NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = B.Singh Found 411 matches. Showing 1 to 100. [Next]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
2024AS01 Nucl.Phys. A1041, 122786 (2024) M.S.Asnain, M.K.Sharma, Mohd.Shuaib, A.Siddique, I.Majeed Bhat, B.P.Singh, R.Prasad Investigating the influence of input angular momentum on independence hypothesis in heavy-ion induced fusion reactions NUCLEAR REACTIONS 159Tb(18O, X), 165Ho(12C, X), E=50-100 MeV; analyzed available data; deduced a channel wise analysis of σ data for evaporation residues within the framework of statistical model code PACE4.
doi: 10.1016/j.nuclphysa.2023.122786
2024PA11 Phys.Lett. B 848, 138379 (2024) Study of octupole deformations in Pb-Pb collisions at 5.02 TeV NUCLEAR REACTIONS 208Pb(208Pb, X), E=5.02 TeV; analyzed available data; deduced sensitivity of octupole deformation by employing Monte-Carlo HYDJET++ model.
doi: 10.1016/j.physletb.2023.138379
2024SI02 Nucl.Data Sheets 194, 3 (2024) Nuclear Structure and Decay Data for A=76 Isobars COMPILATION 76Fe, 76Co, 76Ni, 76Cu, 76Zn, 76Ga, 76Ge, 76As, 76Se, 76Br, 76Kr, 76Rb, 76Sr, 76Y; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2024.02.002
2024SI03 Nucl.Data Sheets 194, 460 (2024) Nuclear Structure and Decay Data for A=165 Isobars COMPILATION 165Pm, 165Sm, 165Eu, 165Gd, 165Tb, 165Dy, 165Ho, 165Er, 165Tm, 165Yb, 165Lu, 165Hf, 165Ta, 165W, 165Re, 165Os, 165Ir, 165Pt; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2024.02.003
2023CH33 Nucl.Data Sheets 190, 1 (2023) Nuclear Structure and Decay Data for A=44 Isobars COMPILATION 44Si, 44P, 44S, 44Cl, 44Ar, 44K, 44Ca, 44Sc, 44Ti, 44V, 44Cr, 44Mn; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2023.06.001
2023GA02 At.Data Nucl.Data Tables 150, 101546 (2023) S.Garg, B.Maheshwari, B.Singh, Y.Sun, A.Goel, A.K.Jain Atlas of nuclear isomers-Second edition COMPILATION Z=4-109; compiled, evaluated nuclear structure data, isomeric T1/2, J, π, decay modes.
doi: 10.1016/j.adt.2022.101546
2023KA03 Phys.Rev. C 107, 014613 (2023) S.Kaur, N.Kaur, R.Kaur, B.B.Singh, S.K.Patra Fusion enhancement within a collective clusterization approach applied to the isotopic chain of neutron-rich light-mass compound nuclei NUCLEAR REACTIONS 12C(12C, X)24Mg, 12C(13C, X)25Mg, 12C(14C, X)26Mg, 12C(15C, X)27Mg, E(cm)=10-15 MeV; calculated fusion σ, fragment mass distribution from Mg compound nucleus fragmentation, fragmentation potential, cluster preformation probability, scattering potential, variation of neck length parameter. Calculations in the framework of dynamical cluster decay model (DCM). Comparison to experimental data.
doi: 10.1103/PhysRevC.107.014613
2023KA25 Phys.Rev. C 108, 034611 (2023) R.Kaur, B.B.Singh, M.Kaur, M.K.Sharma, P.P.Singh Investigating 6, 7Li-induced reactions on 235, 238U through a collective clusterization approach
doi: 10.1103/PhysRevC.108.034611
2023PA03 Eur.Phys.J. A 59, 6 (2023) Transverse momentum spectra and suppression of charged hadrons in deformed Xe-Xe collisions at √ sNN = 5.44 TeV using HYDJET++ model
doi: 10.1140/epja/s10050-023-00916-w
2023SI02 Phys.Rev. C 107, 024906 (2023) A.Singh, P.K.Srivastava, G.Devi, B.K.Singh Production and enhancement of (multi-) strange hadrons in Au+Au collisions at √ sNN = 2000 GeV RHIC energy and Pb+Pb collisions at √ sNN = 2.76 TeV LHC energy
doi: 10.1103/PhysRevC.107.024906
2023SI06 Nucl.Data Sheets 188, 1 (2023) Nuclear Structure and Decay Data for A=71 Isobars COMPILATION 71Mn, 71Fe, 71Co, 71Ni, 71Cu, 71Zn, 71Ga, 71Ge, 71As, 71Se, 71Br, 71Kr; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2023.02.001
2023SI20 Nucl.Data Sheets 191, 1 (2023) Nuclear Structure and Decay Data for A=167 Isobars COMPILATION 167Sm, 167Eu, 167Gd, 167Tb, 167Dy, 167Ho, 167Er, 167Tm, 167Yb, 167Lu, 167Hf, 167Ta, 167W, 167Re, 167Os, 167Ir, 167Pt; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2023.08.001
2023SI22 Nucl.Data Sheets 192, 315 (2023) B.Singh, M.S.Basunia, J.Chen, P.Dimitriou, B.M.S.Amro, S.Basu, S.Das, A.Karmakar, M.J.Lazaric, S.R.Leblond, S.S.Nayak, C.Ngwetsheni, A.Rathi, P.S.Rawat, B.Rohila, V.Vallet Nuclear Structure and Decay Data for A=222 Isobars COMPILATION 222Po, 222At, 222Rn, 222Fr, 222Ra, 222Ac, 222Th, 222Pa, 222U, 222Np; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2023.10.002
2023TU02 At.Data Nucl.Data Tables 152, 101584 (2023) S.Turkat, X.Mougeot, B.Singh, K.Zuber Systematics of log ft values for β- and EC/β+ transitions NUCLEAR STRUCTURE A=1-254; analyzed available data; calculated log ft with the BetaShape code; deduced systematics for β transitions.
doi: 10.1016/j.adt.2023.101584
2023VI05 Phys.Rev. C 108, 064002 (2023) M.Viviani, S.Konig, A.Kievsky, L.E.Marcucci, B.Singh, O.Vazquez Doce Role of three-body dynamics in nucleon-deuteron correlation functions
doi: 10.1103/PhysRevC.108.064002
2023YA11 Phys.Rev. C 107, 044605 (2023) A.Yadav, G.Ram, M.S.Asnain, I.Majeed, M.Shuaib, V.R.Sharma, I.Bala, U.Gupta, S.Gupta, D.P.Singh, P.P.Singh, M.Sharma, R.Kumar, B.P.Singh, R.Prasad Understanding the low-energy incomplete fusion reactions NUCLEAR REACTIONS 159Tb(18O, 3n), (18O, 4n), (18O, 5n), (18O, 6n), (18O, 2nα), (18O, 5nα), (18O, 6nα), (18O, 5npα), E=82, 95, 97, 100 MeV; measured Eγ, Iγ; deduced σ(E), contributions of complete and incomplete fusion channels. Comparison to predictions done using the PACE4 code. Systematics of incomplete fusion with different projectiles - 12C, 13C, 14N, 16O, 18O, 19F, 20Ne. Activation technique experiment at the Inter-University Accelerator Centre (IUAC, New Delhi).
doi: 10.1103/PhysRevC.107.044605
2022AS01 Phys.Rev. C 105, 014609 (2022) M.S.Asnain, M.Shuaib, I.Majeed, M.K.Sharma, V.R.Sharma, A.Yadav, D.P.Singh, P.P.Singh, S.Kumar, R.Kumar, B.P.Singh, R.Prasad Systematic study of fusion suppression for tightly bound projectiles at above-barrier energies NUCLEAR REACTIONS 181Ta(14N, X), E=83.05, 85.17, 87.07 MeV; measured Eγ, Iγ, total complete fusion σ(E) by activation method, and off-line γ-ray spectroscopy at the Pelletron ion-beam facility of IUAC-New Delhi. Comparison with theoretical fusion cross section calculated by using the code CCFULL. 159Tb, 169Tm(12C, X), (13C, X), (16O, X), (19F, X), 175Lu(19F, X), 181Ta(14N, X), E(cm)=50-100 MeV; analyzed previous and present experimental data, and compared fusion σ(E) in different systems with strongly bound projectiles using universal fusion function (UFF) method; deduced suppression factors for various projectiles, breakup effects of strongly bound non-α-cluster projectile 14N on fusion cross section at energies above the Coulomb barrier.
doi: 10.1103/PhysRevC.105.014609
2022AS02 Phys.Rev. C 106, 064607 (2022) M.S.Asnain, Mohd.Shuaib, I.Majeed, M.K.Sharma, A.Yadav, D.P.Singh, P.P.Singh, R.Kumar, B.P.Singh, R.Prasad Decomposing the linear momentum transfer components in break-up fusion reactions: An experimental study of the 19F + 159Tb system NUCLEAR REACTIONS 159Tb(19F, X), (19F, 4n), (19F, 5n), (19F, 4np), (19F, 3nα), (19F, 4nα), (19F, 3npα), (19F, 3n2α), (19F, 2np2α), (19F, 4np2α), E=82.8, 94.3 MeV; measured reaction products, Eγ, Iγ; deduced total ranges of the residues in Al, complete fusion σ(E), fusion function, forward recoil range integrated σ(E), contribution of complete fusion and incomplete fusion components to the production of residues. Stack of Al foils was installed after the target to catch the forward recoiled residues, which later were measured with HPGe detector. Comparison with PACE4 calculation, coupled channels calculations performed with CCFULL and other experimental data. Beam from 15UD Pelletron accelerator facility at Inter University Accelerator Center (IUAC, India).
doi: 10.1103/PhysRevC.106.064607
2022CH37 Nucl.Data Sheets 184, 29 (2022) Nuclear Structure and Decay Data for A=31 Isobars COMPILATION 31F, 31Ne, 31Na, 31Mg, 31Al, 31P, 31S, 31Cl, 31Ar, 31K; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2022.08.002
2022KA06 Nucl.Phys. A1018, 122361 (2022) S.Kaur, R.Kaur, B.B.Singh, S.K.Patra Decay analysis of 24, 25Mg* compound nuclei NUCLEAR REACTIONS 12C(12C, X)24Mg, 12C(13C, X)25Mg, E not given; analyzed available data; deduced preformation probabilities, σ, level density parameters.
doi: 10.1016/j.nuclphysa.2021.122361
2022KU33 J.Phys.(London) G49, 105103 (2022) S.Kumar, P.K.Giri, R.Kumar, A.Yadav, R.Ali, S.Appannababu, A.Agarwal, S.Mukherjee, P.P.Singh, V.R.Sharma, B.P.Singh, S.Dutt Study of incomplete fusion reaction dynamics for the system 14N + 169Tm using the forward Recoil Range distribution technique NUCLEAR REACTIONS 169Tm(14N, X)169Os/179Re/176W/175W/178Re/177W/174W, E ∼ 5.9 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced yields, σ, forward recoil range distribution (FRRD) of evaporation residues (ERs). The general purpose scattering chamber (GPSC) facility at Inter-University Accelerator Centre (IUAC), New Delhi.
doi: 10.1088/1361-6471/ac894b
2022LI08 Phys.Rev. C 105, 024308 (2022) K.C.W.Li, P.Adsley, R.Neveling, P.Papka, F.D.Smit, E.Nikolskii, J.W.Brummer, L.M.Donaldson, M.Freer, M.N.Harakeh, F.Nemulodi, L.Pellegri, V.Pesudo, M.Wiedeking, E.Z.Buthelezi, V.Chudoba, S.V.Fortsch, P.Jones, M.Kamil, J.P.Mira, G.G.O'Neill, E.Sideras-Haddad, B.Singh, S.Siem, G.F.Steyn, J.A.Swartz, I.T.Usman, J.J.van Zyl Multiprobe study of excited states in 12C: Disentangling the sources of monopole strength between the energy of the Hoyle state and ex = 13 MeV NUCLEAR REACTIONS 12C(α, α'), E=118, 160, 196, 200; 14C(p, t), E=67.5, 100 MeV; measured reaction products, Eα, Iα, (particle)α-coin; deduced excitation energy spectra. 12C; deduced levels, J, π, resonances, resonance widths, monopole strength distribution. Discussed the nature of monopole strength excess at around 9 MeV as possible breathing-mode excitation of the Hoyle state. CAKE-array of double-sided silicon strip detectors coupled with K600 magnetic spectrometer at iThemba LABS.
doi: 10.1103/PhysRevC.105.024308
2022LI13 Phys.Lett. B 827, 136928 (2022) K.C.W.Li, F.D.Smit, P.Adsley, R.Neveling, P.Papka, E.Nikolskii, J.W.Brummer, L.M.Donaldson, M.Freer, M.N.Harakeh, F.Nemulodi, L.Pellegri, V.Pesudo, M.Wiedeking, E.Z.Buthelezi, V.Chudoba, S.V.Fortsch, P.Jones, M.Kamil, J.P.Mira, G.G.O'Neill, E.Sideras-Haddad, B.Singh, S.Siem, G.F.Steyn, J.A.Swartz, I.T.Usman, J.J.van Zyl Investigating the predicted breathing-mode excitation of the Hoyle state NUCLEAR REACTIONS 12C(α, α'), E=200 MeV; 14C(p, t)12C, E not given; measured reaction products. 12C; deduced experimentally observed inclusive yields, monopole resonance as the breathing-mode excitation of the Hoyle state. The K600 spectrometer at the iThemba Laboratory for Accelerator-Based Sciences (iThemba LABS) in South Africa.
doi: 10.1016/j.physletb.2022.136928
2022MA13 Nucl.Phys. A1021, 122421 (2022) I.Majeed Bhat, Mohd.S.M.S.Asnain, V.R.Sharma, A.Yadav, M.K.Sharma, P.P.Singh, D.P.Singh, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, R.Kumar, B.P.Singh, R.Prasad Effect of projectile structure on break-up fusion for 14N + 175Lu system at intermediate energies NUCLEAR REACTIONS 175Lu(14N, X)184Pt/185Pt/186Pt/183Ir/184Ir/185Ir/182Os/183Os/181Re/177W/178Ta, E=87.11 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with PACE4 predictions. The Inter University Accelerator, New Delhi, India.
doi: 10.1016/j.nuclphysa.2022.122421
2022MA25 Phys.Rev. C 105, 054607 (2022) I.Majeed Bhat, M.Shuaib, M.S.Asnain, M.K.Sharma, A.Yadav, V.R.Sharma, P.P.Singh, D.P.Singh, S.Gupta, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, S.Kumar, R.Kumar, B.P.Singh, R.Prasad Role of precursor nuclei in heavy-ion induced reactions at low energies NUCLEAR REACTIONS 175Lu(14N, 4np), E=79.68, 87.11 MeV; 159Tb(12C, 3np), E=69.15, 77.77 MeV; 159Tb(13C, 4np), E=77.87, 84.59 MeV; measured Eγ, Iγ; deduced σ(E). Separated yields of the isotope produced in the direct reaction from feeding caused by decay of the isotopes from other channels. Pelletron accelerator facility of the Inter-University Accelerator Centre(IUAC), New Delhi. comparison to theoretical estimations. RADIOACTIVITY 184Pt(β+), (EC) [from 175Lu(14N, 5n), E=79.68, 87.11 MeV]; 167Lu(EC) [from 159Tb(13C, 5n), E=77.87, 84.59 MeV; 159Tb(12C, 4n), E=69.15, 77.77 MeV]; measured Eγ, Iγ; deduced T1/2. Comparison to other experimental data.
doi: 10.1103/PhysRevC.105.054607
2022NI03 Nucl.Data Sheets 181, 1 (2022) Nuclear Data Sheets for A=147 COMPILATION 147I, 147Xe, 147Cs, 147Ba, 147La, 147Ce, 147Pr, 147Nd, 147Pm, 147Sm, 147Eu, 147Gd, 147Tb, 147Dy, 147Ho, 147Er, 147Tm; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2022.03.001
2022PR08 Nucl.Phys. A1027, 122511 (2022), Nucl.Phys. A1029, 122555 (2023) B.Pritychenko, B.Singh, M.Verpelli Systematic trends of 0+2, 1-1, 3-1and 2+1 excited states in even-even nuclei COMPILATION 4He, 12,16O, 44Ar, 36Ca, 40Ca, 68Ni, 72Ge, 72Kr, 90,96,98Zr, 98Mo, 180,182Hg, 184,186,188,190,192,194Pb, 14C, 14O, 146Gd, 208Pb; analyzed available data; deduced J, π, 2+ first excited state dominance in even-even nuclei.
doi: 10.1016/j.nuclphysa.2022.122511
2022SI28 Nucl.Data Sheets 185, 2 (2022) Nuclear Structure and Decay Data for A=149 Isobars COMPILATION 149Xe, 149Cs, 149Ba, 149La, 149Ce, 149Pr, 149Nd, 149Pm, 149Sm, 149Eu, 149Gd, 149Tb, 149Dy, 149Ho, 149Er, 149Tm, 149Yb; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2022.10.001
2022SI29 Nucl.Data Sheets 185, 560 (2022) Nuclear Structure and Decay Data for A=231 Isobars COMPILATION 231Rn, 231Fr, 231Ra, 231Ac, 231Th, 231Pa, 231U, 231Np, 231Pu; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2022.10.002
2022SM03 Nucl.Data Sheets 186, 1 (2022) M.Smith, C.Nesaraja, B.Singh, S.Basunia, L.Bernstein, R.Firestone, J.Tuli Murray J. Martin (1935-2022)
doi: 10.1016/j.nds.2022.11.001
2022TU05 Nucl.Data Sheets 185, 1 (2022) Edgardo (Eddie) Browne-Moreno (1939-2022)
doi: 10.1016/j.nds.2022.10.003
2021AS08 Phys.Rev. C 104, 034616 (2021) M.S.Asnain, M.Shuaib, I.Majeed, M.K.Sharma, V.R.Sharma, A.Yadav, D.P.Singh, P.P.Singh, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, S.Kumar, R.Kumar, B.P.Singh, R.Prasad Effect of non-α-cluster projectile on incomplete-fusion dynamics: Experimental study of the 14N + 181Ta NUCLEAR REACTIONS 181Ta(14N, 3n)192Hg, (14N, 4n)191Hg/191mHg, (14N, 5n)190Hg, (14N, 6n)189Hg/189mHg, (14N, 3np)191Au, (14N, 4np)190Au, (14N, 5np)189Au/189mAu, (14N, 2nα)189Pt, (14N, 4nα)187Pt, (14N, 5nα)186Pt, (14N, 3npα)187Ir, (14N, 4npα)186Ir/186mIr, (14N, 5npα)185Ir, (14N, 4n2α)183Os, (14N, 5np2α)181Re, E=65.53, 67.50, 69.47, 71.54, 73.65, 75.65, 77.08, 79.51, 81.42, 83.05, 85.17, 87.07 MeV; measured off-line Eγ, Iγ, σ(E) for radio-nuclides populated via complete fusion (CF) and/or incomplete fusion (ICF processes) by activation method at the ion-beam facility of the IUAC-New Delhi; deduced total fusion, total complete fusion, and total incomplete fusion σ(E). Comparison with statistical model calculations using PACE4 code. 190Hg; measured nominal half-life from γ-decay curves as an example for the purpose of correct identification of different radioactive nuclei produced through various reaction channels.
doi: 10.1103/PhysRevC.104.034616
2021CH50 Nucl.Data Sheets 177, 1 (2021) Nuclear Data Sheets for A=194 COMPILATION 194Ta, 194W, 194Re, 194Os, 194Ir, 194Pt, 194Au, 194Hg, 194Tl, 194Pb, 194Bi, 194Po, 194At, 194Rn; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2021.09.001
2021DI04 Nucl.Data Sheets 173, 144 (2021) P.Dimitriou, I.Dillmann, B.Singh, V.Piksaikin, K.P.Rykaczewski, J.L.Tain, A.Algora, K.Banerjee, I.N.Borzov, D.Cano-Ott, S.Chiba, M.Fallot, D.Foligno, R.Grzywacz, X.Huang, T.Marketin, F.Minato, G.Mukherjee, B.C.Rasco, A.Sonzogni, M.Verpelli, A.Egorov, M.Estienne, L.Giot, D.Gremyachkin, M.Madurga, E.A.McCutchan, E.Mendoza, K.V.Mitrofanov, M.Narbonne, P.Romojaro, A.Sanchez-Caballero, N.D.Scielzo Development of a Reference Database for Beta-Delayed Neutron Emission COMPILATION Z=2-87; compiled β-delayed neutron emission data; deduced total delayed neutron yields, time-dependent group parameters in 6- and 8-group representation, and aggregate delayed neutron spectra.
doi: 10.1016/j.nds.2021.04.006
2021KA24 Phys.Rev. C 103, 054608 (2021) Role of microscopic temperature-dependent binding energies in the decay of 32Si* formed in the 20O + 12C reaction NUCLEAR REACTIONS 12C(20O, X)32Si*, E(cm)=7.35, 9.29 MeV; calculated fragmentation potential, mass dependence of fragmentation potential, macroscopic and microscopic binding energies for some isobars of A=10, 14, 18, 22, 26 and 30 at T=0 and 3.09 MeV, preformation probability potentials for the emission of 3H, 4He and 5He, fusion cross-sections for light-charged particles. Relativistic mean-field (RMF) calculations using quantum mechanical fragmentation-based dynamical cluster-decay model (DCM), and Davidson mass formula.
doi: 10.1103/PhysRevC.103.054608
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
2021OJ01 Phys.Rev. C 104, 034615 (2021) A.Ojha, S.Gupta, U.Gupta, P.P.Singh, A.Yadav, D.P.Singh, M.Shuaib, B.P.Singh, R.Prasad Mass-number dependence of statistical model parameters and its impact on incomplete fusion fraction calculations NUCLEAR REACTIONS 181Ta(16O, 3n)194Tl, (16O, 4n)193Tl, (16O, 5n)192Tl, (16O, 3np)193Hg, (16O, 4np)192Hg, (16O, 5np)191Hg, E=75-105 MeV; 165Ho(12C, 3n)174Ta, (12C, 4n)173Ta, (12C, 5n)172Ta, (12C, 3np)173Hf, E=55-85 MeV; 163Dy(14N, 3n)174Ta, (14N, 4n)173Ta, (14N, 5n)172Ta, E=65-85 MeV; 74Ge(16O, 4n)86Zr, (16O, 2np)87Y, (16O, 3np)86Y, (16O, 4np)85Y, E=50-110 MeV; calculated σ(E) using statistical model based PACE4 code, with optical model potential (OMP) parameters, summed σ(E) using different sets of OMP parameters and impact on incomplete fusion (ICF) fraction, and effect of deformation parameter β2 on incomplete fusion. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.034615
2021PA05 Phys.Rev. C 103, 014903 (2021) S.Pandey, S.K.Tiwari, B.K.Singh Pseudorapidity density, transverse momentum spectra, and elliptic flow studies in Xe-Xe collision systems at √ sNN = 5.44 TeV using the HYDJET + + model NUCLEAR REACTIONS 129Xe(129Xe, X), E(cm)=5.44 TeV, calculated pseudorapidity density distributions of all charged particles, transverse momentum spectra and elliptic flow, centrality dependence, geometry of the colliding systems, and geometrical configuration of the collisions using HYDJET++ and AMPT models. Comparison with experimental data from ALICE and CMS Collaborations.
doi: 10.1103/PhysRevC.103.014903
2021SH30 Phys.Rev. C 104, L031601 (2021) M.Sharma, M.Sarswat, S.Arora, S.Kumar, M.Shuaib, I.Majeed, M.S.Asnain, B.P.Singh, R.Prasad, V.R.Sharma, A.Yadav, P.P.Singh, D.P.Singh New experimental approach for developing a mass-energy systematics for precompound emission NUCLEAR REACTIONS 63,65Cu(α, n), E=5-50 MeV; analyzed experimental σ(E) with theoretical calculations using Monte Carlo statistical code PACE4. 63,65Cu, 69,71Ga, 85Rb, 89Y, 93Nb, 103Rh, 107,109Ag(α, n), E(cm)=22-40 MeV; calculated fraction of pre-compound emission as functions of center-of-mass energy, excitation energy and excess energy; deduced mass-energy systematics in pre-compound emission reactions.
doi: 10.1103/PhysRevC.104.L031601
2021SI08 Nucl.Data Sheets 172, 1 (2021) Nuclear Data Sheets for A=100 COMPILATION 100Kr, 100Rb, 100Sr, 100Y, 100Zr, 100Nb, 100Mo, 100Tc, 100Ru, 100Rh, 100Pd, 100Ag, 100Cd, 100In, 100Sn; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2021.02.001
2021SI21 Nucl.Data Sheets 175, 150 (2021) B.Singh, G.Mukherjee, S.K.Basu, S.Bhattacharya, S.Bhattacharya, A.Chakraborti, A.K.De, R.Gowrishankar, A.K.Jain, S.Kumar, S.Singh Nuclear Data Sheets for A=219 COMPILATION 219Pb, 219Bi, 219Po, 219At, 219Rn, 219Fr, 219Ra, 219Ac, 219Th, 219Pa, 219U, 219Np; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2021.06.002
2021SI35 Nucl.Data Sheets 178, 41 (2021) Nuclear Data Sheets for A=64 COMPILATION 64Ti, 64V, 64Cr, 64Mn, 64Fe, 64Co, 64Ni, 64Cu, 64Zn, 64Ga, 64Ge, 64As, 64Se; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2021.11.002
2021SO23 J.Phys.(London) G48, 025105 (2021) A.Sood, S.Thakur, A.Sharma, V.R.Sharma, A.Yadav, M.K.Sharma, B.P.Singh, R.Kumar, R.K.Bhowmik, P.P.Singh Disentangling complete and incomplete fusion events in 12C + 169Tm reaction by spin-distribution measurements NUCLEAR REACTIONS 169Tm(12C, X), E=6.7, 7.5 MeV/nucleon; measured reaction products, Eα, Iα, Eγ, Iγ. 176Re, 174Ta, 171Lu; deduced yields, strong entrance-channel dependence of incomplete fusion dynamics.
doi: 10.1088/1361-6471/abc14a
2020CH10 Nucl.Data Sheets 164, 1 (2020) Nuclear Data Sheets for A=98 COMPILATION 98Br, 98Kr, 98Rb, 98Sr, 98Y, 98Zr, 98Nb, 98Mo, 98Tc, 98Ru, 98Rh, 98Pd, 98Ag, 98Cd, 98In; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2020.01.001
2020GA06 Acta Phys.Pol. B51, 799 (2020) P.E.Garrett, L.Makhathini, R.A.Bark, T.r.rodriguez, S.Valbuena, V.Bildstein, T.D.Bucher, C.Burbadge, R.Dubey, T.Faestermann, R.Hertenberger, M.Kamil, E.A.Lawrie, K.G.Leach, A.D.MacLean, C.Malotana, C.Mehl, S.H.Mthembu, J.Mukwevho, C.Ngwetsheni, S.S.Ntshangase, J.Ondze, J.N.Orce, B.Rebeiro, B.Singh, S.Triambak, E.C.Vyfers, H-F.Wirth Shape Coexistence in the Ru Isotopes; Multi-spectroscopic Study of 98Ru and Beyond-mean-field Calculations
doi: 10.5506/APhysPolB.51.799
2020GA26 Phys.Lett. B 809, 135762 (2020) P.E.Garrett, L.Makhathini, R.A.Bark, T.R.Rodriguez, S.Valbuena, V.Bildstein, T.D.Bucher, C.Burbadge, R.Dubey, T.Faestermann, R.Hertenberger, M.Kamil, E.A.Lawrie, K.G.Leach, A.D.MacLean, C.Mehl, S.H.Mthembu, N.J.Mukwevho, C.Ngwetsheni, S.S.Ntshangase, J.C.Nzobadila Ondze, J.N.Orce, B.Rebeiro, B.Singh, S.Triambak, E.C.Vyfers, H.-F.Wirth Observation of the 0+2 and γ bands in 98Ru, and shape coexistence in the Ru isotopes RADIOACTIVITY 98Rh(β+), (EC) [from 89Y(12C, 3n), E=47.5 MeV]; measured decay products, Eγ, Iγ; deduced γ-ray energies and intensities, branching, σ(θ), J, π, bands. Comparison with theoretical calculations.
doi: 10.1016/j.physletb.2020.135762
2020KA20 Phys.Rev. C 101, 034614 (2020) R.Kaur, S.Kaur, B.B.Singh, B.S.Sandhu, S.K.Patra Clustering effects in the exit channels of 13, 12C + 12C reactions within the collective clusterization mechanism of the dynamical cluster decay model NUCLEAR REACTIONS 12C(12C, X)24Mg*, (12C, 6Li), (12C, 7Li), (12C, 7Be), (12C, 8Be), (12C, 9Be), (12C, X)25Mg*, (13C, 6Li), (13C, 7Li), (13C, 7Be), (13C, 8Be), (13C, 9Be), E*=53.9 MeV; calculated fragmentation potential, fragment preformation probability, l-summed preformation probability, scattering potential, barrier potential, penetration probability, and σ(25Mg*)/σ(24Mg*). Dynamical cluster decay model (DCM). Comparison with experimental data, and with other theoretical predictions. Discussed role of α-clustering in heavy-ion reactions.
doi: 10.1103/PhysRevC.101.034614
2020KA26 Phys.Rev. C 101, 044605 (2020) R.Kaur, M.Kaur, V.Singh, M.Kaur, B.B.Singh, B.S.Sandhu Dynamical aspects od 48Ti + 58Fe, 58Ni → 106Cd*, 106Sn reactions at energies near the Coulomb barrier NUCLEAR REACTIONS 58Fe(48Ti, X)106Cd*,58Ni(48Ti, X)106Sn*, E=118.06-165.8 MeV; calculated fragmentation and scattering potentials, barrier lowering and neck-length parameters, preformation probabilities, σ(E) as function of light and heavy fragments of the compound nuclei. Dynamical cluster decay model (DCM).
doi: 10.1103/PhysRevC.101.044605
2020KR03 At.Data Nucl.Data Tables 133-134, 101336 (2020) Compilation of recent atomic mass measurements and deduced quantities COMPILATION Z=5-102; compiled atomic mass measurements; deduced β- and α-decay Q-values, one- and two-nucleon separation energies using the newly measured mass excesses.
doi: 10.1016/j.adt.2020.101336
2020LI32 Nucl.Data Sheets 168, 1 (2020) J.Liang, B.Singh, E.A.McCutchan, I.Dillmann, M.Birch, A.A.Sonzogni, X.Huang, M.Kang, J.Wang, G.Mukherjee, K.Banerjee, D.Abriola, A.Algora, A.A.Chen, T.D.Johnson, K.Miernik Compilation and Evaluation of Beta-Delayed Neutron Emission Probabilities and Half-Lives for Z > 28 Precursors RADIOACTIVITY 73,74,75,76,77,78,79,80,81,82,83Cu, 78,79,80,81,82,83,84,85Zn, 79,80,81,82,83,84,85,86,87Ga, 83,84,85,86,87,88,89,90Ge, 84,85,86,87,88,89,90,91,92As, 86,87,88,89,90,91,92,93,94,95Se, 87,88,89,90,91,92,93,94,95,96,97,98Br, 91,92,93,94,95,96,97,98,99,100,101Kr, 91,92,93,94,95,96,97,98,99,100,101,102,103,104Rb, 96,97,98,99,100,101,102,103,104,105,106,107Sr, 97,98,99,100,101,102,103,104,105,106,107,108,109Y, 103,104,105,106,107,108,109,110,111,112,113Zr, 103,104,105,106,107,108,109,110,111,112,113,114,115,116Nb, 109,110,111,112,113,114,115,116,117,118,119Mo, 109,110,111,112,113,114,115,116,117,118,119,120,121,122Tc, 114,115,116,117,118,119,120,121,122,123,124,125Ru, 115,116,117,118,119,120,121,122,123,124,125,126,127,128Rh, 119,120,121,122,123,124,125,126,127,128,129,130,131Pd, 120,121,122,123,124,125,126,127,128,129,130,131,132Ag, 126,127,128,129,130,131,132,133,134Cd, 127,128,129,130,131,132,133,134,135,136,137In, 133,134,135,136,137,138,139,140Sn, 134,135,136,137,138,139,140,141,142Sb, 136,137,138,139,140,141,142,143,144,145Te, 137,138,139,140,141,142,143,144,145,146,147I, 141,142,143,144,145,146,147,148,149,150Xe, 141,142,143,144,145,146,147,148,149,150,151,152Cs, 147,148,149,150,151,152,153,154Ba, 147,148,149,150,151,152,153,154,155,156,157La, 153,154,155,156,157,158Ce, 153,154,155,156,157,158,159,160,161Pr, 158,159,160,161,162,163Nd, 159,160,161,162,163,164,165Pm, 163,164,165,166,167Sm, 165,166,167,168,169Eu, 169,170,171Gd, 169,170,171,172,173,174Tb, 174,175,176Dy, 174,175,176,177,178Ho, 180Er, 179,180,181Tm, 185Yb, 186,187,188Lu, 191,192,193,194Ta, 198,199Re, 203Os, 203,204,205Ir, 206,207,208Pt, 206,207,208,209,210Au, 209,210,211,212,213,214,215,216Hg, 210,211,212,213,214,215,216,217Tl, 219,220,221,222,223,224Bi, 225,226,227,228,229At, 223Fr(β-); analyzed available data; deduced β-delayed neutron emission probabilities (Pn) and T1/2 for known or potential β-delayed neutron precursors. Comparison with systematics using three different approaches.
doi: 10.1016/j.nds.2020.09.001
2020SH29 Eur.Phys.J. A 56, 247 (2020) M.K.Sharma, M.Kumar, M.Shuaib, I.Majeed, M.S.Asnain, V.R.Sharma, A.Yadav, P.P.Singh, D.P.Singh, B.P.Singh, R.Prasad A systematic experimental study of pre-compound emission in α-particle induced reactions on odd mass nuclei A = 103-123 NUCLEAR REACTIONS 103Rh, 107,109Ag, 113,115In, 121,123Sb(α, n), E not given; analyzed available data; deduced systematics on the pre-compound emission process using EXFOR library data.
doi: 10.1140/epja/s10050-020-00238-1
2020SI16 Nucl.Data Sheets 167, 1 (2020) S.Singh, S.Kumar, B.Singh, A.K.Jain Nuclear radius parameters (r0) for even-even nuclei from alpha decay RADIOACTIVITY 106,108Te, 108,110,112Xe, 114Ba, 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,164,156Er, 154,156,158Yb, 156,158,160,162,174Hf, 158,160,162,164,166,168W, 162,164,166,168,170,172,174,186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190W, 170,172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194,210Pb, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230,232Th, 216,218,222,224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260Sg, 264,266,268,270Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og(α); analyzed available data decay data for 186 even-even alpha emitters; deduced nuclear radius parameters (r0) for the daughternuclides using ALPHAD code.
doi: 10.1016/j.nds.2020.07.001
2020SI26 Nucl.Data Sheets 169, 1 (2020) Nuclear Data Sheets for A=190 COMPILATION 190Hf, 190Ta, 190W, 190Re, 190Os, 190Ir, 190Pt, 190Au, 190Hg, 190Tl, 190Pb, 190Bi, 190Po; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2020.10.001
2020SI28 Nucl.Data Sheets 170, 499 (2020) Nuclear Data Sheets for A=233 COMPILATION 233Fr, 233Ra, 233Ac, 233Th, 233Pa, 233U, 233Np, 233Pu, 233Am, 233Cm, 233Bk; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2020.11.002
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
2019CH23 Nucl.Data Sheets 157, 1 (2019) Nuclear Data Sheets for A=50 COMPILATION 50Cl, 50Ar, 50K, 50Ca, 50Sc, 50Ti, 50V, 50Cr, 50Mn, 50Fe, 50Co, 50Ni; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2019.04.001
2019KA05 Phys.Rev. C 99, 014614 (2019) M.Kaur, B.B.Singh, S.Kaur, R.K.Gupta N/Z dependence of decay channels in A=80 compound nuclei NUCLEAR REACTIONS 40Ca(40Ca, X)80Zr*, E(cm)=62.14 MeV; 64Zn(16O, X)80Sr*, E(cm)=48.0 MeV; 48Ca(32S, X)80Kr*, E(cm)=39.8 MeV; calculated radial scattering potential profiles, fragmentation potential, preformation and penetration probability probabilities as function of fragment mass and angular momentum, fusion σ for emission of light particles, intermediate mass fragments, and symmetric mass fragments. Dynamical cluster-decay model. Comparison with experimental values of fusion σ.
doi: 10.1103/PhysRevC.99.014614
2019KA27 Phys.Rev. C 100, 014002 (2019) Density-dependent NN interaction from subleading chiral three-nucleon forces: Long-range terms
doi: 10.1103/PhysRevC.100.014002
2019SA15 Nucl.Phys. A983, 145 (2019) R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, V.R.Sharma, A.Yadav, P.P.Singh, M.K.Sharma, R.Kumar, B.P.Singh, S.Aydin, R.Prasad Insights into the low energy incomplete fusion NUCLEAR REACTIONS 169Tm(12C, x), E(cm)=52.98 - 89.25 MeV; measured Eγ, Iγ(t); deduced production σ of evaporation residues. 169Tm(12C, x), E=52.98 - 89.25 MeV;160Gd(12C, x), Ei(cm)=83.7 MeV;103Rh(16O, x), 159Tb(16O, x), E not given; calculated ER production σ using PACE4 and with different level density parameters and using CCFULL; deduced potential parameters, radius parameter from the fit to the data, variation of incomplete fusion fraction with neutron skin thickness and with angular momentum.
doi: 10.1016/j.nuclphysa.2018.12.013
2019SA17 Phys.Rev. C 99, 024607 (2019) R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, A.Sharma, S.Thakur, P.P.Singh, P.K.Raina, M.M.Shaikh, R.Biswas, A.Yadav, J.Gehlot, S.Nath, N.Madhavan, V.Srivastava, M.K.Sharma, B.P.Singh, R.Prasad, A.Rani, A.Banerjee, U.Gupta, N.K.Deb, B.J.Roy Sub-barrier fusion in the 37Cl + 130Te system NUCLEAR REACTIONS 130Te(37Cl, X), E=121-155 MeV; measured reaction products, evaporation residues, time of flight of evaporation residue, fusion σ(E) using the HIRA recoil mass spectrometer at the 15UD Pelletron accelerator of IUAC-New Delhi; deduced fusion barrier distributions, astrophysical S factor, logarithmic derivative L(E) factor. Comparison with coupled-channels code calculations using CCFULL code. Systematics of reduced fusion excitation functions of 37Cl projectiles on 58,60,62,64Ni, 130Te targets at sub-barrier energies.
doi: 10.1103/PhysRevC.99.024607
2019SH02 Phys.Rev. C 99, 014608 (2019) M.K.Sharma, M.M.Musthafa, M.Shuaib, M.Kumar, V.R.Sharma, A.Yadav, P.P.Singh, B.P.Singh, R.Prasad Semiclassical and quantum mechanical analysis of α-particle-induced reactions on praseodymium: A study relevant to precompound emission NUCLEAR REACTIONS 141Pr(α, n), (α, 2n), E=14.2-40.0 MeV; measured Eγ, Iγ of offline irradiated sample, excitation functions, σ(E) at VECC-Kolkata cyclotron facility; deduced role of precompound emission. Comparison with previous experimental values, and theoretical predictions based on semiclassical model codes: PACE4, TALYS-1.9, ACT, and ALICE91, and the quantum mechanical model code EXIFON. 141Pr, 159Tb, 181Ta, 197Au, 203Tl(α, n), E=17-32 MeV; systematics of precompound fraction.
doi: 10.1103/PhysRevC.99.014608
2019SH09 Phys.Rev. C 99, 024617 (2019) M.Shuaib, V.R.Sharma, A.Yadav, S.Thakur, M.K.Sharma, I.Majeed, M.Kumar, P.P.Singh, D.P.Singh, R.Kumar, R.P.Singh, S.Muralithar, B.P.Singh, R.Prasad Mass and isotopic yield distributions of fission-like events in the 19F + 169Tm system at low energies NUCLEAR REACTIONS 169Tm(19F, X)67Ge/75Br/80Sr/84mRb/101Mo/107In/108In/109In/110mIn/115Sb/120Xe/125Cs/126Ba/128Xe/130Sb/131Te/134Nd/135Nd/137Nd/139Nd/140Sm/156Ho, E=92, 102.5, 105.4 MeV; measured Eγ, Iγ, σ(E) by activation method at IUAC, New Delhi; deduced isotopic yield distributions and fractional independent yield for In and Nd isotopes, mass variance and distribution of fission-like events and heavy residues, isobaric charge dispersion parameter and compared with theoretical calculations, and grazing angular momentum. Systematics of isotopic yield distribution variance in 169Tm(19F, X), (12C, X), 159Tb, 169Tm, 181Ta(16O, X), 232Th(7Li, X), (11B, X), 238U(11B, X), (22Ne, X), 208Pb(22Ne, X) systems.
doi: 10.1103/PhysRevC.99.024617
2019SH17 Phys.Rev. C 99, 034617 (2019) V.R.Sharma, R.Kumar, S.Mukherjee, E.F.Aguilera, M.Shuaib, P.P.Singh, A.Yadav, R.Dubey, S.Appannababu, J.C.Morales-Rivera, S.Kumar, B.P.Singh, R.Prasad Fissionlike events in the 14N + 181Ta system NUCLEAR REACTIONS 181Ta(14N, X)65Ga/72Ga/66Ge/67Ge/69mZn/71mZn/72Zn/70As/76Kr/79Kr/83Se/95Ru/105Rh/106mRh/106In/108In/109In/110In/130Sb/132Ce/133mCe/135I, E=72.9, 76.8, 79.18, 82.2 MeV; measured Eγ, Iγ, σ(E) using offline γ detection at the 15UD pelletron accelerator of IUAC, New Delhi; deduced isotopic yield distribution for In isotopes, mass distribution of fission products, and mass variance as a function of excitation energy for 195Hg. 65Ga; measured half-life for its decay. Comparison of measured σ with theoretical calculations using PACE code, and with previously measured isotopic yield distributions in the following fissioning systems: 159Tb, 169Tm, 181Ta(16O, X), E=57.1, 61.06, 67.04 MeV, 232,233Th(7Li, X), E=41.7 MeV, 232Th, 238U(11B, X), E=55.7, 67.4 MeV, 238U(22Ne, X), E=54.5 MeV, and 208Pb(20Ne, X), E=46.4 MeV.
doi: 10.1103/PhysRevC.99.034617
2019SI11 Nucl.Data Sheets 156, 1 (2019) Nuclear Data Sheets for A=254 COMPILATION 254U, 254Cf, 254Es, 254Fm, 254Md, 254No, 254Lr, 254Rf; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2019.02.003
2019SI12 Nucl.Data Sheets 156, 70 (2019) Nuclear Data Sheets for A=266, 270, 274, 278, 282, 286, 290, 294, 298 COMPILATION 266Db, 266Sg, 266Bh, 266Hs, 266Mt, 270Db, 270Bh, 270Hs, 270Mt, 270Ds, 274Bh, 274Mt, 274Rg, 278Mt, 278Rg, 278Nh; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2019.02.004
2019SI13 Nucl.Data Sheets 156, 148 (2019) Nuclear Data Sheets for A=268, 272, 276, 280, 284, 288, 292 COMPILATION 268Db, 268Hs, 268Mt, 272Bh, 272Rg, 276Mt, 280Rg, 284Cn, 284Nh, 284Fl, 288Fl, 288Mc, 292Lv, 296Rg, 300Mc; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2019.02.005
2019SI18 Appl.Radiat.Isot. 148, 126 (2019) B.Singh, S.Prajapati, B.K.Singh, R.Shanker Angular and impact energy dependence of intensity ratio of Kα, β x-rays to underneath bremsstrahlung radiation emitted from 15 to 25 keV electrons incident on a pure thick Cu (Z=29) target NUCLEAR REACTIONS Cu(E, E'), E=15-25 keV; measured reaction products, X-rays; deduced X-ray energies and intensities. Comparison with theoretical calculations.
doi: 10.1016/j.apradiso.2019.03.022
2019SI24 Nucl.Data Sheets 158, 1 (2019) Nuclear Data Sheets for A = 73 COMPILATION 73Mn, 73Fe, 73Co, 73Ni, 73Cu, 73Zn, 73Ga, 73Ge, 73As, 73Se, 73Br, 73Kr, 73Rb, 73Sr; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2019.02.006
2019SI39 Nucl.Data Sheets 160, 405 (2019) B.Singh, M.S.Basunia, M.Martin, E.A.McCutchan, I.Bala, R.Caballero-Folch, R.Canavan, R.Chakrabarti, A.Chekhovska, M.M.Grinder, S.Kaim, D.Kanjilal, D.Kasperovych, M.J.Kobra, H.Koura, S.Nandi, A.Olacel, A.Singh, B.P.E.Tee Nuclear Data Sheets for A=218 COMPILATION 218Pb, 218Bi, 218Po, 218At, 218Rn, 218Fr, 218Ra, 218Ac, 218Th, 218Pa, 218U; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2019.100524
2019SO21 Acta Phys.Pol. B50, 291 (2019) A.Sood, P.Kumar, R.N.Sahoo, P.P.Singh, A.Yadav, V.R.Sharma, M.K.Sharma, D.P.Singh, U.Gupta, S.Aydin, R.Kumar, B.P.Singh, R.Prasad Entrance Channel Effects on Fission Fragment Mass Distribution in 12C + 169Tm System NUCLEAR REACTIONS 169Tm(12C, X), E= 77.18, 83.22, 89.25 MeV; measured Eγ, Iγ(t); deduced production σ of evaporation residues, isotopic yieldsmass distribution of fission fragments.
doi: 10.5506/aphyspolb.50.291
2019SR03 Eur.Phys.J. A 55, 69 (2019) P.K.Srivastava, A.Singh, O.S.K.Chaturvedi, P.K.Raina, B.K.Singh Transverse momentum distribution of charged hadrons based on wounded quark mode
doi: 10.1140/epja/i2019-12741-3
2018CH16 Eur.Phys.J. A 54, 46 (2018) O.S.K.Chaturvedi, P.K.Srivastava, A.Singh, B.K.Singh Universal freezeout condition for charged hadrons in a hybrid approach
doi: 10.1140/epja/i2018-12488-3
2018KA02 Nucl.Phys. A969, 14 (2018) M.Kaur, B.B.Singh, M.K.Sharma, R.K.Gupta Analysis of intermediate and light mass fragments from composite systems 26-29Al* formed in 16, 18O + 10, 11B reactions NUCLEAR REACTIONS 10,11B(16O, x), (18O, x), E=1-4 MeV/nucleon; calculated fragmentation potential for the composite system, fragment mass distribution, fragment preformation probability using DCM (Dynamical Cluster decay Model) for both spherical and deformed nucleus. Light particle emission σ compared to data.
doi: 10.1016/j.nuclphysa.2017.09.014
2018KA43 Nucl.Phys. A980, 67 (2018) M.Kaur, B.B.Singh, M.K.Sharma, R.K.Gupta Study of α-induced reactions forming A=60 compound systems within dynamical cluster-decay model
doi: 10.1016/j.nuclphysa.2018.09.079
2018KA53 Phys.Rev. C 98, 064612 (2018) R.Kaur, M.Kaur, V.Singh, S.Kaur, B.B.Singh, B.S.Sandhu Investigating the fusion enhancement for neutron-rich mid-mass nuclei using the dynamical cluster-decay model NUCLEAR REACTIONS 28Si(39K, X)67As*,28Si(40K, X)68As*,28Si(41K, X)69As*,28Si(45K, X)73As*,28Si(46K, X)74As*,28Si(47K, X)75As*, E(cm)=36.8-42.6 MeV; calculated fragment potentials and l-summed preformation probability as a function of fragment mass number, scattering potentials for the compound nuclei decaying through one-proton and one-neutron channels, barrier lowering as function of incident energy, summed penetration probabilities, fusion σ(E), -summed fragment cross sections using dynamical cluster-decay model (DCM). Comparison with available experimental data.
doi: 10.1103/PhysRevC.98.064612
2018KO01 Nucl.Data Sheets 147, 382 (2018) F.G.Kondev, E.A.McCutchan, B.Singh, K.Banerjee, S.Bhattacharya, A.Chakraborty, S.Garg, N.Jovancevic, S.Kumar, S.K.Rathi, T.Roy, J.Lee, R.Shearman Nuclear Data Sheets for A=217 COMPILATION 217Tl, 217Pb, 217Bi, 217Po, 217At, 217Rn, 217Fr, 217Ra, 217Ac, 217Th, 217Pa, 217U; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2018.01.002
2018SA38 Acta Phys.Pol. B49, 585 (2018) R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, V.R.Sharma, A.Yadav, M.Shuaib, D.P.Singh, P.P.Singh, U.Gupta, M.K.Sharma, R.Kumar, B.P.Singh, S.Aydin, H.J.Wollersheim, R.Prasad Entrance Channel Effect on Incomplete Fusion NUCLEAR REACTIONS 169Tm(12C, x), E=5-7.5 MeV/nucleon; measured evaporation residues (ER) Eγ, Iγ(time); deduced 177Re σER; calculated σER using statistical model code PACE-IV with different level density parameter; calculated total (summed over all ERs) σT, complete and incomplete fusion σCF, σICF. 103Rh, 115In, 159Tb, 169Tm, 197Au(12C, x), E not given;103Rh, 159Tb, 169Tm(16O, x), E not given; measured reaction products Eγ, Iγ; deduced incomplete fusion fraction vs mass asymmetry (relative projectile-target velocity close to 0.05c vs asymmetry).
doi: 10.5506/aphyspolb.49.585
2018SH25 Phys.Rev. C 98, 014605 (2018) M.Shuaib, 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 Effects of projectile break-up on fusion cross sections at energies near and above the Coulomb barrier: A case of incomplete fusion NUCLEAR REACTIONS 175Lu(19F, 4n), (19F, 5n), (19F, 6n), (19F, 3np), (19F, 4np), (19F, 5np), (19F, nα), (19F, 2nα), (19F, 3nα), (19F, 4nα), (19F, 2npα), (19F, 3npα), (19F, 4npα), (19F, 3n2α), (19F, 4n2α), (19F, 4np2α), E=82-112 MeV; measured Eγ, Iγ, σ(E) of evaporation residues populated via complete fusion (CF) and/or incomplete fusion (ICF) processes using offline γ-activation method at the Inter University Accelerator Centre (IUAC-New Delhi). Comparison with statistical model calculations using PACE4 model.
doi: 10.1103/PhysRevC.98.014605
2018SH38 Phys.Rev. C 98, 054607 (2018) M.K.Sharma, M.Kumar, Mohd.Shuaib, V.R.Sharma, A.Yadav, P.P.Singh, B.P.Singh, R.Prasad Systematic study of precompound neutron emission in α-particle-induced reactions NUCLEAR REACTIONS 141Pr(α, n), E=10-40 MeV; measured Eγ, Iγ offline, σ(E) at VECC-Kolkata facility. 51V(α, n), E=5-35 MeV; 55Mn(α, n), E=5-25 MeV; 93Nb(α, n), E=10-40 MeV; 121Sn(α, n), E=6-60 MeV; 123Sb(α, n), E=10-40 MeV; 141Pr(α, n), E=10-40 MeV; analyzed σ(E) data; deduced precompound nucleus (PCN) fraction for one neutron channels. Comparison with predictions using ALICE code.
doi: 10.1103/PhysRevC.98.054607
2018SH39 Eur.Phys.J. A 54, 205 (2018) M.K.Sharma, M.Kumar, M.Shuaib, V.R.Sharma, A.Yadav, Pushpendra P.Singh, D.P.Singh, B.P.Singh, R.Prasad Analysis of experimental cross-section for (α, n) reactions in odd A and odd Z heavy nuclei: A systematics on pre-compound emission COMPILATION 139La, 159Tb, 181Ta, 197Au, 203Tl(α, n), E=cyclotron; compiled σ; calculated σ, pre-equilibrium fraction using PACE4 (compound nucleus only) and ALICE (includes pre-equilibrium) with varied parameters; deduced parameters influence on the cross sections.
doi: 10.1140/epja/i2018-12634-y
2018SI01 Nucl.Data Sheets 147, 1 (2018) Nuclear Data Sheets for A=164 COMPILATION 164Sm, 164Eu, 164Gd, 164Tb, 164Dy, 164Ho, 164Er, 164Tm, 164Yb, 164Lu, 164Hf, 164Ta, 164W, 164Re, 164Os, 164Ir; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2018.01.001
2017AL39 Nucl.Phys. A968, 403 (2017) R.Ali, M.Afzal Ansari, D.Singh, R.Kumar, D.P.Singh, M.K.Sharma, U.Gupta, B.P.Singh, P.D.Shidling, D.Negi, S.Muralithar, R.P.Singh, R.K.Bhowmik Observed side feeding in incomplete fusion dynamics in 16O + 160Gd reaction at energy ∼ 5.6 MeV/A: Spin distribution measurements NUCLEAR REACTIONS 160Gd(16O, x), E≈5.6 MeV/nucleon; measured Eγ, Iγ(θ), Ep, Ip(θ), Eα, Iα(θ), pγ-coin, αγ-coin using GDA (Gamma Detector Array) consisting of 12 n-type Compton suppressed HPGE working together with CPDA (Charged Particle Detector Array); deduced relative spin distributions (relative yields vs spin) of different reaction channels, evaporation residues yrast bands side feeding intensities, mean input angular momentum for different reaction channels.
doi: 10.1016/j.nuclphysa.2017.09.005
2017JO05 Nucl.Data Sheets 142, 1 (2017) Nuclear Data Sheets for A=189 COMPILATION 189Hf, 189Ta, 189W, 189Re, 189Os, 189Ir, 189Pt, 189Au, 189Hg, 189Tl, 189Pb, 189Bi, 189Po; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2017.04.001
2017KA05 Phys.Rev. C 95, 014611 (2017) M.Kaur, B.B.Singh, S.K.Patra, R.K.Gupta Clustering effects and decay analysis of the light-mass N=Z and N ≠ Z composite systems formed in heavy ion collisions NUCLEAR REACTIONS 10B(10B, X)20Ne*, E(cm)=12-25 MeV; 16O(12C, X)28Si*, E(cm)=50.14-68.57 MeV; 28Si(12C, X)40Ca*, E(cm)=53.90 MeV; 10B(11B, X)21Ne*, E(cm)=13.09-26.19 MeV; 11B(11B, X)22Ne*, E(cm)=12-25 MeV; 11B(28Si, X)39K*, E(cm)=45.94 MeV; 12C(27Al, X)39K*, E(cm)=50.53 MeV; calculated preformation and penetration probabilities as function of fragment or cluster mass, scattering and fragment potentials for the decay of α- and non-α conjugate systems, fission-fusion σ(E). Dynamical cluster-decay model (DCM) based on quantum-mechanical fragmentation theory (QMFT). Comparison with experimental data.
doi: 10.1103/PhysRevC.95.014611
2017KU29 Phys.Rev. C 96, 054614 (2017) R.Kumar, V.R.Sharma, A.Yadav, P.P.Singh, A.Agarwal, S.Appannababu, S.Mukherjee, B.P.Singh, R.Ali, R.K.Bhowmik Low-energy nuclear reaction of the 14N + 169Tm system: Incomplete fusion NUCLEAR REACTIONS 169Tm(14N, X)174W/175W/176W/177W/178Re/179Re/179Os, E=76, 78, 80, 83 MeV; measured Eγ, Iγ; deduced complete fusion (CF) σ(E) for 4n-, p3n-, p4n-, α2n-, α3n-, α4n- and α5n-channels, incomplete fusion (ICF) σ(E), and compared with statistical model code PACE4; discussed several other systems for complete and incomplete fusion strength functions and percentage fraction of ICF.
doi: 10.1103/PhysRevC.96.054614
2017PR04 Nucl.Phys. A962, 73 (2017) B.Pritychenko, M.Birch, B.Singh Revisiting Grodzins systematics of B(E2) values COMPILATION Z=6-96 (all even-Z nuclei); compiled, analyzed B(E2), E(4+1)/E(2+1). NUCLEAR STRUCTURE 10,12,14,16,18,20C, 16,18,20,22O, 18,20,22,24,26,28Ne, 22,24,26,28,30,32,34Mg, 24,26,28,30,32,34,36,38,40Si, 28,30,32,34,36,38,40,42,44S, 32,34,36,38,40,42,44,46,48Ar, 38,40,42,44,46,48,50Ca, 42,44,46,48,50,52,54,56Ti, 46,48,50,52,54,56,58,60,62,64Cr, 54,56,58,60,62,64,66,68Fe, 54,56,58,60,62,64,66,68,70,74Ni, 62,64,66,68,70,72,74,76,78,80Zn, 64,66,68,70,72,74,76,78,80,82Ge, 68,70,72,74,76,78,80,82,84Se, 72,74,76,78,80,82,84,86,88,90,92,94,96Kr, 76,78,80,82,84,86,88,90,92,94,96,98,100Sr, 82,84,86,88,90,92,94,96,98,100,102,104,106Zr, 92,94,96,98,100,102,104,106,108Mo, 96,98,100,102,104,106,108,110,112Ru, 100,102,104,106,108,110,112,114,116Pd, 100,102,104,106,108,110,112,114,116,118,120,122,124,126Cd, 104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Te, 114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144Xe, 122,124,126,128,130,132,134,136,138,140,142,144,146Ba, 124,126,128,130,132,134,136,138,140,142,144,146,148,150,152Cs, 130,132,134,136,138,140,142,144,146,148,150,152,154Nd, 134,136,138,140,142,144,146,148,150,152,154Sm, 138,148,152,154,156,158,160,162,164Gd, 152,154,156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 158,160,162,164Dy, 156,158,160,162,164,166,168,170,172,174,176Yb, 162,164,166,168,170,172,174,176,178,180Hf, 168,170,172,174,176,178,180,182,184,186,188W, 172,174,176,178,180,182,184,186,188,190,192Os, 176,178,180,182,184,186,188,190,192,194,196,198Pt, 180,182,184,186,188,196,198,200,202,204Hg, 184,186,204,206,208,210Pb, 194,196,198,200,202,210Po, 202,204,220,222Rn, 218,222,224,226,230Ra, 222,224,226,228,230,232,234Th, 230,232,234,236,238U, 238,240,242,244Pu, 240,244,246,248Cm; evaluated B(E2). Compared with Raman and Habs published evaluations, few elements also with available data.
doi: 10.1016/j.nuclphysa.2017.03.011
2017SH32 J.Phys.(London) G44, 105108 (2017) M.Shuaib, 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 Influence of incomplete fusion on complete fusion at energies above the Coulomb barrier NUCLEAR REACTIONS 169Tm(19F, X)185Pt/184Pt/183Pt/184Ir/183Ir/175W/174W/176Ta/175Ta/179Os/181Os/182Os/183Os/174W/175W/176W, E<120 MeV; measured reaction products, Eγ, Iγ; deduced σ, ICF strength function. Comparison with statistical model code pace4.
doi: 10.1088/1361-6471/aa84fb
2017SI08 Nucl.Data Sheets 141, 327 (2017) Nuclear Data Sheets for A=256 COMPILATION 256Cf, 256Es, 256Fm, 256Md, 256No, 256Lr, 256Rf, 256Db; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2017.03.002
2017SI20 Nucl.Data Sheets 144, 297 (2017) Nuclear Data Sheets for A = 258 COMPILATION 258Fm, 258Md, 258No, 258Lr, 258Rf, 258Db, 258Sg; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2017.08.003
2017SO12 Phys.Rev. C 96, 014620 (2017) A.Sood, P.P.Singh, R.N.Sahoo, P.Kumar, A.Yadav, V.R.Sharma, Mohd.Shuaib, M.K.Sharma, D.P.Singh, U.Gupta, R.Kumar, S.Aydin, B.P.Singh, H.J.Wollersheim, R.Prasad Fission-like events in the 12C + 169Tm system at low excitation energies NUCLEAR REACTIONS 169Tm(12C, X)74mBr/74Kr/75Br/75Ge/75Kr/76Kr/77Kr/78As/79Rb/81Sr/84Br/85Zr/86Y/87Zr/89Rb/93Y/94Ru/95Ru/97Nb/98mNb/101Tc/102mTc/104Tc/104Ag/105Tc/105In/175Re/176Re/177Re/178Re/177W/173Ta/174Ta/175Ta/176Ta/171Lu, E=77.81, 83.22, 89.25 MeV; measured Eγ, Iγ, recoil-catcher activation technique, half-life of 74Kr decay, production σ(E) of fission products and evaporation residues, charge and mass distribution of fission fragments at the pelletron accelerator facility of IUAC-New Delhi; deduced fission as one of the competing modes of deexcitation of complete and/or incomplete fusion composites at low excitation energies. Comparison with calculations using PACE code. 181Ta(16O, X), E*=67.04 MeV; 159Tb(16O, X), E*=57.1 MeV; 169Tm(16O, X), E*=61.06 MeV; 232Th(7Li, X), E*=41.7 MeV; 232Th(11B, X), E*=55.7 MeV; 238U(11B, X), E*=67.4 MeV; 238U(22Ne, X), E*=64.5 MeV; 208Pb(20Ne, X), E*=46.4 MeV; analyzed previous experimental data for isotopic yield distributions.
doi: 10.1103/PhysRevC.96.014620
2017YA25 Phys.Rev. C 96, 044614 (2017) A.Yadav, P.P.Singh, Mohd.Shuaib, V.R.Sharma, I.Bala, Unnati, S.Gupta, D.P.Singh, M.K.Sharma, R.Kumar, S.Murlithar, R.P.Singh, B.P.Singh, R.Prasad Systematic study of low-energy incomplete fusion: Role of entrance channel parameters NUCLEAR REACTIONS 159Tb(13C, 3n), (13C, 4n), (13C, 5n), (13C, 4np), (13C, 2nα), (13C, 3nα), (13C, 5nα), (13C, 2n2α), (13C, 3n2α), (13C, 4n2α), E AP 58, 60, 70, 73, 85, 88 MeV; measured reaction products, Eγ, Iγ, σ(E) at IUAC facility in New Delhi; deduced ICF fraction, and compared with several other systems in the literature. Comparison with theoretical calculations using PACE4 code. 168Lu; measured half-life of the decay of the g.s. from decay curve of 228-keV γ ray.
doi: 10.1103/PhysRevC.96.044614
2016BI09 Nucl.Phys. A955, 145 (2016) M.Birch, B.Pritychenko, B.Singh On the equivalence of experimental B(E2) values determined by various techniques COMPILATION Z=8-78; compiled available B(E2) data obtained by Coulomb excitation, Doppler-shift attenuation, nuclear resonance fluorescence, delayed coincidences, recoil Doppler shift, electron scattering; deduced general agreement of data obtained using different methods with weak indication that Doppler shift attenuation may somewhat differ from that of Coulomb excitation.
doi: 10.1016/j.nuclphysa.2016.06.012
2016CH23 Nucl.Data Sheets 135, 1 (2016) Nuclear Data Sheets for A = 42 COMPILATION 42Al, 42Si, 42P, 42S, 42Cl, 42Ar, 42K, 42Ca, 42Sc, 42Ti, 42V, 42Cr; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2016.06.001
2016JO10 Nucl.Data Sheets 138, 1 (2016) P.K.Joshi, B.Singh, S.Singh, A.K.Jain Nuclear Data Sheets for A = 139 COMPILATION 139Sn, 139Sb, 139Te, 139I, 139Xe, 139Cs, 139Ba, 139La, 139Ce, 139Pr, 139Nd, 139Pm, 139Sm, 139Eu, 139Gd, 139Tb, 139Dy; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2016.11.001
2016KO07 Nucl.Data Sheets 132, 257 (2016) F.Kondev, E.McCutchan, B.Singh, J.Tuli Nuclear Data Sheets for A = 227 COMPILATION 227Po, 227At, 227Rn, 227Fr, 227Ra, 227Ac, 227Th, 227Pa, 227U, 227Np; compiled, evaluated nuclear structure data.
doi: 10.1016/j.nds.2016.01.002
2016MA31 Nucl.Phys. A952, 62 (2016) B.Maheshwari, A.K.Jain, B.Singh Asymmetric behavior of the B(E2↑; 0+ → 2+) values in 104-130Sn and generalized seniority NUCLEAR STRUCTURE 104,106,108,110,112,114,116,118,120,122,124,126,128,130Sn; calculated B(E2) for 0+ to 2+1 state using both generalized seniority and seniority guided LSSM (Large Scale Shell Model); compared to data or evaluations; deduced B(E2) dip in the middle of full valence space (seen also in the data).
doi: 10.1016/j.nuclphysa.2016.04.021
2016PR01 At.Data Nucl.Data Tables 107, 1 (2016), Erratum At.Data Nucl.Data Tables 114, 371 (2017) B.Pritychenko, M.Birch, B.Singh, M.Horoi Tables of E2 transition probabilities from the first 2+ states in even-even nuclei COMPILATION 4,6,8,10He, 6,8,10,12,14Be, 10,12,14,16,18,20C, 12,14,16,18,20,22,24,26O, 16,18,20,22,24,26,28,30,32Ne, 20,22,24,26,28,30,32,34,36,38Mg, 24,26,28,30,32,34,36,38,40,42Si, 28,30,32,34,36,38,40,42,44,46S, 32,34,36,38,40,42,44,46,48Ar, 36,38,40,42,44,46,48,50,52,54Ca, 42,44,46,48,50,52,54,56,58Ti, 46,48,50,52,54,56,58,60,62,64Cr, 48,50,52,54,56,58,60,62,64,66,68Fe, 52,54,56,58,60,62,64,66,68,70,72,74,76Ni, 60,62,64,66,68,70,72,74,76,78,80Zn, 62,64,66,68,70,72,74,76,78,80,82,84,86Ge, 66,68,70,72,74,76,78,80,82,84,86Se, 72,74,76,78,80,82,84,86,88,90,92,94,96Kr, 76,78,80,82,84,86,88,90,92,94,96,98,100,102Sr, 80,82,84,86,88,90,92,94,96,98,100,102,104,106,108Zr, 84,86,88,90,92,94,96,98,100,102,104,106,108,110Mo, 88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118Ru, 92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128Pd, 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Cd, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138Te, 110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144Xe, 118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148Ba, 122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152Ce, 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156Nd, 130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160Sm, 138,140,142,144,146,148,150,152,154,156,158,160,162,164Gd, 140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170Dy, 144Er, 148,150,152,154,156,158,160,162,164,166,168,170,172,174Er, 152,154,156,158,160,162,164,166,168,170,172,174,176,178Yb, 160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192W, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198Os, 168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204Pt, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210Hg, 180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 206,208,210,212,214,216,218,220,222,224,226,228,230,232Ra, 214,216,218,220,222,224,226,228,230,232,234,236Th, 226,228,230,232,234,236,238,240,242U, 236,238,240,242,244,246Pu, 238,240,242,244,246,248,250Cm, 244,246,248,250,252Cf, 246,248Fm, 252,254,256Fm, 252,254No, 256Rf; compiled evaluated B(E2) values, T1/2, deformation parameters, first 2+ state energies in even-even nuclei. NUCLEAR STRUCTURE 6He, 10,12Be, 10,12,14,16,18,20C, 16,18,20,22O, 18,20,22,24,26,28,30Ne, 20,22,24,26,28,30,32,34Mg, 24,26,28,30,32,34,36,38,40Si, 30,32,34,36,38,40,42,44S, 32,34,36,38,40,42,44,46Ar, 38,40,42Ca, 46,48,50Ca, 42,44,46,48,50,52,54,56Ti, 46,48,50,52,54,56,58,60,62Cr, 50,52,54,56,58,60,62,64,66Fe, 54,56,58,60,62,64,66,68,70,72,74,76Ni, 62,64,66,68,70,72,74,76,78Zn, 104,106Sn; calculated transition energies, B(E2). Nuclear shell model.
doi: 10.1016/j.adt.2015.10.001
2016SH04 Nucl.Phys. A946, 182 (2016) Vijay R.Sharma, Pushpendra P.Singh, M.Shuaib, A.Yadav, I.Bala, Manoj K.Sharma, S.Gupta, D.P.Singh, R.Kumar, S.Muralithar, R.P.Singh, B.P.Singh, R.Prasad, R.K.Bhowmik Incomplete fusion in 16O+159Tb
doi: 10.1016/j.nuclphysa.2015.11.012
2016SH23 Phys.Rev. C 94, 014613 (2016) Mohd.Shuaib, V.R.Sharma, A.Yadav, P.P.Singh, M.K.Sharma, D.P.Singh, R.Kumar, R.P.Singh, S.Muralithar, B.P.Singh, R.Prasad Incomplete fusion studies in the 19F + 159Tb system at low energies and its correlation with various systematics NUCLEAR REACTIONS 159Tb(19F, X), E=99.45, 102.6, 105.44, 108.1 MeV from 15UD-pelletron accelerator of IUAC-New Delhi; measured Eγ, Iγ, σ(E) using activation method; deduced evaporation residue σ(E), complete fusion (CF) and incomplete fusion (ICF) σ(E); analyzed experimental excitation functions for the present reaction and data for 103Rh, 115In, 128Te, 159Tb, 165Ho, 169Tm(12C, X), 159Tb(13C, X), 159Tb, 169Tm, 181Ta(16O, X), and 175Lu(19F, X) reactions with statistical model code PACE4 to extract incomplete fusion strength function.
doi: 10.1103/PhysRevC.94.014613
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