.Kaur, I.Ahmed, K.S.Golda, N.Saneesh, M.Kumar, A.Jhingan, P.Sugathan

Exploring breakup coupling effect in ⁷Li+^{92, 100}Mo elastic scattering around Coulomb barrier energies

NUCLEAR REACTIONS ^92,100Mo(⁷Li, ⁷Li), E=15-35 MeV; measured reaction products; deduced σ, optical model potentials. Comparison with continuum-discretized coupled-channels calculations. The General Purpose Scattering Chamber (GPSC) facility at Inter University Accelerator Centre (IUAC), New Delhi.

doi: 10.1140/epja/s10050-022-00690-1
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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 T_1/2 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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2022KU25      Int.J.Mod.Phys. E31, 2250061 (2022)

B.Kumari, M.K.Singh, R.Singh, V.Singh

Emission feature of the shower particles produced in backward hemisphere in the interaction of ⁸⁴Kr₃₆ + Em at 1 A GeV

NUCLEAR REACTIONS Ag, Br(⁸⁴Kr, X), E=1 GeV/nucleon; measured reaction products; deduced emission probability of the shower particle, correlations, fitting parameters. The nuclear emulsion detector (NED), GSI, Germany.

doi: 10.1142/S0218301322500616
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2022MA16      Phys.Rev. C 105, 034308 (2022)

Madhu, K.Yadav, A.Y.Deo, Pragati, P.C.Srivastava, S.K.Tandel, S.G.Wahid, S.Kumar, S.Muralithar, R.P.Singh, I.Bala, S.S.Bhattacharjee, R.Garg, S.Chakraborty, S.Rai, A.K.Jain

Evolution of nuclear structure through isomerism in ²¹⁶Fr

NUCLEAR REACTIONS ²⁰⁸Pb(¹¹B, 3n), E=54-62 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. ²¹⁶Fr; deduced high-spin isomers, J, π, T_1/2 of isomeric states, γ-ray branching ratios, B(E1), B(M2), single-particle transition rates, configurations. Half-lives extracted using centroid-shift and decay-curve analyses. Systematics of the 11⁺ isomers properties in the ²¹⁶Fr, ²¹²At, ²¹⁸Ac. Comparison to the shell-model calculations. Beam from 15 UD Pelletron accelerator at Inter-University Accelerator Centre (IUAC). Detector system - Indian National Gamma Array (INGA) with 14 Compton suppressed clover HPGe.

doi: 10.1103/PhysRevC.105.034308
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2022MA34      Phys.Rev. C 106, 014613 (2022)

A.Mahato, D.Singh, N.Sharma, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, A.Ali, N.K.Deb, N.P.M.Sathik, S.Kumar, R.Kumar, S.Muralithar, R.P.Singh

Effects of entrance channels on breakup fusion induced by ¹⁹F projectiles

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁹F, X), (¹⁹F, 4n), (¹⁹F, 5n), (¹⁹F, 6n), (¹⁹F, 5np), (¹⁹F, 3nα), (¹⁹F, 4nα), (¹⁹F, 5nα), (¹⁹F, 3n2α), (¹⁹F, 4n2α)E=78-110 MeV; measured Eγ, Iγ; deduced complete fusion and evaporation residues production σ(E), critical angular momentum, excitation functions for complete, incomplete fusion and total fusion. Incomplete fusion strength functions systematics for ¹⁶O, ¹⁹F, ^20Ne induced reactions. Activation technique measurement with HPGe detector. Comparison to statistical model calculations (PACE-4 code) and coupled channels (CCFULL code). 15UD Pelletron accelerator facility at the Inter-University Accelerator Center (IUAC), New Delhi.

doi: 10.1103/PhysRevC.106.014613
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2022ME05      Appl.Radiat.Isot. 182, 110142 (2022)

M.Mehta, N.L.Singh, R.Singh, R.Chauhan, R.Makwana, S.V.Suryanarayana, H.Naik, P.V.Subhash, S.Mukherjee, J.Varmuza, K.Katovsky

Cross-section of (n, 2n) reaction for niobium and strontium isotopes between 13.97 to 20.02 MeV neutron energies

NUCLEAR REACTIONS ⁹³Nb, ⁸⁸Sr(n, 2n), E=13.97-20.02 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS-1.9 calculations, EXFOR library. The 14UD BARC-TIFR (Bhabha Atomic Research Center-Tata Institute of Fundamental Research) Pelletron facility in Mumbai-India.

doi: 10.1016/j.apradiso.2022.110142
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2022MU03      Phys.Rev. C 105, 014322 (2022)

A.Mukherjee, S.Bhattacharya, T.Trivedi, R.P.Singh, S.Muralithar, D.Negi, R.Palit, S.Nag, S.Rajbanshi, M.Kumar Raju, S.Kumar, D.Choudhury, R.Kumar, R.K.Bhowmik, S.C.Pancholi, A.K.Jain

Shape coexistence and octupole correlations in ⁷²Se

NUCLEAR REACTIONS ⁵⁰Cr(²⁸Si, 2pα)⁷²Se, E=90 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(θ)(ADO), γγ-linear polarization asymmetries using INGA array of 17 Compton-suppressed clover detectors at the 15UD Pelletron accelerator of IUAC, New Delhi. ⁷²Se; deduced high-spin levels, J, π, multipolarities, multipole mixing ratios, Kπ=0+ bands, γ-band, alignments, B(E1)/B(E2) ratios, octupole correlations, intrinsic dipole moment D₀ for the octupole band; calculated single-particle energy as a function of β₂ for fixed triaxiality and hexadecapole deformation parameters, single-particle proton and neutron energy levels; bands interpreted in terms of the total Routhian surface (TRS) calculations. Systematics of B(E1)/B(E2) ratios and D₀ values for ⁷²Se, ⁷³Br, ^114,116,117Xe, ¹²⁵Ba, and for energies of 3- states for ^{70,72,74,76,78,80,82}Se.

doi: 10.1103/PhysRevC.105.014322
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2022MU19      Eur.Phys.J. A 58, 250 (2022)

S.Muralithar, N.Madhavan, P.Sugathan, R.P.Singh, A.Jhingan, R.Kumar, S.Nath, K.S.Golda, J.Gehlot

Nuclear reaction and structure studies using experimental facilities at Inter-University Accelerator Centre (IUAC)

doi: 10.1140/epja/s10050-022-00855-y
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2022NA02      Appl.Radiat.Isot. 179, 109993 (2022)

H.Naik, S.P.Dange, R.J.Singh

Charge distribution of light mass fission products in the fast neutron induced fission of ²³⁷Np, ²⁴¹Am and ²⁴³Am

NUCLEAR REACTIONS ²³⁷Np(n, F)⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹⁰Kr/⁹¹Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰³Mo/¹⁰⁵Tc/¹⁰⁶Tc/¹⁰⁷Ru, ²⁴¹Am(n, F)⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹⁰Kr/⁹¹Rb/⁹²Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰³Mo/¹⁰⁵Tc/¹⁰⁶Tc/¹⁰⁸Ru, ²⁴³Am(n, F)⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹²Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰⁵Tc/¹⁰⁶Tc/¹⁰⁸Ru, E thermal; measured reaction products, Eγ, Iγ; deduced fractional cumulative yields, charge distribution parameters. Comparison with available data.

doi: 10.1016/j.apradiso.2021.109993
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2022NA04      Nucl.Sci.Eng. 196, 16 (2022)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²³⁷Np

NUCLEAR REACTIONS ²³⁷Np(n, F), E ∼ 0.5 eV; measured reaction products, Eγ, Iγ. ^78,81As, ⁸⁰Ge, ^83,84Se, ^84,86,87Br, ^{85,87,88,89,90}Kr, ^88,89,90Rb, ^91,92,93,94Sr, ^91,93,94,95Y, ^95,97Zr, ^99,101,103Mo, ^{102,103,104,105}Tc, ^{103,105,107,108}Ru, ^105,107,109Rh, ^111,112,113Ag, ^115,117Cd, ^{123,125,127,129,130}Sn, ^{127,129,130,131}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135}I, ^135,137,139Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ^{141,143,144,145,146,147}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^149,151,153Pm, ^153,155,156Sm, ^156,157Eu; deduced cumulative or independent fission yields, mass chain yields. Comparison with ENDF/B-VIII.0, available data.

doi: 10.1080/00295639.2021.1951078
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2022NA12      Appl.Radiat.Isot. 182, 110137 (2022)

H.Naik, S.P.Dange, R.J.Singh

Charge distribution of heavy mass fission products in the thermal neutron induced fission of ²³³U, ²³⁵U and ²³⁹Pu

NUCLEAR REACTIONS ^233,235U, ²³⁹Pu(n, F), E thermal; measured reaction products, Eγ, Iγ. ^{127,128,129,130,131,132}Sn, ^{129,130,131,132}Sb, ^{131,132,133,134,136,137}Te, ^{134,135,136,137,138,139,140}I, ^{136,137,138,139,140,141,142,143,144}Xe, ^{139,140,142,143}Cs, ^{140,141,142,143,144,145,146}Ba, ^144,145,147La, ^{146,147,148,149}Ce; deduced fractional cumulative yields (FCY), isobaric charge distribution. Comparison with available data, ENDF/B library.

doi: 10.1016/j.apradiso.2022.110137
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2022NA14      Nucl.Sci.Eng. 196, 433 (2022)

H.Naik, R.J.Singh, W.Jang, S.P.Dange

Post-Neutron Mass Yield Distribution in the Thermal Neutron Induced Fission of ²³²U

NUCLEAR REACTIONS ²³²U(n, F), E thermal; measured reaction products, Eγ, Iγ. ^72,73,74Ga, ^77,78Ge, ⁷⁸As, ⁸¹As, ^83,84Se, ⁸⁴Br, ^86,87Br, ⁸⁵Kr, ^87,88,89,90Kr, ^88,89,90,91Rb, ^91,92,93,94Sr, ^{91,92,93,94,95}Y, ⁹⁹Mo, ¹⁰¹Mo, ^{101,102,103,104,105,106}Tc, ⁹⁵Zr, ⁹⁷Zr, ¹⁰³Ru, ¹⁰⁵Rh, ¹⁰⁷Rh, ¹²³Sn, ¹²⁵Sn, ^{127,128,129,130}Sn, ^{128,129,130,131,132,133}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ¹³⁵Xe, ^137,138,139Xe, ^138,139,140Cs, ¹⁴¹Ce, ¹⁴³Ce, ^145,146Ce, ¹⁴⁸Ce, ¹⁴⁶Pr, ¹⁴⁷Nd, ¹⁴⁹Nd, ^151,152Nd, ¹⁵¹Pm, ¹⁵³Pm, ¹⁵³Sm, ^155,156Sm, ^157,158Eu; measured reaction products, Eγ, Iγ; deduced cumulative and independent yields of various fission products, mass yield distributions. Comparison with available data, EXFOR library. Off-line gamma-ray spectrometric technique. The highly enriched uranium-fueled light water-moderated swimming pool reactor APSARA.

doi: 10.1080/00295639.2021.1993425
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33173.

2022NA18      Nucl.Sci.Eng. 196, 694 (2022)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴³Am

NUCLEAR REACTIONS ²⁴³Am(n, F), E∼0.5 eV; measured reaction products, Eγ, Iγ. ^83,82Se, ^84,86,87Br, ^85,87,89Kr, ^89,90Rb, ^91,92,93,94Sr, ^{91,82,93,94,95}Y, ^95,97Zr, ^99,101Mo, ^{102,104,105,106}Tc, ^103,105,108Ru, ^105,107,109Rh, ^{111,112,113,116}Ag, ¹¹⁷Cd, ¹¹⁹In, ^{123,125,127,128,129,130}Sn, ^{127,128,129,130,131,132,133}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ^135,137,138Xe, ^138,138,140Cs, ^{139,140,141,142}Ba, ^142,144La, ^{141,143,145,146,148}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^151,153Pm, ^155,156Sm, ^157,158Eu; deduced mass yields, cumulative yields of fission products, the average number of neutrons. Two different reactor facilities in Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2021.2014753
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33174.

2022NA21      Nucl.Sci.Eng. 196, 824 (2022)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-Neutron Mass Yield Distribution in the Thermal Neutron-Induced Fission of ²³⁹Pu

NUCLEAR REACTIONS ²³⁹Pu(n, F), E thermal; measured reaction products, Eγ, Iγ. ^78,81As, ^79,80Ge, ^83,84Se, ^84,86,87Br, ^{85,87,88,89,90}Kr, ^88,89,90,91Rb, ^91,92,93,94Sr, ^91,92,93,94Y, ^95,97Zr, ^99,101Mo, ^{101,102,103,104,105,106}Tc, ^{105,107,108,109}Ru, ^105,109Rh, ^111,113,116Ag, ¹¹⁷Cd, ¹¹⁹In, ^{123,125,127,128,129,130}Sn, ^129,130,131Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ^{135,137,138,139}Xe, ^{139,140,141,142}Ba, ^142,144La, ^{141,143,145,146,147}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^151,153,154Pm, ^{153,155,156,157}Sm, ^158,159Eu; deduced cumulative or independent yields. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries. The reactors CIRUS and APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2021.2025298
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33178.

2022NA25      Nucl.Sci.Eng. 196, 982 (2022)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴¹Am

NUCLEAR REACTIONS ²⁴¹Am(n, F), E ∼ 0.5 eV; measured reaction products, Eγ, Iγ. ⁸⁰Ge, ⁸¹As, ^83,84Se, ⁸⁴Br, ^86,87Br, ⁸⁵Kr, ^87,88,89,90Kr, ^89,90,91Rb, ^91,92Sr, ^91,92,93,94Y, ⁹⁵Zr, ⁹⁷Zr, ^99,101,103Mo, ¹⁰²Tc, ^104,105,106Tc, ^103,105Ru, ¹⁰⁸Ru, ^105,107,109Rh, ^111,113Ag, ¹¹⁶Ag, ^115,117Cd, ¹¹⁹In, ^{123,125,127,129}Sn, ¹³⁰Sn, ^{129,130,131,132,133}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ¹³⁵Xe, ^137,138,139Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ^142,144La, ^140,141Ce, ^{143,144,145,146}Ce, ¹⁴⁸Ce, ¹⁴⁶Pr, ^147,149Nd, ¹⁵¹Pm, ^153,154Pm, ¹⁵³Sm, ^155,156,157Sm, ^157,158Eu, ^159,161Gd; deduced cumulative, independent and chain yields. Comparison with evaluated data. Two reactor facilities of Bhabha Atomic Research Centre (BARC) in India.

doi: 10.1080/00295639.2022.2038529
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33179.

2022NI05      Physics of Part.and Nuclei 53, 441 (2022)

Niyti, A.Deep, R.Kharab, R.Singh, S.Chopra

Study of Decay Properties of ²⁶⁰Sg^* Nucleus Formed in ⁵²Cr + ²⁰⁸Pb Reaction by Using GSkI Skyrme Force

NUCLEAR REACTIONS ²⁰⁸Pb(⁵²Cr, X)²⁶⁰Sg, E=13.3, 18.6 MeV; analyzed available data; deduced σ using the Dynamical Cluster-decay Model (DCM).

doi: 10.1134/S1063779622020642
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2022SH01      Nucl.Instrum.Methods Phys.Res. B511, 1 (2022)

A.Sharma, S.K.Dhiman, S.Muralithar, R.P.Singh, S.Chakraborty, K.Katre, S.R.Abhilash, D.Kabiraj, Meenakshi, G.R.Umapathy

Fabrication and characterization of ¹⁶⁹Tm target for Nuclear Lifetime Measurements

NUCLEAR REACTIONS ¹⁶⁹Tm(¹⁸O, 4n)¹⁸³Ir, E=94 MeV; measured reaction products, Eγ, Iγ, X-rays, γ-X-ray coin.; deduced γ-ray energies and relative intensities, high-spin states. Doppler broadened lineshapes of gamma transitions. The target laboratory of Inter-University Accelerator Centre, New Delhi. Two HPGe low energy photon spectrometer (LEPS) of the Indian National Gamma array (INGA).

doi: 10.1016/j.nimb.2021.10.014
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2022SI10      Phys.Rev. C 105, 035202 (2022)

R.Singh, Y.Bailung, A.Roy

Dynamics of particle production in Pb-Pb collisions at √ S_NN=2.76 TeV using the PYTHIA8 Angantyr model

doi: 10.1103/PhysRevC.105.035202
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2022SI15      Chin.Phys.C 46, 054002 (2022)

R.K.Singh, N.L.Singh, R.D.Chauhan, M.Mehta, S.V.Suryanarayana, R.Makwana, B.K.Nayak, H.Naik, T.N.Nag, K.Katovsky

Systematic study of the (n, 2n) reaction cross section for ¹²¹Sb and ¹²³Sb isotopes

NUCLEAR REACTIONS ^121,123Sb(n, 2n), ²⁷Al(n, α), E=12.50, 15.79, 18.87 MeV; measured reaction products, Eγ, Iγ; deduced relative σ and covariances. Comparison with JEFF-3.3, ENDF/B-VIII.0, JENDL/AD-2017 and TENDL-2019 libraries. TALYS-1.9 and EMPIRE-3.2.2 calculations, experimental data. The BARC-TIFR Pelletron Linac Facility, Mumbai, India.

doi: 10.1088/1674-1137/ac4a5a
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2022VA03      Phys.Rev. C 105, 044613 (2022)

V.Vashi, R.Makwana, B.Quintana, M.H.Mehta, B.K.Soni, S.Mukherjee, R.K.Singh, R.Chauhan, P.M.Prajapati, M.Abhangi, S.Vala, N.L.Singh, G.B.Patel, S.V.Suryanarayana, B.K.Nayak, S.C.Sharma, T.N.Nag, Y.Kavun

Cross-section measurement of the ¹¹⁴Cd(p, γ)^115mIn reaction for nuclear reactor and astrophysical applications

NUCLEAR REACTIONS ¹¹⁴Cd(p, γ), (p, n), E=7.83, 12.27, 16 MeV; measured Eγ, Iγ; deduced σ(E), astrophysical S-factor. Comparison to TALYS calculations and other experimental data. Activation techniques. BARC-TIFR Pelletron facility.

doi: 10.1103/PhysRevC.105.044613
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6428.

2022YA10      Phys.Rev. C 105, 034307 (2022)

K.Yadav, A.Y.Deo, Madhu, Pragati, P.C.Srivastava, S.K.Tandel, S.G.Wahid, S.Kumar, S.Muralithar, R.P.Singh, I.Bala, S.S.Bhattacharjee, R.Garg, S.Chakraborty, S.Rai, A.K.Jain

Level structure in the transitional nucleus ²¹⁵Fr

NUCLEAR REACTIONS ²⁰⁸Pb(¹¹B, 4n), E=54-62 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, γγγ-coin. ²¹⁵Fr; deduced levels, high-spin states, J, π, δ, DCO-ratios, γ-ray multipolarities, polarization, T_1/2 of the excited states, configurations; calculated levels, J, π, B(E2), B(M1), B(E3), δ. Large scale shell model calculations with CD-Bonn NN potential. Discussed possible structure of yrast and near-yrast lines. Beam from 15 UD Pelletron accelerator at Inter-University Accelerator Centre (IUAC). Detector system - Indian National Gamma Array (INGA) with 14 Compton suppressed clover HPGe.

doi: 10.1103/PhysRevC.105.034307
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Data from this article have been entered in the XUNDL database. For more information, click here.

2021BA43      Phys.Rev. C 104, 044302 (2021)

I.Bala, S.C.Pancholi, M.K.Raju, A.Dhal, S.Saha, J.Sethi, T.Trivedi, R.Raut, S.S.Ghugre, R.Palit, R.P.Singh, S.Muralithar

Collective and noncollective states in ⁶⁶Zn

NUCLEAR REACTIONS ⁵⁶Fe(¹²C, 2p)⁶⁶Zn, E≈62 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization) using INGA array at the 14UD pelletron accelerator of TIFR-Mumbai. ⁶⁶Zn; deduced high-spin levels, J, π, multipolarities, bands, upper limit of half-life of 2826, 3- level from line-shape analysis of Doppler-shifted peaks, alignments, B(E1)/B(E2) ratios, configurations, large octupole correlations from B(E1) values; calculated levels, J, π, average particle occupancies, quasiparticle energies for proton and neutron, total routhian surface (TRS) for zero quasiparticle configuration using shell model in fpg model space and jj44bpn effective interaction. Comparison between experimental results and theoretical model calculations.

doi: 10.1103/PhysRevC.104.044302
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Data from this article have been entered in the XUNDL database. For more information, click here.

2021CH23      Int.J.Mod.Phys. E30, 2150030 (2021)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, A.K.Gupta, A.Kumar, P.Banerjee, S.Ganguly, S.Kumar, A.Kumar, R.P.Singh, S.Muralithar

Octupole correlations in ¹²⁷I

NUCLEAR REACTIONS ¹²⁴Sn(⁷Li, 4n), E=33 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, B(E1)/B(E2), intrinsic electric dipole moment, γ-ray angular distribution asymmetry ratios.

doi: 10.1142/S0218301321500300
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Data from this article have been entered in the XUNDL database. For more information, click here.

2021CH58      Int.J.Mod.Phys. E30, 2150085 (2021)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, A.K.Gupta, P.Banerjee, S.Ganguly, S.Rai, Pragati, Mayank, S.Kumar, S.S.Bhattacharjee, R.P.Singh, S.Muralithar, A.Kumar, R.Palit

A note on the parity of I^π = 5^- state in ^{126, 128}Xe

NUCLEAR REACTIONS ¹²²Sn(⁹Be, 5n), (⁹Be, 3n), E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, level scheme, Weisskopf transition rates, Directional Correlations from Oriented states ratios (RDCO) and linear polarization asymmetries. The 15UD pelletron accelerator facility of Inter-University Accelerator Centre, New Delhi. INGA spectrometer.

doi: 10.1142/S0218301321500853
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Data from this article have been entered in the XUNDL database. For more information, click here.

2021KA31      Int.J.Mod.Phys. E30, 2150053 (2021)

S.Kalkal, S.Mandal, N.Madhavan, A.Jhingan, S.Nath, E.Prasad, R.Sandal, S.Goyal, M.Saxena, G.Mohanto, S.Verma, B.R.Behera, S.Kumar, U.Datta, A.K.Sinha, R.Singh, S.Noor

Ground state and excited state multinucleon transfer channels in interactions of ²⁸Si with ^{90, 94}Zr in near barrier region

NUCLEAR REACTIONS ^90,94Zr(²⁸Si, X), E=95.5 MeV; measured reaction products; deduced ground and excited states transfer reaction yields.

doi: 10.1142/S0218301321500531
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2021MA50      Nucl.Phys. A1014, 122236 (2021)

I.Majeed Bhat, Mohd.Shuaib, M.S.Asnain, V.R.Sharma, A.Yadav, M.K.Sharma, P.P.Singh, D.P.Singh, R.Kumar, R.P.Singh, S.Muralithar, B.P.Singh, R.Prasad

Systematic study of fusion-fission like events in ¹⁹F + ¹⁷⁵Lu interactions at low energies

NUCLEAR REACTIONS ¹⁷⁵Lu(¹⁹F, X)¹²⁰Xe/⁹⁹Tc/⁷⁹Rb/¹⁰⁷In/¹²⁹Ba/¹⁰⁸In/⁸⁴Rb/⁷⁴Kr/⁹⁰Mo/¹²³Xe/¹²²Xe/¹⁰⁹In/¹²¹Xe/¹²⁹La/¹²¹I/¹¹¹In/⁸¹Rb/⁹⁵Ru/⁸⁹Rb/⁸²Rb/⁹⁸Nb, E=105, 110 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, σ, isotopic yield and isobaric charge distributions, fractional independent yields, mass distributions.

doi: 10.1016/j.nuclphysa.2021.122236
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6402.

2021ME10      J.Radioanal.Nucl.Chem. 328, 71 (2021)

M.Mehta, N.L.Singh, R.K.Singh, S.Parashari, P.V.Subhash, H.Naik, R.D.Chauhan, R.Makwana, S.V.Suryanarayana, S.Mukherjee, A.Gandhi, J.Varmuza, K.Katovsky

Measurement of ⁹⁰Zr(n, 2n)⁸⁹Zr and ⁹⁰Zr(n, p)^90mY reaction cross-sections in the neutron energy range of 10.95 to 20.02 MeV

NUCLEAR REACTIONS ⁹⁰Zr(n, 2n), (n, p), E=10.95-20.02 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS-1.9 and EMPIRE-3.2.2 calculations.

doi: 10.1007/s10967-021-07625-y
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33156.

2021NA05      Eur.Phys.J. A 57, 112 (2021)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass yield distribution in the epi-cadmium neutron induced fission of ²⁴⁰Pu

NUCLEAR REACTIONS ²⁴⁰Pu(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹⁰Rb/⁹¹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰³Mo/¹⁰²Tc/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰³Ru/¹⁰⁵Ru/¹⁰⁸Ru/¹⁰⁵Rh/¹⁰⁹Rh/¹¹¹Ag/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹³⁰Sn/¹²⁷Sb/¹²⁹Sb/¹³⁰Sb/¹³¹Sb/¹³²Sb/¹³³Sb/¹³¹Te/¹³²Te/¹³³Te/¹³⁴Te/¹³¹I/¹³²I/¹³³I/¹³⁴I/¹³⁵I/¹³⁶I/¹³⁵Xe/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹⁴⁰Cs/¹⁴¹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴²Ba/¹⁴²La/¹⁴⁴La/¹⁴¹Ce/¹⁴³Ce/¹⁴⁴Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁷Ce/¹⁴⁸Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵³Sm/¹⁵⁵Sm/¹⁵⁶Sm/¹⁵⁷Eu, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields. Comparison with experimental data, EXFOR and ENDF/B-VIII.0 libraries.

doi: 10.1140/epja/s10050-021-00377-z
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33155.

2021NA07      Appl.Radiat.Isot. 173, 109718 (2021)

H.Naik, R.J.Singh, S.P.Dange

Charge distribution of light mass fission products in the ²³²U(n_th, f), ²³⁸Pu(n_th, f) and ²⁴⁴Cm(SF) reactions

NUCLEAR REACTIONS ²³²U, ²³⁸Pu(n, F)⁸¹As/⁸³Se/⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹⁰Kr/⁹¹Rb/⁹¹Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰³Mo/¹⁰⁵Tc/¹⁰⁷Ru/¹⁰⁸Ru, E thermal; measured reaction products, Eγ, Iγ; deduced fractional cumulative yields of various light mass fission products, charge distribution parameters. Comparison with available data.

RADIOACTIVITY ²⁴⁴Cm(SF); measured decay products, Eγ, Iγ. ^91,92,94Sr, ⁹⁷Zr, ¹⁰¹Mo, ¹⁰⁵Tc, ^105,108Ru, ¹¹²Pd; deduced fractional cumulative yields of various light mass fission products, charge distribution parameters. Comparison with available data.

doi: 10.1016/j.apradiso.2021.109718
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33157.

2021NA09      Nucl.Sci.Eng. 195, 717 (2021)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-Neutron Mass Yield Distribution in the Spontaneous Fission of ²⁵²Cf

RADIOACTIVITY ²⁵²Cf(SF); measured decay products, Eγ, Iγ; deduced cumulative and independent yields of various fission products, mass yield distribution parameters.

doi: 10.1080/00295639.2020.1866389
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33158.

2021NA10      Eur.Phys.J.Plus 136, 694 (2021)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass chain yield distribution in the epi-cadmium neutron-induced fission of ²³²Th

NUCLEAR REACTIONS ²³²Th(n, F)⁷⁸As/⁸⁰Ge/⁸¹As/⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁶Br/⁸⁷Br/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹⁰Kr/⁹⁰Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰¹Tc/¹⁰²Tc/¹⁰³Mo/¹⁰³Tc/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁶Tc/¹⁰⁷Rh/¹⁰⁸Ru/¹⁰⁹Rh/¹¹²Ag/¹¹³Ag/¹¹⁶Ag/¹¹⁷Cd/¹¹⁹Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹²⁹Sb/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹³⁴Te/¹³⁴I/¹³⁵I/¹³⁵Xe/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Xe/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Cs/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁴La/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Ce/¹⁴⁷Nd/¹⁴⁸Ce/¹⁴⁹Nd/¹⁵¹Nd/¹⁵²Nd/¹⁵³Pm, E>0.5 eV; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields. Comparison with ENDF/B-VIII.0 evaluations, available data.

doi: 10.1140/epjp/s13360-021-01690-8
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2021NA12      Eur.Phys.J. A 57, 176 (2021)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Mass yield distribution in the fission of ²⁴⁴Cm induced by a spectrum of epi-cadmium to fast neutron

NUCLEAR REACTIONS ²⁴⁴Cm(n, F), E>0.0253 eV; measured reaction products, Eγ, Iγ. ^83,84Se, ^84,86,87Br, ^{85,87,88,89,90}Kr, ^89,90,91Rb, ^91,92,93,94Sr, ^92,93,94,95Y, ^95,97Zr, ^99,101,103Mo, ^102,104,105Tc, ^103,105,108Ru, ^105,107,109Rh, ^{111,112,113,116}Ag, ^115,117Cd, ¹¹⁹In, ^{123,125,127,128,129,130}Sn, ^{127,129,130,131,132,133}Sb, ^{131,132,133,134,135,136}I, ^{131,132,133,134}Te, ^135,137,138Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ^{141,143,144,145,146,147,148}Ce, ^142,144La, ¹⁴⁶Pr, ^147,149,151Nd, ^151,153Pm, ^153,155,156Sm, ^157,158Eu; deduced mass chain yields of fission products. Comparison with ENDF/B-VIII.0 library.

doi: 10.1140/epja/s10050-021-00485-w
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33159.

2021NA15      Ann.Nucl.Energy 162, 108493 (2021)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-neutron mass yield distribution in the thermal neutron induced fission of ²³⁸Pu

NUCLEAR REACTIONS ²³⁸Pu(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁶Br/⁸⁷Br/⁸⁷Kr/⁸⁸Kr/⁸⁸Br/⁸⁸Rb/⁸⁹Kr/⁸⁹Rb/⁹⁰Kr/⁹⁰Rb/⁹¹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰²Tc/¹⁰³Tc/¹⁰³Ru/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁷Ru/¹⁰⁷Rh/¹⁰⁸Ru/¹⁰⁹Rh/¹¹²Ag/¹²⁵Sn/¹²⁷Sn/¹²⁷Sb/¹²⁸Sn/¹²⁸Sb/¹²⁹Sn/¹²⁹Sb/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹³⁴Te/¹³⁴I/¹³⁵I/¹³⁵Xe/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Xe/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Cs/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁴La/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁸Ce/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵³Sm/¹⁵⁵Sm, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields, chain yields. Comparison with JEFF-3.3 evaluations, experimental data.

doi: 10.1016/j.anucene.2021.108493
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33160.

2021PA01      Nucl.Instrum.Methods Phys.Res. A985, 164667 (2021)

A.Pandey, R.Bhushan, A.Rohilla, C.Majumder, S.Chakraborty, R.P.Singh, A.Kapil, S.K.Chamoli

Fabrication of thin Nb target for lifetime measurements of short lived excited nuclear states

NUCLEAR REACTIONS ⁹³Nb(²⁸Si, 2np)¹¹⁸Xe, E=115 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π. DSAM lifetime measurement experiment.

doi: 10.1016/j.nima.2020.164667
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2021PA43      Phys.Rev. C 104, 064905 (2021)

S.Panda, S.Chatterjee, A.Dash, B.Mohanty, R.Paikaray, S.Samanta, R.Singh

Multiplicity dependence of freezeout scenarios in pp collisions at √ s = 7 TeV

doi: 10.1103/PhysRevC.104.064905
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2021RO24      Phys.Lett. B 823, 136756 (2021)

K.Rojeeta Devi, S.Kumar, N.Kumar, Neelam, F.S.Babra, M.S.R.Laskar, S.Biswas, S.Saha, P.Singh, S.Samanta, S.Das, S.Chakraborty, R.P.Singh, S.Muralithar, A.Kumar

Observation of multiphonon transverse wobbling in ¹³³Ba

NUCLEAR REACTIONS ¹²⁴Sn(¹³C, 4n), E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, directional correlation from oriented states ratio and polarization asymmetry parameters, wobbling bands. Total Routhian Surface (TRS) calculations. 14-UD pelletron at Tata Institute of Fundamental Research (TIFR). Indian National Gamma Array (INGA) spectrometer.

doi: 10.1016/j.physletb.2021.136756
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2021SH09      Phys.Rev. C 103, 024324 (2021)

A.Sharma, R.Raut, S.Muralithar, R.P.Singh, S.S.Bhattacharjee, S.Das, S.Samanta, S.S.Ghugre, R.Palit, S.Jehangir, N.Rather, G.H.Bhat, J.A.Sheikh, S.S.Tiwary, Neelam, P.V.Madhusudhana Rao, U.Garg, S.K.Dhiman

Evidence of antimagnetic rotational motion in ¹⁰³Pd

NUCLEAR REACTIONS ⁹⁴Zr(¹³C, 4n)¹⁰³Pd, E=55 MeV; measured Eγ, Iγ, half-lives of levels in the negative-parity yrast band by Doppler-shift attenuation method (DSAM) using the INGA array of 18 Compton suppressed HPGe clover detectors. ¹⁰³Pd; deduced levels, J, π, B(E2), configurations, dynamic moment of inertia, antimagnetic rotational (AMR) band structure; calculated total Routhian surface (TRS) contour for the negative-parity yrast band in (β₂cos(γ+30°), β₂sin(γ+30°)) plane, and quasiparticle Routhians for proton and neutron using cranked-shell model. Comparison of spin versus angular frequency distribution and B(E2) values with tilted-axis cranked-shell model calculations based on the covariant density functional theory, and with semi-classical particle-rotor model calculations.

doi: 10.1103/PhysRevC.103.024324
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2021SI34      Eur.Phys.J. A 57, 337 (2021)

R.K.Singh, N.L.Singh, R.D.Chauhan, M.Mehta, S.V.Suryanarayana, R.Makwana, S.Mukherjee, B.K.Nayak, H.Naik, T.N.Nag, J.Varmuza, K.Katovsky

Neutron induced reaction cross section of ⁵¹V with covariance analysis

NUCLEAR REACTIONS ⁵¹V(n, p), E=7.87, 13.05, 16.98 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, JENDL/AD-2017 libraries, TALYS calculations. The 14UD BARC-TIFR Pelletron Facility, Mumbai, India.

doi: 10.1140/epja/s10050-021-00638-x
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33168.

2021TO09      Phys.Lett. B 821, 136603 (2021)

D.Tonev, G.de Angelis, I.Deloncle, N.Goutev, G.De Gregorio, P.Pavlov, I.L.Pantaleev, S.Iliev, M.S.Yavahchova, P.G.Bizzeti, A.Demerdjiev, D.T.Dimitrov, E.Farnea, A.Gadea, E.Geleva, C.Y.He, H.Laftchiev, S.M.Lenzi, S.Lunardi, N.Marginean, R.Menegazzo, D.R.Napoli, F.Nowacki, R.Orlandi, H.Penttila, F.Recchia, E.Sahin, R.P.Singh, M.Stoyanova, C.A.Ur, H.-F.Wirth

Transition probabilities in ³¹P and ³¹S: A test for isospin symmetry

NUCLEAR REACTIONS ²⁰Ne(¹²C, p), (¹²C, n)³¹P/³¹S, E=33 MeV from Piave-Alpi accelerator of LNL-Legnaro; measured Eγ, Iγ, γγ-coin, (proton)γγ-coin, γγ(θ), level T_1/2 by DSAM and line-shape analysis using GASP array for γ rays and EUCLIDES Si-ball for charged particles. ³¹S, ³¹P; deduced levels, J, π, multipolarity, mixing ratios, B(E1), B(M2), violation of isospin symmetry for mirror nuclei. Comparison with Self-consistent beyond mean field calculations using Equation of Motion method based on a chiral potential, and with previous experimental data.

doi: 10.1016/j.physletb.2021.136603
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2020CH05      Nucl.Phys. A996, 121687 (2020)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Rai, Pragati, Mayank, S.Kumar, A.Kumar, R.Palit, S.S.Bhattacharjee, R.P.Singh, S.Muralithar

γ-vibration in ¹²⁶Xe: A revisit

doi: 10.1016/j.nuclphysa.2019.121687
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2020CH11      Eur.Phys.J. A 56, 50 (2020)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Rai, P.Popli, S.Modi, P.Arumugam, M.Singh, S.Kumar, A.Kumar, S.S.Bhattacharjee, R.P.Singh, S.Muralithar, R.Palit

Signature splitting in the positive parity bands of ¹²⁷Xe

doi: 10.1140/epja/s10050-020-00066-3
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2020CH36      J.Phys.(London) G47, 095104 (2020)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Kumar, A.Kumar, A.Kumar, R.P.Singh, S.Muralithar

Indication of g-vibration in ^{123, 125, 127}I

NUCLEAR REACTIONS ¹²⁴Sn(⁷Li, 4n), E=33 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies, level schemes, bands, high-spin states, possible existence of γ-vibration and chiral rotation. Comparison with systematics.

doi: 10.1088/1361-6471/ab97c8
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2020CH46      Phys.Lett. B 811, 135854 (2020)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, A.K.Gupta, P.Banerjee, S.Ganguly, S.Rai, Pragati, Mayank, S.Kumar, A.Kumar, R.Palit, S.S.Bhattacharjee, R.P.Singh, S.Muralithar

Multiphonon longitudinal wobbling in ¹²⁷Xe

NUCLEAR REACTIONS ¹²²Sn(⁹Be, X)¹²⁷Xe, E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, E2 fraction, wobbling bands. Comparison with available data.

doi: 10.1016/j.physletb.2020.135854
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2020CH48      J.Phys.(London) G47, 015103 (2020)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Rai, Pragati, S.Muralithar, R.P.Singh, S.S.Bhattacharjee, S.Kumar, Mayank, A.Kumar, R.Palit

Possible antimagnetic rotational band in ¹²⁷Xe

NUCLEAR REACTIONS ¹²²Sn(⁹Be, 4n)¹²⁷Xe, E=48 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and intensities, branching ratios, J, π, bands. Comparison with semiclassical particles-plus-rotor model calculations.

doi: 10.1088/1361-6471/ab5374
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2020DA01      Acta Phys.Pol. B51, 103 (2020)

P.Das, H.K.Singh, U.Lamani, S.Muralithar, R.P.Singh

Nuclear shapes and symmetries seen through measurement of short lifetimes

NUCLEAR REACTIONS ¹²⁴Sn(⁷Li, 5n)¹²⁶I, E=50 MeV; ¹¹⁶Cd(¹⁹F, 5n)¹³⁰La, E=94 MeV; measured reaction products, Eγ, Iγ; deduced energy levels, J, π, B(E2). Doppler shift attenuation method (DSAM).

doi: 10.5506/APhysPolB.51.103
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2020DE33      Phys.Rev. C 102, 034607 (2020)

A.Deep, Niyti, R.Kharab, R.Singh, S.Chopra

Examining the entrance channel effects on the synthesis of the double deformed nucleus ²⁷⁰Hs: A theoretical study using the dynamical cluster-decay model including Skyrme forces

NUCLEAR REACTIONS ²⁶Mg(²⁴⁸Cm, xn)²⁷⁴Hs^*,36S(²³⁸U, xn)²⁷⁴Hs^*,48Ca(²²⁶Ra, xn)²⁷⁴Hs^*, E^*=40-51 MeV; calculated fusion evaporation residue cross sections for 3n-, 4n- and 5n-channels, mass fragmentation potentials, preformation yields, excitation function of individual 3n- to 5n-evaporation channels, best-fitted neck-length parameter using dynamical cluster-decay model (DCM), with Skyrme energy density functionals. Comparison with experimental data. Relevance to super-heavy nuclei.

doi: 10.1103/PhysRevC.102.034607
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2020GH08      Phys.Rev. C 102, 024328 (2020)

U.S.Ghosh, S.Rai, B.Mukherjee, A.Biswas, A.K.Mondal, K.Mandal, A.Chakraborty, S.Chakraborty, G.Mukherjee, A.Sharma, I.Bala, S.Muralithar, R.P.Singh

Spectroscopic investigation of complex nuclear excitations in ⁶⁶Ga

NUCLEAR REACTIONS ⁵²Cr(¹⁸O, 3np)⁶⁶Ga, E=72.5 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization) using the INGA array of 14 Compton-suppressed HPGe clover detectors at the 15-UD pelletron accelerator of IUAC-New Delhi. ⁶⁶Ga; deduced high-spin levels, J, π, bands, multipolarities, configurations. Comparison with shell model calculations with jj44bpn and jun45pn interactions using NUSHELLX@MSU code. Comparison with data in the ENSDF database, and with ⁶⁸Ga structure.

NUCLEAR STRUCTURE ⁶⁶Ga; calculated levels, J, π, occupation probabilities of the f_5/2, p_3/2, p_1/2, and g_9/2 orbitals for protons and neutrons, configurations with the highest probabilities using shell model with jj44bpn and jun45pn interactions and NUSHELLX@MSU code. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.024328
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2020KU22      Nucl.Phys. A1002, 121973 (2020)

H.Kumawat, C.Joshi, V.V.Parkar, V.Jha, B.J.Roy, Y.S.Sawant, P.C.Rout, E.T.Mirgule, R.K.Singh, N.L.Singh, B.K.Nayak, S.Kailas

Elastic scattering for ⁶Li+⁵¹V and systematic study of breakup threshold anomaly

NUCLEAR REACTIONS ⁵¹V(⁶Li, ⁶Li), E=14-23 MeV; measured reaction products; deduced σ. Comparison with theoretical calculations.

doi: 10.1016/j.nuclphysa.2020.121973
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6386.

2020MA22      Eur.Phys.J. A 56, 131 (2020)

A.Mahato, D.Singh, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh

Probing of incomplete fusion dynamics in ¹⁴N + ¹²⁴Sn system and its correlation with various entrance channel effects

doi: 10.1140/epja/s10050-020-00126-8
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2020MA55      J.Phys.(London) G46, 125104 (2020)

C.Majumder, H.P.Sharma, S.Chakraborty, S.S.Tiwary, R.P.Singh, S.Muralithar, I.Bala, S.S.Bhattacharjee, R.Garg, Neelam, A.Sharma, P.V.Madhusudhana Rao

Lifetime measurements in ¹⁰⁴Pd

NUCLEAR REACTIONS ⁹⁴Zr(¹³C, 3n), E=55 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, lifetimes, B(E2), negative parity bands. Comparison with Woods-Saxon total Routhian surface calculations.

doi: 10.1088/1361-6471/abb785
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2020NA07      Eur.Phys.J. A 56, 82 (2020)

H.Naik, R.J.Singh, S.P.Dange

Post-neutron mass chain yield distribution in the thermal neutron induced fission of ²²⁹Th

doi: 10.1140/epja/s10050-020-00080-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33139.

2020NA22      Eur.Phys.J. A 56, 186 (2020)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass yield distribution in the thermal neutron induced fission of ²⁴¹Pu

NUCLEAR REACTIONS ²⁴¹Pu(n, f), E=thermal; measured cumulative yields, post-neutron mass yields of fission products with mass A=83-115, 125-157 using charge distribution correction, independent yields of fission products with mass A=83-115, 125-157; deduced full width and tenth maxima (FWTM) of light- and heavy-mass yields[ reaction compared with ²²⁹Th(n, f) data; deduced nuclear structure effect - mass yield distribution in neutron-induced fission are fine structurearound asymmetric with triple humps for light-Z actinides, asymmetric with double humps for medium actinides (they have the higher mass yield, compared to EXFOR compilation of fission yield data); deduced fission products T_1/2, γ-ray evaluated abundance; compared to EXFOR compilation of fission yield data; yields compared with present work and with more than 10 other fission yields.

doi: 10.1140/epja/s10050-020-00184-y
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2020NA32      Eur.Phys.J. A 56, 227 (2020)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass yield distribution in the thermal neutron induced fission of ²⁴⁵Cm

NUCLEAR REACTIONS ²⁴⁵Cm(n, F), E thermal; measured fission products, Eγ, Iγ. ^83,84Se, ⁸⁴Br, ⁸⁵Kr, ^86,87Br, ^87,88,89,90Kr, ^{87,88,89,90,91}Rb, ^91,92,93,94Sr, ^{91,92,93,94,95}Y, ^91,92,93,94Sr, ^95,97Zr, ^100,101Mo, ¹⁰³Mo, ^{102,103,104,105,106}Tc, ¹⁰³Ru, ¹⁰⁵Ru, ^107,108,109Ru, ^105,107,109Rh, ^111,112,113Ag, ¹¹⁶Ag, ^115,117Cd, ¹¹⁹In, ^123,125,127Sn, ^128,129,130Sn, ^{128,129,130,131}Sb, ^{131,132,133,134,135,136}I, ^{131,132,133,134}Te, ¹³⁵Xe, ^137,138,139Xe, ^{138,139,140,141}Cs, ^{139,140,141,142}Ba, ^142,144La, ^{141,143,145,147}Ce, ¹⁴⁸Ce, ¹⁴⁶Pr, ^147,149Nd, ¹⁵²Nd, ¹⁵¹Pm, ^153,154Pm, ^{152,153,154,155,156,157}Sm, ^157,158,159Eu, ^161,162Gd; deduced cumulative, independent and chain yields. Comparison with ENDF/B-VIII.0 library.

doi: 10.1140/epja/s10050-020-00228-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33145.

2020RA28      Phys.Rev. C 102, 064313 (2020)

S.Rai, U.S.Ghosh, B.Mukherjee, A.Biswas, A.K.Mondal, K.Mandal, A.Chakraborty, S.Chakraborty, G.Mukherjee, A.Sharma, I.Bala, S.Muralithar, R.P.Singh

Evolution of collectivity and shape transition in ⁶⁶Zn

NUCLEAR REACTIONS ⁵²Cr(¹⁸O, 2n2p)⁶⁶Zn, E=72.5 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization) using INGA array of 14 Compton-suppressed HPGe Clover detectors at the tandem accelerator facility of IUAC-New Delhi. ⁶⁶Zn; deduced levels, J, π, multipolarities, configurations, alignments, terminating states, shape transitions; calculated total Routhian surfaces (TRS) based on Hartree-Fock-Bogoliuobov formalism.

doi: 10.1103/PhysRevC.102.064313
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2020SO05      Acta Phys.Pol. B51, 775 (2020)

A.Sood, P.Kumar, R.N.Sahoo, P.P.Singh, A.Yadav, V.R.Sharma, M.K.Sharma, R.Kumar, R.P.Singh, S.Muralithar, B.P.Singh, R.K.Bhowmik

Evidence of Narrow Range High Spin Population in Incomplete Fusion

doi: 10.5506/APhysPolB.51.775
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2020TI04      Phys.Scr. 95, 095304 (2020)

S.S.Tiwary, H.P.Sharma, S.Chakraborty, C.Majumder, A.K.Gupta, S.Modi, P.Arumugam, P.Banerjee, S.Ganguly, K.Rojeeta Devi, Neelam, S.Kumar, S.K.Chamoli, A.Sharma, V.V.Jyothi, Mayank, A.Kumar, S.S.Bhattacharjee, I.Bala, S.Muralithar, R.P.Singh

Structure of positive parity states in ¹³⁹Pm

NUCLEAR REACTIONS ¹²⁷I(¹⁶O, 4n)¹³⁹Pm, E=84 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, partial level scheme, bands. Comparison with systematics, particle rotor model calculations.

doi: 10.1088/1402-4896/abaea8
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2020WA24      Phys.Rev. C 102, 024329 (2020)

S.G.Wahid, S.K.Tandel, S.Suman, M.Hemalatha, A.Patel, P.Roy, A.Y.Deo, Pragati, P.C.Srivastava, B.Bhoy, S.S.Bhattacharjee, R.P.Singh, S.Muralithar, P.Chowdhury, R.V.F.Janssens, M.P.Carpenter, T.L.Khoo, F.G.Kondev, T.Lauritsen, C.J.Lister, D.Seweryniak, S.Zhu, S.Rai, A.Sharma

Metastable states from multinucleon excitations in ²⁰²Tl and ²⁰³Pb

NUCLEAR REACTIONS ¹⁹⁸Pt(⁷Li, 3n)²⁰²Tl, E=31-36 MeV; ¹⁹⁷Au(²⁰⁹Bi, X), E=1450 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization), half-lives of isomers by γ(t) and centroid-shift method using the INGA array at IUAC-New Delhi for the ²⁰²Tl experiment, and Gammasphere array at the ATLAS-ANL facility for ²⁰³Pb. ²⁰²Tl, ²⁰³Pb; deduced high-spin levels, isomers, J, π, multipolarities, B(E2), B(E3), configurations. Systematics of energies and B(Eλ) for isomers in ^202,203,204Tl and ^203,204,205Pb. Comparison with shell-model calculations.

doi: 10.1103/PhysRevC.102.024329
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2019BH04      Phys.Rev. C 100, 014315 (2019)

S.Bhattacharya, T.Trivedi, D.Negi, R.P.Singh, S.Muralithar, R.Palit, I.Ragnarsson, S.Nag, S.Rajbanshi, M.Kumar Raju, V.V.Parkar, G.Mohanto, S.Kumar, D.Choudhury, R.Kumar, R.K.Bhowmik, S.C.Pancholi, A.K.Jain

Evolution of collectivity and evidence of octupole correlations in ⁷³Br

NUCLEAR REACTIONS ⁵⁰Cr(²⁸Si, pα), E=90 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(lin pol), and level half-lives by DSAM and line-shape method using the INGA array at 15UD Pelletron accelerator of IUAC. ⁷³Br; deduced high-spin levels, J, π, multipolarities, bands, octupole band, B(E2), B(E1), B(M1), B(E1)/B(E2) ratios, transition quadrupole moments, configurations, octupole correlations, possible band termination at higher spin; calculated low-lying configurations, total Routhian surfaces using cranked Nilsson-Strutinsky method, and compared with experimental data.

doi: 10.1103/PhysRevC.100.014315
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2019CH15      Europhys.Lett. 125, 52001 (2019)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Rai, Pragati, Mayank, S.Kumar, A.Kumar, S.S.Bhattacharjee, R.P.Singh, S.Muralithar

Search for the 23/2⁺ isomeric state in ¹²⁵ Te

NUCLEAR REACTIONS ¹²²Sn(⁹Be, X)¹²⁵Te, E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, high-spin states, isomeric state. Comparison with systematics.

doi: 10.1209/0295-5075/125/52001
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2019CH28      Eur.Phys.J. A 55, 46 (2019)

S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Muralithar, R.P.Singh, G.H.Bhat, J.A.Sheikh, R.Palit

γ-vibration in ¹⁹⁸Hg

NUCLEAR REACTIONS ¹⁹⁷Au(⁷Li, α2nγ), E=33, 38 MeV; measured Eγ, Iγ, γγ-coin using Indian Gamma Ray Array (INGA) of 15 Compton suppressed clover detector using Collection and Analysis of Nuclear Data using Linux nEtwork (CANDLE) CAMAC-based data acquisition system; calculated band structure using microscopic Triaxial Projected Shell Model (TPSM); deduced E(4⁺)/E(2⁺) ratio vs nuclear mass (isotopes of Hg, Pt, Os), γ-ray transitions, low-lying levels, J, π using Directional Correlation of Oriented states (DCO) ratios, linear polarization asymmetries.

doi: 10.1140/epja/i2019-12707-5
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2019DE31      Int.J.Mod.Phys. E28, 1950079 (2019)

A.Deep, Niyti, R.Kharab, R.Singh, S.Chopra

Skyrme forces and isotopic dependence of evaporation residue cross-section in the decay of ^{252, 254-256}No^* formed in ^{204, 206, 207, 208}Pb ⁴⁸Ca reactions

NUCLEAR REACTIONS ^{204,206,207,208}Pb(⁴⁸Ca, X)^{252,254,255,256}No, E=20-45 MeV; analyzed available data; calculated preformation yields and probabilities, σ.

RADIOACTIVITY ^{252,254,255,256}No(n), (2n), (3n), (4n); analyzed available data; deduced fusion evaporation residue σ for he decay of compound nuclei using the Skyrme energy density functional (SEDF)-based on semi-classical extended Thomas Fermi (ETF) approach under frozen density approximation.

doi: 10.1142/S0218301319500794
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2019FL05      Phys.Rev. C 99, 044910 (2019)

W.Florkowski, A.Kumar, R.Ryblewski, R.Singh

Spin polarization evolution in a boost-invariant hydrodynamical background

doi: 10.1103/PhysRevC.99.044910
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2019GH09      Phys.Rev. C 100, 034314 (2019)

U.S.Ghosh, S.Rai, B.Mukherjee, A.Biswas, A.K.Mondal, K.Mandal, A.Chakraborty, S.Chakraborty, G.Mukherjee, A.Sharma, I.Bala, S.Muralithar, R.P.Singh

In-beam spectroscopic study of ⁶³Zn

NUCLEAR REACTIONS ⁵²Cr(¹⁸O, 3nα), E=72.5 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), linear polarization asymmetries using the INGA array with 14 Compton-suppressed HPGe clover detectors at the 15-UD pelletron accelerator of IUAC-New Delhi. ⁶³Zn; deduced high-spin levels, J, π; calculated total-Routhian surfaces (TRS) using Hartree-Fock-Bogoliubov approach. Comparison with shell-model calculations.

NUCLEAR STRUCTURE ⁶³Zn; calculated levels, J, π, proton and neutron orbitals occupation probabilities using shell model code NUSHELLX with jj44bpn interaction in the f_5/2pg_9/2 model space; calculated TRS, and collective excitations with triaxial and prolate shapes using a computer code based on Hartree-Fock-Bogoliubov approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.034314
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Data from this article have been entered in the XUNDL database. For more information, click here.

2019GI15      Phys.Rev. C 100, 024621 (2019)

P.K.Giri, D.Singh, A.Mahato, S.B.Linda, H.Kumar, S.A.Tali, S.Parasari, A.Ali, M.Afzal Ansari, R.Dubey, R.Kumar, S.Muralithar, R.P.Singh

Systematic study of low-energy incomplete-fusion dynamics in the ¹⁶O + ¹⁴⁸Nd system: Role of target deformation

NUCLEAR REACTIONS ¹⁴⁸Nd(¹⁶O, 3n)¹⁶¹Er, ¹⁴⁸Nd(¹⁶O, 5n)¹⁵⁹Er, ¹⁴⁸Nd(¹⁶O, 6n)¹⁵⁸Er, ¹⁴⁸Nd(¹⁶O, 2np)¹⁶¹Ho, ¹⁴⁸Nd(¹⁶O, 3np)¹⁶⁰Ho, ¹⁴⁸Nd(¹⁶O, 4np)¹⁵⁹Ho, ¹⁴⁸Nd(¹⁶O, 3nα)¹⁵⁷Dy, ¹⁴⁸Nd(¹⁶O, 5nα)¹⁵⁵Dy, ¹⁴⁸Nd(¹⁶O, 4npα)¹⁵⁵Tb, E=67.2, 72.4, 77.4, 84.1, 89.1, 94.7, 99.9 MeV; measured Eγ, Iγ; deduced σ(E), incomplete fusion (ICF) σ(E), effect of target deformation; analyzed previous experimental σ(E) data for many other systems for fraction of incomplete fusion. Measured σ compared with statistical model code PACE-4, and with previous experimental data. Experiment was performed using the 15UD Pelletron accelerator facility at Inter-University Accelerator Centre (IUAC), New Delhi, India.

doi: 10.1103/PhysRevC.100.024621
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6368.

2019GI17      Phys.Rev. C 100, 054604 (2019)

P.K.Giri, A.Mahato, D.Singh, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh

Examination of break-up fusion in the ¹⁶O + ¹⁴⁸Nd system through measurements of forward recoil range distributions and angular distributions

NUCLEAR REACTIONS ¹⁴⁸Nd(¹⁶O, 6n)¹⁵⁸Er, (¹⁶O, 5n)¹⁵⁹Er, (¹⁶O, 4np)¹⁵⁹Ho, (¹⁶O, 3np)¹⁶⁰Ho, (¹⁶O, 5nα)¹⁵⁵Dy, (¹⁶O, 3nα)¹⁵⁷Dy, (¹⁶O, 4npα)¹⁵⁵Tb, E AP 6 MeV/nucleon; measured Eγ, Iγ off-line, σ(θ) and forward recoil range distributions (FRRD) for evaporation residues, yields of evaporation residues using the 15 UD Pelletron facility at IUAC-New Delhi; deduced σ(θ) for total and complete fusion; analyzed incomplete fusion (ICF) fraction for several parameters using data from the present system, and previous experimental data for 16 other systems (six with ¹⁶O beam, four with ¹³C beam and three each for ¹²C and ²⁰Ne beams). Comparison of angular distributions with calculations using PACE4 code.

doi: 10.1103/PhysRevC.100.054604
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6374.

Note: The following list of authors and aliases matches the search parameter R.Singh: , R.J.SINGH, R.K.SINGH, R.M.SINGH, R.N.SINGH, R.P.SINGH