NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Sharma Found 98 matches. 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
2024KA01 Nucl.Phys. A1042, 122791 (2024) A.Kaur, A.Kumar, Ch.Sharma, N.Dhanda, Raghav, N.Madhavan, S.Nath, J.Gehlot, Gonika, Ch.Kumar, P.Sherpa, A.Parihari, J.Pandey, A.K.Gupta, H.P.Sharma, B.R.Behera Evaporation residue cross-section measurements for 30Si+142Ce system NUCLEAR REACTIONS 142Ce(30Si, X), (28Si, X), E=105-132 MeV; measured reaction products; deduced evaporation residue (ER) σ. Comparison with coupled-channels calculations using the CCFULL code. The HYbrid Recoil mass Analyzer (HYRA) at IUAC, New Delhi.
doi: 10.1016/j.nuclphysa.2023.122791
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
2024SH09 Eur.Phys.J. A 60, (2024) H.Sharma, M.Maiti, M.Sagwal, R.Kumar, A.Singh, S.Sodaye Study of 9Be fusion in 93Nb near the Coulomb barrier NUCLEAR REACTIONS 93Nb(9Be, X), E=20-46 MeV; measured reaction products, Eγ, Iγ; deduced fusion σ. Comparison with the framework of the coupled-channel approach using the CCFULL code. The BARC-TIFR Pelletron facility in India.
doi: 10.1140/epja/s10050-024-01296-5
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
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
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
2023SH10 Eur.Phys.J. A 59, 71 (2023) H.Sharma, S.Jain, Amritpal, R.Kumar, M.K.Sharma Fusion dynamics of spherical and deformed projectiles with hexadecapole deformed target nuclei NUCLEAR STRUCTURE 147,148,149,150Sm, 152,154Sm, 172,174,176,178,180,182Yb, 40Sc, 43Sc, 55Sc, 77Sc, 82Sc, 70Ge, 72,73,74Ge, 16O, 48Ca, 48Ar, 62Fe; analyzed available data; deduced quadrupole and hexadecapole deformation of target nuclei impact on fusion dynamics.
doi: 10.1140/epja/s10050-023-00981-1
2023SH15 Phys.Rev. C 107, 064601 (2023) H.Sharma, M.Maiti, T.N.Nag, S.Sodaye Analysis of residual cross sections from 14N +93Nb reaction: Fusion dynamics of a non-α-cluster projectile NUCLEAR REACTIONS 93Nb(14N, 3n)104Cd, (14N, 2np)104Ag, (14N, 3np)103Ag, 93Nb(14N, 2nα)101Pd, 93Nb(14N, npα)101mRh, E=42-59 MeV; measured Eγ, Iγ; deduced σ(E), total fusion σ(E), Coulomb barrier and barrier radius. 103Ag; deduced γ-ray intensity 118.7 keV transition. Comparison to calculations done in the framework of EMPIRE3.2.2 and PACE4. Activation technique. Offline measurement with HPGe of stacked foils irradiated at BARC-TIFR Pelletron facility.
doi: 10.1103/PhysRevC.107.064601
2023SH16 Phys.Rev. C 107, 064615 (2023) C.Sharma, B.R.Behera, Shruti, Amit, B.Rohila, A.Kaur, Subodh, N.Dhanda, A.Kumar, P.Sugathan, A.Jhingan, K.S.Golda, N.Saneesh, M.Kumar, H.Arora, D.Arora, H.P.Sharma Fission dynamics and entrance-channel study in the 210Po compound nucleus via light-particle multiplicities NUCLEAR REACTIONS 198Pt(12C, X)210Po, E=81 MeV; measured reaction products, fission fragments, neutron time-of-flight, En, In, angular distribution, (fragment)n-coin; deduced neutron multiplicity spectra, neutron angular distribution, pre-scission and post-fission contributions to neutron multiplicity, time evolution of the reactions (dynamical model calculations with HICOL). Comparison to experimental results obtained for 18O+192Os reaction and statistical model calculations done using the JOANNE2 code. National Array of Neutron Detectors (NAND) consisting of 50 organic liquid scintillator detectors (BC 501A) coupled to the pair of position-sensitive multiwire proportional counters (MWPCs) at IUAC (New Delhi).
doi: 10.1103/PhysRevC.107.064615
2023SH25 Phys.Rev. C 108, 044613 (2023) H.Sharma, S.Jain, R.Kumar, M.K.Sharma Optimum orientation of compact and elongated hexadecapole deformed actinide targets: Application to synthesizing superheavy nuclei
doi: 10.1103/PhysRevC.108.044613
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
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 Iπ = 5- state in 126, 128Xe 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
2021KU10 Phys.Rev. C 103, 034315 (2021) A.Kundu, Md.S.R.Laskar, R.Palit, R.Raut, S.Santra, N.Shimizu, T.Togashi, E.Ideguchi, H.Pai, S.Ali, F.S.Babra, R.Banik, S.Bhattacharya, S.Biswas, B.Das, P.Dey, R.Donthi, A.Goswami, S.Jadhav, G.Mukherjee, B.S.Naidu, S.Rajbanshi, L.P.Singh, H.P.Sharma, S.S.Tiwary, A.T.Vazhappilly New lifetime measurement for the 2+1 level in 112Sn by the Doppler-shift attenuation method NUCLEAR REACTIONS 112Sn(35Cl, 35Cl'), E=195 MeV; measured Eγ, Iγ, γγ-coin, half-lives of the first 2+ and 3- states from Doppler broadening using INGA array at BARC-TIFR Pelletron LINAC Facility. 112Sn; deduced levels, J, π, B(E2), B(E1); calculated potential energy surface in (Q2, Q4) plane using Q-constrained Hartree-Fock method. Comparison with previous measurements, and with generalized seniority model (GSM) and state-of-the-art Monte Carlo shell model (MCSM) calculations. Systematics of B(E2) for the first 2+ states in A=112-124 Sn nuclei.
doi: 10.1103/PhysRevC.103.034315
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
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
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, 127I 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
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
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
2020GA04 Acta Phys.Pol. B51, 473 (2020) S.Ganguly, C.Majumder, S.S.Tiwary, H.P.Sharma, S.Chakraborty Magnetic Rotation in 60Ni: A Semiclassical Description NUCLEAR STRUCTURE 60Ni; calculated magnetic dipole bands, B(M1) using semiclassical particle rotor model. Comparison with available data.
doi: 10.5506/aphyspolb.51.473
2020GA28 Int.J.Mod.Phys. E29, 2050055 (2020) S.Ganguly, S.Chakraborty, C.Majumder, S.S.Tiwary, H.P.Sharma Total Routhian surface calculations to study the abrupt band termination phenomenon in 121, 123I NUCLEAR STRUCTURE 119,121,123I; analyzed available data on J, π, level energies; calculated total Routhian surface (TRS), transition quadrupole moments; deduced noncollective oblate shapes become yrast at higher angular frequency and at lower spin, all of these nuclei exhibit a collective prolate shape, loss of collectivity. Comparison with experimental data.
doi: 10.1142/S021830132050055X
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
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
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
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
2019KA29 Phys.Rev. C 100, 014620 (2019) K.Kapoor, N.Bansal, C.Sharma, S.Verma, K.Rani, R.Mahajan, B.R.Behera, K.P.Singh, A.Kumar, H.Singh, R.Dubey, N.Saneesh, M.Kumar, A.Yadav, A.Jhingan, P.Sugathan, B.K.Nayak, A.Saxena, H.P.Sharma, S.K.Chamoli Role of viscosity in fusion-fission dynamics via simultaneously measured neutron and α-particle multiplicities NUCLEAR REACTIONS 196Pt(16O, X)212Rn*, E=93, 99, 106 MeV pulsed beam; measured reaction products, particle-identification plot, Eα, Iα, En, In, (fragment)α- and (fragment)n-coin, pre-, and post-scission α and n multiplicity spectra, angular distributions using multiwire proportional counters for fragment detection, CsI(Tl) detectors for α detection, and organic scintillators for neutron detection at 15UD Pelletron facility of IUAC, New Delhi. Comparison with statistical model calculations using JOANNE2 code.
doi: 10.1103/PhysRevC.100.014620
2019KH03 Eur.Phys.J. A 55, 3 (2019) A.Khuntia, H.Sharma, S.K.Tiwari, R.Sahoo Radial flow and differential freeze-out in proton-proton collisions at √ s = 7 TeV at the LHC
doi: 10.1140/epja/i2019-12669-6
2019MA91 Braz.J.Phys. 49, 539 (2019) C.Majumder, H.P.Sharma, S.S.Tiwary, S.Chakraborty Possible Antimagnetic Rotational Band in 102Ru NUCLEAR STRUCTURE 102Ru; calculated levels, J, π for the g.s. band, dynamic moment of inertia versus spin; deduced possible anti-magnetic rotational character of states between 14+ and 24+. Semiclassical particle-rotor model calculations. Comparison with g.s. bands in 104Pd and 106Cd.
doi: 10.1007/s13538-019-00667-4
2019TI07 Eur.Phys.J. A 55, 163 (2019) S.S.Tiwary, H.P.Sharma, S.Chakraborty, C.Majumder, G.H.Bhat, J.A.Sheikh, P.Baneerjee, S.Ganguly, S.Rai, Pragati, Mayank, S.Kumar, A.Kumar, S.S.Bhattacharjee, R.P.Singh, S.Muralithar Observation of quasi-γ bands in Te nuclei NUCLEAR REACTIONS 122Sn(9Be, 3nα)124Te, E=48 MeV; measured Eγ, Iγ(θ), γγ-coin, γγγ-coin using INGA array (14 Compton suppressed HPGe clover detectors); deduced energy and intensity of coin using symmetric Eγ-Eγ γ-transitions, multiplicity using asymmetric Eγ-Eγ matrices and INGASORT and RADWARE codes, level energies; deduced, verified 124Te yrast band up to 4596 keV, other rotational bands, relative intensity of γ transitions, RDCO, polarization asymmetry.
doi: 10.1140/epja/i2019-12842-y
2018BA34 Phys.Rev. C 98, 034320 (2018) P.Banerjee, S.Ganguly, M.K.Pradhan, Md.M.Shaikh, H.P.Sharma, S.Chakraborty, R.Palit, R.G.Pillay, V.Nanal, S.Saha, J.Sethi Spectroscopy of weakly deformed bands in 87Zr: First observation of the shears mechanism in a Zr isotope NUCLEAR REACTIONS 60Ni(31P, n3p), E=112.5 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO ratio), level half-lives by DSA and line-shape analysis using the INGA array at BARC-TIFR Pelletron LINAC facility. 87Zr; deduced high-spin levels, J, π, γ-ray branching ratios, bands, magnetic-dipole (shears) band, multipolarities, mixing ratios, B(M1), B(E2). Systematics of level energies of similar negative-parity bands in 87Zr, 85Sr, 89Mo. Comparison with theoretical predictions.
doi: 10.1103/PhysRevC.98.034320
2018CH24 Phys.Rev. C 97, 054311 (2018); Erratum Phys.Rev. C 98, 059902 (2018) S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Rai, Pragati, S.Modi, P.Arumugam, Mayank, S.Kumar, R.Palit, A.Kumar, S.S.Bhattacharjee, R.P.Singh, S.Muralithar Rotational band on a three-quasineutron isomer in 127Xe NUCLEAR REACTIONS 122Sn(9Be, 4n), E=48 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization), and half-lives of isomers by γγ(t) using INGA array at 15UD pelletron accelerator of IUAC-New Delhi. 127Xe; deduced high-spin levels, J, π, bands, multipolarities, configurations, alignment plots, 3-qp states, reduced K-hindrance factors for γ transitions from 3-qp states in 127Xe and 129Ba. Comparison with modified particle rotor model (MPRM) calculations.
doi: 10.1103/PhysRevC.97.054311
2018CH29 Europhys.Lett. 121, 42001 (2018) S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Rai, Pragati, Mayank, S.Kumar, S.S.Bhattacharjee, R.P.Singh, S.Muralithar, A.Kumar, R.Palit Revised level structure of 127Xe NUCLEAR REACTIONS 122Sn(9Be, 4n)127Xe, E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π. Comparison with available data.
doi: 10.1209/0295-5075/121/42001
2018CH43 Eur.Phys.J. A 54, 112 (2018) S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.Kumar, A.Kumar, A.Kumar, S.Muralithar Negative parity three-quasiparticle band in 127I NUCLEAR REACTIONS 124Sn(7Li, 4nγ), E=33 MeV; measured Eγ, Iγ(θ), γγ-coin using 15 clover Compton suppressed detectors of INGA (Indian National Gamma Array); deduced 127I γ-ray transitions, levels, J, π, energy, high-spin states, linear polarization asymmetries, γ-intensity ratio of different negative parity states populated from the 2423 keV state (compared to Weisskopf transition rates) using CANDLE (Collection and Analysis of Nuclear Data using Linux nEtwork) and INGAsort and RadWare codes.
doi: 10.1140/epja/i2018-12540-4
2018CH50 Phys.Scr. 93, 115302 (2018) S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.Banerjee, S.Ganguly, S.R.Abhilash, D.Kabiraj, R.P.Singh, S.Muralithar Fabrication of 122Sn target and its application in γ-ray spectroscopy NUCLEAR REACTIONS 122Sn(9Be, 9Be'), E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, σ. Comparison with PACE4 calculations.
doi: 10.1088/1402-4896/aae346
2018MA28 Int.J.Mod.Phys. E27, 1850034 (2018) C.Majumder, H.P.Sharma, S.Chakraborty, S.S.Tiwary Study of antimagnetic rotation in 109, 111Cd NUCLEAR STRUCTURE 109,111Cd; calculated reduced electric quadrupole transition rates for the states of the negative parity bands using semiclassical model (SCM). Comparison with experimental values.
doi: 10.1142/S0218301318500349
2018SH19 Chin.Phys.C 42, 054104 (2018) Band head spin assignment of superdeformed bands in Hg isotopes through power index formula NUCLEAR STRUCTURE 189,190,191,192,193,194,195Hg; analyzed available data; deduced transition energies, head spins of super deformed band, moment of inertia using the power index formula.
doi: 10.1088/1674-1137/42/5/054104
2017CH15 Acta Phys.Pol. B48, 337 (2017) S.K.Chamoli, A.Rohilla, C.K.Gupta, R.P.Singh, S.Muralithar, S.Chakraborty, H.P.Sharma, A.Kumar, I.M.Govil, D.C.Biswas Investigating Prolate-Oblate Shape Inversion in Pt Nuclei Near A - 188 NUCLEAR REACTIONS 174Yb(18O, 2n), E=79 MeV; measured Eγ, Iγ using GDA (Gamma Detector Array) setup; deduced B(E2) vs spin, γ transitions near the yrast band, shifted and unshifted components of γ-ray transitions up to spin 12+, level population using set of Bateman equations, quadrupole moment, changing of nuclear shape of 188Pt at low spins; calculated B(E2) for states up to 45+ state using CHFB and IBM for oblate and prolate shapes; deduced absolute β2 deformation from the fit to measured data.
doi: 10.5506/APhysPolB.48.337
2017CH46 Braz.J.Phys. 47, 406 (2017) S.Chakraborty, H.P.Sharma, S.S.Tiwary, C.Majumder, P.K.Prajapati, S.Rai, P.Popli, M.Singh, S.S.Bhattacharjee, R.P.Singh, S.Muralithar, P.Banerjee, S.Ganguly, S.Kumar, A.Kumar, R.Palit Two-Neutron Alignment in 127Xe NUCLEAR REACTIONS 122Sn(9Be, 4n)127Xe, E=48 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, high-spin states. Comparison with Routhian calculations.
doi: 10.1007/s13538-017-0513-0
2017KA58 Phys.Rev. C 96, 054605 (2017) K.Kapoor, S.Verma, P.Sharma, R.Mahajan, N.Kaur, G.Kaur, B.R.Behera, K.P.Singh, A.Kumar, H.Singh, R.Dubey, N.Saneesh, A.Jhingan, P.Sugathan, G.Mohanto, B.K.Nayak, A.Saxena, H.P.Sharma, S.K.Chamoli, I.Mukul, V.Singh Fission time scale from pre-scission neutron and α multiplicities in the 16O + 194Pt reaction NUCLEAR REACTIONS 194Pt(16O, X)210Rn*, E=98.4 MeV; measured Eα, Iα, fission fragments, (fragments)α-coin, angular distributions using multiwire proportional counters (MWPC) for detection of fission fragments, and an array of CsI detectors for α particles at 15UD Pelletron facility of IUAC-New Delhi; deduced particle identification plot, fission fragments mass ratio distribution, normalized α-particle multiplicity spectra, dissipation energy and dinucleus elongation as function of time and angular momentum, transient times and saddle to scission times. Comparison with statistical model calculations using JOANNE2 code.
doi: 10.1103/PhysRevC.96.054605
2017RO07 Eur.Phys.J. A 53, 64 (2017) A.Rohilla, C.K.Gupta, R.P.Singh, S.Muralithar, S.Chakraborty, H.P.Sharma, A.Kumar, I.M.Govil, D.C.Biswas, S.K.Chamoli Lifetime measurements in shape transition nucleus 188Pt NUCLEAR REACTIONS 174Yb(18O, 4n), E=79 MeV; measured Eγ, Iγ using Gamma Detector Array of 6 HPGe and BGO multiplicity filter; deduced yrast band γ-ray transitions, yrast band quadrupole moment, B(E2), γ transitions T1/2 using LIFETIME code; calculated equilibrium shape, deformation, quadrupole moment for the yrast band using TRS (Total Routhian Surface), B(E2) using TPSM (Triaxial Projected Shell Model) and TRS (Total Routhian Surface).
doi: 10.1140/epja/i2017-12256-y
2017SH22 Chin.Phys.C 41, 084104 (2017) H.Sharma, N.Sharma, H.M.Mittal Systematic study of kinematic and dynamic moments of inertia of superdeformed bands with NpNn scheme NUCLEAR STRUCTURE N=72-112; analyzed available data; deduced systematics of kinematic moment of inertia, dynamic moment of inertia of superdeformed bands in A ∼ 130, 150, 190 mass regions.
doi: 10.1088/1674-1137/41/8/084104
2017SH48 Int.J.Mod.Phys. E26, 1750074 (2017) Band head spin assignment of superdeformed bands in A∼60-80 mass region through nuclear softness formula NUCLEAR STRUCTURE 58Ni, 58Cu, 62,65,68Zn, 84,86Zr; analyzed available data; deduced the band head spin of superdeformed rotational bands, dynamic moment of inertia, the nuclear softness formula applicability.
doi: 10.1142/S0218301317500744
2017SH56 Chin.Phys.C 41, 124105 (2017) Systematic study of rotational energy formulae for superdeformed bands in La and Ce isotopes NUCLEAR STRUCTURE 130La, 131,132,133Ce; analyzed available data; calculated of superdeformed (SD) band head spins using four parameter formula.
doi: 10.1088/1674-1137/41/12/124105
2016BA36 Phys.Rev. C 94, 014316 (2016) P.Banerjee, S.Ganguly, M.K.Pradhan, H.P.Sharma, S.Muralithar, R.P.Singh, R.K.Bhowmik Band structure in 113Sn NUCLEAR REACTIONS 100MO(19F, 5np), E=105 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization, IPDCO), level half-lives by DSAM at 15UD Pelletron accelerator of IUAC-New Delhi. 113Sn; deduced high-spin levels, J, π, B(E2), transition quadrupole moments, multipolarities, mixing ratios, moment of inertia plots, quadrupole deformations, bands and configurations. Calculated total-Routhian-surface plots in (β2, γ) plane using Woods-Saxon potential plus monopole pairing. Systematics of band in neighboring 113Sb, 109,111,113,115Sn nuclides.
doi: 10.1103/PhysRevC.94.014316
2015BA33 Phys.Rev. C 92, 024318 (2015) P.Banerjee, S.Ganguly, M.K.Pradhan, Md.M.Shaikh, H.P.Sharma, S.Chakraborty, R.Palit, R.G.Pillay, V.Nanal, S.Saha, J.Sethi, D.C.Biswas γ-ray spectroscopy of fission fragments produced in 208Pb(18O, f) NUCLEAR REACTIONS 208Pb(18O, F), E=90 MeV; measured Eγ, Iγ, γγ-coin, average total neutron multiplicity during fission, relative isotopic yields of fission fragments and fragment mass distribution by detecting prompt γ rays using INGA array at BARC-TIFR Pelletron LINAC facility. 110Pd, 116Cd; deduced high-spin levels, J, π, bands, configuration. 104Mo; observed γ.
doi: 10.1103/PhysRevC.92.024318
2014KA07 Eur.Phys.J. A 50, 5 (2014) N.Kaur, A.Kumar, G.Mukherjee, A.Singh, S.Kumar, R.Kaur, V.Singh, B.R.Behera, K.P.Singh, G.Singh, H.P.Sharma, S.Kumar, M.K.Raju, P.V.M.Rao, S.Muralithar, R.P.Singh, R.Kumar, N.Madhvan, R.K.Bhowmik High spin structure in 130, 131Ba NUCLEAR REACTIONS 122Sn(13C, 5n), (13C, 4n), E=65 MeV; measured Eγ, Iγ(θ), γγ-coin using INGA Compton-suppressed clover detectors. 130,131Ba deduced levels, J, π, high spin states, γ transitions, band crossing, deformation, bands alignment. 131Ba deduced asymmetry parameter using 152Eu source.
doi: 10.1140/epja/i2014-14005-2
2013BA10 Phys.Rev. C 87, 034321 (2013) P.Banerjee, S.Ganguly, M.K.Pradhan, H.P.Sharma, S.Muralithar, R.P.Singh, R.K.Bhowmik Rotational bands in 113Sb NUCLEAR REACTIONS 100Mo(19F, 6n), E=105 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(lin pol), half-lives by DSAM using INGA array at IUAC facility. 113Sb; deduced high-spin levels, J, π, bands, multipolarity, mixing ratio, B(E2), B(M1)/B(E2), transition quadrupole moments, β2. Comparison with Donau-Frauendorf semiclassical calculations.
doi: 10.1103/PhysRevC.87.034321
2012SC09 Nucl.Instrum.Methods Phys.Res. A681, 94 (2012) N.D.Scielzo, G.Li, M.G.Sternberg, G.Savard, P.F.Bertone, F.Buchinger, S.Caldwell, J.A.Clark, J.Crawford, C.M.Deibel, J.Fallis, J.P.Greene, S.Gulick, A.A.Hecht, D.Lascar, J.K.P.Lee, A.F.Levand, M.Pedretti, R.E.Segel, H.Sharma, K.S.Sharma, I.Tanihata, J.Van Schelt, R.M.Yee, B.J.Zabransky The β-decay Paul trap: A radiofrequency-quadrupole ion trap for precision β-decay studies RADIOACTIVITY 8Li(β-), (α); measured decay products, Eβ, Iβ, Eα, Iα, nuclear recoils; deduced technique for the β-ν angular correlations.
doi: 10.1016/j.nima.2012.04.035
2011BA05 Phys.Rev. C 83, 024316 (2011) P.Banerjee, S.Ganguly, M.K.Pradhan, H.P.Sharma, S.Muralithar, R.P.Singh, R.K.Bhowmik Experimental study of ΔI = 1 bands in 111In NUCLEAR REACTIONS 100Mo(19F, 4nα), E=105 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), level half-lives via DSAM using INGA array. 111In; deduced levels, J, π, bands, shears band, B(M1), B(E2), mixing ratio, shears angle, proton angle, gyromagnetic ratios. Comparison of B(M1) values with predictions of semi-classical model.
doi: 10.1103/PhysRevC.83.024316
2011DU05 Phys.Atomic Nuclei 74, 49 (2011) S.S.Duhan, M.Singh, R.Kharab, H.C.Sharma Dynamic polarization potentials for 6He + 209Bi and 11Li + 208Pb systems at near-barrier energies NUCLEAR REACTIONS 209Bi(6He, X), 208Pb(11Li, X), E(cm)<100 MeV; calculated internuclear separation, dynamic polarization potential, breakup transmission factors.
doi: 10.1134/S1063778811010066
2011FA10 Phys.Rev. C 84, 045807 (2011) J.Fallis, J.A.Clark, K.S.Sharma, G.Savard, F.Buchinger, S.Caldwell, A.Chaudhuri, J.E.Crawford, C.M.Deibel, S.Gulick, A.A.Hecht, D.Lascar, J.K.P.Lee, A.F.Levand, G.Li, B.F.Lundgren, A.Parikh, S.Russell, M.Scholte-van de Vorst, N.D.Scielzo, R.E.Segel, H.Sharma, S.Sinha, M.G.Sternberg, T.Sun, I.Tanihata, J.Van Schelt, J.C.Wang, Y.Wang, C.Wrede, Z.Zhou Mass measurements of isotopes of Nb, Mo, Tc, Ru, and Rh along the Νp- and rp-process paths using the Canadian Penning trap mass spectrometer ATOMIC MASSES 87Nb, 87,90,91,92Mo, 90,91,92,93Tc, 90,91,92,93,94Ru, 92,93,94,95Rh; measured cyclotron frequency ratios using Canadian Penning trap mass spectrometer; deduced mass excesses. 88Tc; deduced S(p). Comparison with previous measurements and AME-2003. Z=42-47, A=87-96; analyzed systematics of S(2p) values. Z=42-45, N=45-52; analyzed systematics of S(2n) values. Z=42-45, A=87-95; analyzed systematics of S(p) values. 94mAg; discussed 2p decay mode of 21+ isomer. NUCLEAR REACTIONS 58Ni(40Ca, X)87Nb/87Mo/90Mo/92Mo/90Tc/90Tc/92Tc/93Tc/90Ru/91Ru/92Ru/93Ru/92Rh/93Rh/94Rh, E=185, 190, 200 MeV; 58Ni(36Ar, X)91Tc/91Ru, E=125 MeV; Ni(36Ar, X)90Mo/91Mo/90Tc/91Tc/92Tc/91Ru/92Ru, E=130, 150 MeV; Ni(40Ca, X)93Tc/93Ru/94Ru/94Rh/95Rh, E=170 MeV; measured yields at ATLAS facility.
doi: 10.1103/PhysRevC.84.045807
2011KU06 Nucl.Phys. A849, 182 (2011) Parameterization scheme for determining the reaction cross sections at intermediate beam energies for normal and exotic nuclei NUCLEAR REACTIONS 12C(12C, X), E=20-1000 MeV/nucleon; 28Si, 40Ca, 58,60Ni, 112,116,118,120,124Sn, 208Pb(3He, X), E=32.1, 45.9 MeV/nucleon; 28Si, 40Ca, 58,60Ni, 112,116,118,120,124Sn, 208Pb(α, X), E=41, 48.1 MeV/nucleon; 12C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), E=20-40, 700-965 MeV/nucleon; 12C(17C, X), (18C, X), (19C, X), E=700-965 MeV/nucleon; 12C(13C, X), (14C, X), (15N, X), (16N, X), (17O, X), (18O, X), (19F, X), (20F, X), (21Ne, X), (22Ne, X), (23Na, X), (24Na, X), (25Mg, X), (26Mg, X), (27Si, X), (28Si, X), (29S, X), E=30 MeV/nucleon; 12C(23Al, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), (19F, X), (20Ne, X), (21Na, X), (22Mg, X), E=30 MeV/nucleon; 28Si(12N, X), E=29.3 MeV/nucleon; 28Si(12B, X), E=25.6 MeV/nucleon; 12C(17B, X), E=77 MeV/nucleon; calculated total σ. Comparison with other models and data.
doi: 10.1016/j.nuclphysa.2010.10.010
2010KU06 Chin.Phys.Lett. 27, 032502 (2010) Intermediate Energy Coulomb Excitation of Neutron-Rich Nuclei NUCLEAR STRUCTURE 38,40,42S, 44,46Ar; calculated B(E2) values suppression.
doi: 10.1088/0256-307X/27/3/032502
2010KU08 Phys.Rev. C 81, 037602 (2010) Parametrization scheme for determining a safe lower limit of the impact parameter for Coulomb excitation experiments NUCLEAR REACTIONS Au(26Ne, 26Ne'), Au(32Mg, 32Mg'), Au(32Si, 32Si'), Au(42S, 42S'), Au(46Ar, 46Ar'), Au(52Fe, 52Fe'), Au(78Kr, 78Kr'), E at Coulomb barrier; calculated σ; parametrization of scattering angle and impact parameter. Hartree-Fock-Bogoliubov (HFB) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.037602
2009KU07 Phys.Atomic Nuclei 72, 969 (2009) The B(E1) strength of 11Be extracted from the Coulomb excitation measurements NUCLEAR REACTIONS Pb(11Be, 11Be'), E=43 MeV/nucleon; analyzed Coulomb excitation data, extracted B(E1).
doi: 10.1134/S106377880906009X
2008FA11 Phys.Rev. C 78, 022801 (2008) J.Fallis, J.A.Clark, K.S.Sharma, G.Savard, F.Buchinger, S.Caldwell, J.E.Crawford, C.M.Deibel, J.L.Fisker, S.Gulick, A.A.Hecht, D.Lascar, J.K.P.Lee, A.F.Levand, G.Li, B.F.Lundgren, A.Parikh, S.Russell, M.Scholte-van de Vorst, N.D.Scielzo, R.E.Segel, H.Sharma, S.Sinha, M.Sternberg, T.Sun, I.Tanihata, J.Van Schelt, J.C.Wang, Y.Wang, C.Wrede, Z.Zhou Determination of the proton separation energy of 93Rh from mass measurements ATOMIC MASSES 92Ru, 93Rh; measured masses; deduced mass excesses, proton separation energies. Penning trap method.
doi: 10.1103/PhysRevC.78.022801
2008KH04 Int.J.Mod.Phys. E17, 693 (2008) R.Kharab, P.Singh, R.Kumar, H.C.Sharma Contribution of E2 and E1-E2 interference in the Coulomb breakup of 11Be NUCLEAR REACTIONS 238U(11Be, n10Be), E=63 MeV/nucleon; 238U(11Be, n10Be), E=72 MeV/nucleon; analyzed 10Be longitudinal momentum distributions from Coulomb dissociation including the effect of higher order multipole transitions.
doi: 10.1142/S0218301308010088
2008SI07 Nucl.Phys. A802, 82 (2008) P.Singh, R.Kumar, R.Kharab, H.C.Sharma Structural analysis of 19C through Coulomb dissociation reactions NUCLEAR REACTIONS 181Ta, 208Pb(19C, n18C), E=67-88 MeV/nucleon; calculated σ, relative energy spectra and momentum distribution for Coulomb breakup using eikonal approximation; deduced configuration. Comparison with data.
doi: 10.1016/j.nuclphysa.2008.01.020
2007KH08 Pramana 68, 779 (2007) R.Kharab, R.Kumar, P.Singh, H.C.Sharma One-neutron stripping reactions of 11Be and 19C on light target NUCLEAR REACTIONS 9Be(11Be, X), E=63 MeV/nucleon; 9Be(19C, X), E=88 MeV/nucleon; calculated one-neutron absorption cross section and longitudinal momentum distribution of the core fragment within the framework of eikonal approximation.
doi: 10.1007/s12043-007-0077-6
2006SA56 Int.J. Mass Spectrom. 251, 252 (2006) G.Savard, J.C.Wang, K.S.Sharma, H.Sharma, J.A.Clark, C.Boudreau, F.Buchinger, J.E.Crawford, J.P.Greene, S.Gulick, A.A.Hecht, J.K.P.Lee, A.F.Levand, N.D.Scielzo, W.Trimble, J.Vaz, B.J.Zabransky Studies of neutron-rich isotopes with the CPT mass spectrometer and the CARIBU project ATOMIC MASSES 141,142,143,144,145,146,147Ba, 143,144,145,146,147,148La, 145,146,147,148,149,150,151Ce, 148,149,150,151,152,153Pr; measured masses with the Canadian Penning Trap (CPT) mass spectrometer and reviewed the CARIBU Project. Isotopes produced from fission of 252Cf. Comparisons with 1995 and 2003 mass evaluations.
doi: 10.1016/j.ijms.2006.01.047
2005SA44 Phys.Rev.Lett. 95, 102501 (2005) G.Savard, F.Buchinger, J.A.Clark, J.E.Crawford, S.Gulick, J.C.Hardy, A.A.Hecht, J.K.P.Lee, A.F.Levand, N.D.Scielzo, H.Sharma, K.S.Sharma, I.Tanihata, A.C.C.Villari, Y.Wang Q Value of the Superallowed Decay of 46V and Its Influence on Vud and the Unitarity of the Cabibbo-Kobayashi-Maskawa Matrix ATOMIC MASSES 46Ti, 46V; measured masses; deduced Q(EC). Penning trap mass spectrometer. RADIOACTIVITY 46V(EC); analyzed masses; deduced Q(EC), log ft. 10C, 14O, 22Mg, 26mAl, 34Cl, 34Ar, 38mK, 42Sc, 46V, 50Mn, 54Co, 74Rb; compiled, analyzed log ft; deduced quark-mixing matrix element.
doi: 10.1103/PhysRevLett.95.102501
2003KO78 Acta Phys.Hung.N.S. 18, 399 (2003) Yu.N.Kopatch, M.Mutterer, P.Jesinger, J.von Kalben, I.Kojouharov, H.Schaffner, H.-J.Wollersheim, N.Kurz, E.Lubkiewicz, P.Adrich, H.Sharma, A.Wagner, Z.Mezentseva, W.H.Trzaska, A.Krasznahorkay, F.Gonnenwein Spontaneous Ternary Fission of 252Cf: New Experiment with GSI Super Clover Detectors RADIOACTIVITY 252Cf(SF); measured ternary fission associated Eγ, Iγ, (charged particle)γ-coin.
doi: 10.1556/APH.18.2003.2-4.48
2001SH02 Phys.Rev. C63, 014313 (2001) H.Sharma, B.Sethi, P.Banerjee, R.Goswami, R.K.Bhandari, J.Singh Experimental Evidence for Coexisting Structures in 125I NUCLEAR REACTIONS 123Sb(α, 2n), E=25-33 MeV; measured Eγ, Iγ(θ). 125I deduced levels, J, π, δ, B(E2), configurations, possible shape coexistence.
doi: 10.1103/PhysRevC.63.014313
2001SH40 Phys.Rev. C64, 064310 (2001) Coexistence of Prolate and Oblate Bands with Similar Proton Configurations in 121, 123, 125I NUCLEAR STRUCTURE 121,123,125I; calculated levels, J, π, configurations, deformation, rotational band features. Particle-rotor model.
doi: 10.1103/PhysRevC.64.064310
2001SH42 Pramana 57, 171 (2001) H.Sharma, B.Sethi, P.Banerjee, R.Goswami, R.K.Bhandari, J.Singh Particle-Rotor-Model Calculations in 125I NUCLEAR STRUCTURE 125I; calculated levels, J, π. Particle-rotor model, comparisons with data.
doi: 10.1007/s12043-001-0169-7
1999SH19 Phys.Rev. C59, 2446 (1999) H.Sharma, B.Sethi, R.Goswami, P.Banerjee, R.K.Bhandari, J.Singh Collective Bands in 125I NUCLEAR REACTIONS 123Sb(α, 2n), E=30 MeV; measured Eγ, Iγ, γγ-coin. 125I deduced levels, J, π, configurations.
doi: 10.1103/PhysRevC.59.2446
1997RA05 Appl.Radiat.Isot. 48, 327 (1997) Radiochemical Separation of 101mRh Via 101Pd from a Rhodium Target
doi: 10.1016/S0969-8043(96)00216-3
1992WO03 Appl.Radiat.Isot. 43, 551 (1992) D.H.Woods, S.A.Woods, M.J.Woods, J.L.Makepeace, C.W.A.Downey, D.Smith, A.S.Munster, S.E.M.Lucas, H.Sharma The Standardization and Measurement of Decay Scheme Data of 124I RADIOACTIVITY 124I(β+); measured β-spectra, T1/2, Eγ, γ-emission probabilities.
doi: 10.1016/0883-2889(92)90138-5
1991TI03 Radiochim.Acta 54, 29 (1991) N.D.Tinker, J.Zweit, H.L.Sharma, S.Downey, C.A.McAuliffe Production of No-Carrier Added 191Pt, a Radiolabel for the Synthesis and Biological Investigations of Platinum Anti-Tumour Compounds NUCLEAR REACTIONS, ICPND Ir(d, X)191Pt/193Pt/193mPt, E=19 MeV; Os(α, X)191Pt/193Pt/193mPt, E=38 MeV; measured residual production thick target yields. Activation technique.
1991ZW01 Appl.Radiat.Isot. 42, 193 (1991) J.Zweit, A.M.Smith, S.Downey, H.L.Sharma Excitation Functions for Deuteron Induced Reactions in Natural Nickel: Production of no-carrier-added 64Cu from enriched 64Ni targets for positron emission tomography NUCLEAR REACTIONS, ICPND Ni, 64Ni(d, xnyp)64Cu/61Cu/57Ni/55Co/56Co/57Co/58Co, 64Ni(d, 2n), E=threshold-19 MeV; measured residual production σ, thick target yields; deduced 64Ni(d, 2n) reaction effective σ. Activation technique, radiochemical separation.
doi: 10.1016/0883-2889(91)90073-A
1991ZW02 Appl.Radiat.Isot. 42, 199 (1991) Production of No-Carrier-Added Zirconium-89 for Positron Emission Tomography NUCLEAR REACTIONS, ICPND 89Y(d, 2n), (d, 3n), (d, 2np), E=20 MeV; measured thick target yields. Radiochemical separation.
doi: 10.1016/0883-2889(91)90074-B
1989SH04 J.Labelled Compd.Radiopharm. 26, 165 (1989) H.L.Sharma, J.Zweit, S.Downey, A.M.Smith, A.G.Smith Production of 124I for Positron Emission Tomography NUCLEAR REACTIONS, ICPND Sb, Te, 124Te(d, 2n)124I/125I/126I/131I, E=20 MeV; measured residual production yields. Natural Sb, Te, enriched 124Te targets.
doi: 10.1002/jlcr.2580260171
1989ZW01 J.Labelled Compd.Radiopharm. 26, 150 (1989) J.Zweit, H.L.Sharma, A.M.Smith, S.Downey Production of Carrier-Free 64Cu: A positron emitting radionuclide NUCLEAR REACTIONS, ICPND 64Ni(d, 2n), E ≈ 7.5-20 MeV; measured σ(E), yield vs E. Natural Ni target.
doi: 10.1002/jlcr.2580260165
1988ZW01 Appl.Radiat.Isot. 39, 1197 (1988) A Method for the Production of Iron-52 with a Very Low Iron-55 Contamination NUCLEAR REACTIONS, ICPND 50Cr(α, xnyp)52Fe/55Fe/52Mn/54Mn/56Mn/49Cr/51Cr/48V, E=38 MeV; measured residual production yields.
doi: 10.1016/0883-2889(88)90099-8
1987ZW01 Appl.Radiat.Isot. 38, 499 (1987) Production of Gallium-66, a Short-Lived, Positron Emitting Radionuclide NUCLEAR REACTIONS, ICPND Cu(α, X)66Ga/67Ga/64Cu/65Zn, E ≤ 40 MeV; measured residues σ(E). Natural target, Ge(Li) detector.
doi: 10.1016/0883-2889(87)90194-8
1986SH09 Int.J.Appl.Radiat.Isotop. 37, 105 (1986) H.Sharma, J.Zweit, A.M.Smith, S.Downey Production of Cobalt-55, a Short-Lived, Positron Emitting Radiolabel for Bleomycin NUCLEAR REACTIONS, ICPND 54Fe(d, n), E=12 MeV; measured Eγ, Iγ; deduced residual yield.
doi: 10.1016/0883-2889(86)90055-9
1982WA10 Phys.Rev. C25, 2353 (1982) E.Warde, R.Seltz, D.Magnac, H.L.Sharma 181Ta(p, t)179Ta Reaction: Evidence for particle-core coupling NUCLEAR REACTIONS 181Ta(p, t), E=19 MeV; measured σ(θ), σ(Et). 179Ta deduced levels, L, tentative J, π, rotational band. DWBA analysis.
doi: 10.1103/PhysRevC.25.2353
1980HY01 J.Phys.(London) G6, 261 (1980) M.Hyland, R.Chapman, J.L.Durell, J.N.Mo, M.Macphail, H.Sharma The Isotone Shift of the 2p3/2 Neutron Orbit Radius for N = 29 NUCLEAR REACTIONS 50Ti(t, d), E=2.25-3.0 MeV; measured Eγ, Iγ, σ(E). 54Fe(t, d), E=2.5-3.5 MeV; measured σ(E, θ). 51Ti, 55Fe, 49Ca, 53Cr deduced rms isotone shift of 2p3/2 n orbit.
doi: 10.1088/0305-4616/6/2/016
1979CH08 Nucl.Phys. A316, 40 (1979) R.Chapman, M.Hyland, J.L.Durell, J.N.Mo, M.Macphail, H.Sharma, N.H.Merrill Neutron Orbit Sizes in the Isotopes of Tin NUCLEAR REACTIONS 112,114,116,117,118,119Sn(t, d), E=4.25-5.75 MeV; measured σ(θ). 113,115,117,118,119,120Sn levels deduced rms radii of neutron orbits, S. Enriched targets.
doi: 10.1016/0375-9474(79)90672-9
1978BE09 Phys.Rev. C17, 529 (1978) G.Berrier-Ronsin, M.Vergnes, G.Rotbard, J.Vernotte, J.Kalifa, R.Seltz, H.L.Sharma Nuclear Levels in 191,193,195,197Pt Excited via Neutron Pickup NUCLEAR REACTIONS 192,194,196,198Pt(p, d), E=26 MeV; measured σ(Ed, θ); deduced Q. 192,194,196,198Pt(d, t), E=26 MeV; measured σ(Et, θ). 191,193,195,197Pt deduced levels, L, J, π, S. Natural, enriched targets.
doi: 10.1103/PhysRevC.17.529
1976SH15 Phys.Rev. C13, 2288 (1976) Osmium Isotopes with the (p, t) Reactions NUCLEAR REACTIONS 186,187,189,190,192Os(p, t), E=19 MeV; measured σ(Et, θ). 184,185,187,188,190Os deduced levels, K, L, J, π. Pairing plus DWBA.
doi: 10.1103/PhysRevC.13.2288
1975TA12 Phys.Rev. C12, 108 (1975) H.Taketani, H.L.Sharma, N.M.Hintz Shape Transitional Aspects of Odd-A Eu Isotopes Studied by the (p, t) Reaction NUCLEAR REACTIONS 151,153Eu(p, t), E=18.5, 19.0 MeV; measured σ(Et, θ); deduced Q. 149,151Eu deduced levels, J, π, L.
doi: 10.1103/PhysRevC.12.108
1974PA17 J.Inorg.Nucl.Chem. 36, 2392 (1974) Nuclear Charge Distribution in Mass Chains 131-134 in Thermal Neutron Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured Eγ; deduced fractional yields.
doi: 10.1016/0022-1902(74)80292-7
1973CH15 J.Inorg.Nucl.Chem. 35, 2621 (1973) A.Chattopadhyay, K.A.Dost, I.Krajbich, H.D.Sharma Mass-Yield Distributions in Photofission of 232Th and 238U NUCLEAR REACTIONS, Fission 232Th, 238U(γ, F), E=25-40 MeV; measured fission yields.
doi: 10.1016/0022-1902(73)80491-9
1973PA24 Radiochem.Radioanal.Lett. 15, 335 (1973) A simple method for the determination of independent yields in fission with a Ge(Li) detector NUCLEAR REACTIONS 235U(n, F)131Te/131Sb/132Te/132Sb/133Te/133Sb/133I/134I, E thermal; measured reaction products, Eγ, Iγ; deduced independent and cumulative fission yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13331. 1973SA01 Phys.Rev. C7, 395 (1973) Directional Correlation of the Gamma Transitions in 140Ce RADIOACTIVITY 140La; measured γγ(θ). 140Ce levels deduced J, π, γ-mixing.
doi: 10.1103/PhysRevC.7.395
1973SH09 Phys.Rev. C7, 2567 (1973) H.L.Sharma, R.Seltz, N.M.Hintz Search for an Excited Rotational Band in 98Mo with the (p, t) Reaction NUCLEAR REACTIONS 100Mo(p, t), E=19 MeV; measured σ(Et, θ). 98Mo deduced levels, L, J, π.
doi: 10.1103/PhysRevC.7.2567
1973SH18 Phys.Rev.Lett. 31, 1517 (1973) New K = 0 Bands and Two-Phonon Gamma Vibrations in 188Os and 190Os NUCLEAR REACTIONS 190,192Os(p, t), E=19.0 MeV; measured σ(Et, θ). 188,190Os deduced levels, J, π, B(E2).
doi: 10.1103/PhysRevLett.31.1517
1973TA28 Proc.Int.Conf.Nuclear Physics, Munich, J.de Boer, H.J.Mang, Eds., North-Holland Publ.Co., Amsterdam, Vol.1, p.229 (1973) H.Taketani, H.L.Sharma, N.M.Hintz Shape Transition Observed in the Odd-A Eu Isotopes by (p, t) and (3He, d) Reactions
1971SA09 Nucl.Phys. A171, 593 (1971) Energy Levels of 133Xe RADIOACTIVITY 133I, 135I[from 235U(n, F) or 238U(γ, F)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 133Xe deduced levels, J, π. Natural target, Ge(Li) detectors.
doi: 10.1016/0375-9474(71)90605-1
1971SH20 Progr.Theor.Phys. 45, 1337 (1971) Analysis of 127I(n, n'γ) Reaction Data NUCLEAR REACTIONS 127I(n, n'γ), E not given; analyzed σ(E;Eγ). 127I levels deduced J, π.
doi: 10.1143/PTP.45.1337
1970CA23 Nucl.Phys. A156, 338 (1970) The Excited States of 129Te Populated in the β- Decay of 129Sb RADIOACTIVITY 129Sb[from 235U(n, fission), 130Te(γ, p)]; measured Eγ.Iγ, γγ-coin; deduced log ft. 129Te deduced levels, J, π. Natural targets, Ge(Li) detector.
doi: 10.1016/0375-9474(70)90146-6
1970GE15 Can.J.Chem. 48, 641 (1970) L.H.Gevaert, R.E.Jervis, H.D.Sharma Cumulative yields in the 14 MeV neutron fission of 232Th and 238U in the symmetric region NUCLEAR REACTIONS 238U, 232Th(n, F)99Mo/103Ru/105Ru/109Pd/112Pd/111Ag/113Ag/115Cd/121Sn/125Sn, E=14 MeV; measured reaction products, Eγ, Iγ, Eβ, Iβ; deduced chain and mass fission yields.
doi: 10.1139/v70-104
1970MA45 Nucl.Phys. A156, 321 (1970) The β- Decay of 112Ag RADIOACTIVITY 112Ag[from 235U(n, fission), 113Cd(γ, p)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 112Cd deduced levels, J, π, γ-branching. Natural targets, Ge(Li) detector.
doi: 10.1016/0375-9474(70)90145-4
1970SH03 Nucl.Phys. A142, 291 (1970) Spin and Parity Assignments in 93Nb NUCLEAR REACTIONS 93Nb(n, n'γ), E=0.8-1.4 MeV; analyzed existing data. 93Nb levels deduced J, π. Optical model, Hauser-Feshbach theory.
doi: 10.1016/0375-9474(70)90530-0
1968SH02 Nucl.Phys. A106, 241 (1968) Spectroscopic Information on the 127I Levels Through Neutron Scattering
doi: 10.1016/0375-9474(67)90869-X
1963IY01 J.Inorg.Nucl.Chem. 25, 465 (1963) R.H.Iyer, C.K.Mathews, N.Ravindran, K.Rengan, D.V.Singh, M.V.Ramaniah, H.D.Sharma Fission of 232Th by Reactor Neutrons: Mass-Yield Curve NUCLEAR REACTIONS, Fission 232Th(n, F), E=reactor spectrum; measured A=77-156 mass-yield curves.
doi: 10.1016/0022-1902(63)80230-4
1953SH35 Curr.Sci.(India) 22, 45 (1953) Double Beta Decay of Te130 and Se82
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