NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Singh Found 65 matches. 2024CO05 Phys.Rev.Lett. 132, 152503 (2024) I.Cox, Z.Y.Xu, R.Grzywacz, W.-J.Ong, B.C.Rasco, N.Kitamura, D.Hoskins, S.Neupane, T.J.Ruland, J.M.Allmond, T.T.King, R.S.Lubna, K.P.Rykaczewski, H.Schatz, B.M.Sherrill, O.B.Tarasov, A.D.Ayangeakaa, H.C.Berg, D.L.Bleuel, G.Cerizza, J.Christie, A.Chester, J.Davis, C.Dembski, A.A.Doetsch, J.G.Duarte, A.Estrade, A.Fijalkowska, T.J.Gray, E.C.Good, K.Haak, S.Hanai, J.T.Harke, C.Harris, K.Hermansen, D.E.M.Hoff, R.Jain, M.Karny, K.Kolos, A.Laminack, S.N.Liddick, B.Longfellow, S.Lyons, M.Madurga, M.J.Mogannam, A.Nowicki, T.H.Ogunbeku, G.Owens-Fryar, M.M.Rajabali, A.L.Richard, E.K.Ronning, G.E.Rose, K.Siegl, M.Singh, A.Spyrou, A.Sweet, A.Tsantiri, W.B.Walters, R.Yokoyama Proton Shell Gaps in N=28 Nuclei from the First Complete Spectroscopy Study with FRIB Decay Station Initiator RADIOACTIVITY 45Cl(β-) [from 9Be(82Se, X), E=165 MeV/nucleon]; measured decay products, Eγ, Iγ, Eβ, Iβ; deduced β-decay strength distribution, the transitioning of neutrons into protons excited across the Z=20 shell gap. Comparison with shell model calculations using SDPF-MU interaction. The Facility for Rare Isotope Beams (FRIB) with the FRIB Decay Station Initiator.
doi: 10.1103/PhysRevLett.132.152503
2024KA10 Phys.Rev. C 109, L031902 (2024) Disoriented isospin condensates may be the source of anomalous kaon correlations measured in Pb-Pb collisions at √ σNN=2.76 TeV
doi: 10.1103/PhysRevC.109.L031902
2024RA03 Nucl.Phys. A1042, 122815 (2024) Role of multi-neutron transfer channels on fusion enhancement NUCLEAR REACTIONS 116,122Sn(40Ar, X), 124Sn(40Ca, X), E(cm)=90-150 MeV; analyzed available data; deduced σ with coupled channel (CC) approach using code-CCFULL.
doi: 10.1016/j.nuclphysa.2023.122815
2023GR04 Phys.Rev.Lett. 130, 242501 (2023) T.J.Gray, J.M.Allmond, Z.Xu, T.T.King, R.S.Lubna, H.L.Crawford, V.Tripathi, B.P.Crider, R.Grzywacz, S.N.Liddick, A.O.Macchiavelli, T.Miyagi, A.Poves, A.Andalib, E.Argo, C.Benetti, S.Bhattacharya, C.M.Campbell, M.P.Carpenter, J.Chan, A.Chester, J.Christie, B.R.Clark, I.Cox, A.A.Doetsch, J.Dopfer, J.G.Duarte, P.Fallon, A.Frotscher, T.Gaballah, J.T.Harke, J.Heideman, H.Huegen, J.D.Holt, R.Jain, N.Kitamura, K.Kolos, F.G.Kondev, A.Laminack, B.Longfellow, S.Luitel, M.Madurga, R.Mahajan, M.J.Mogannam, C.Morse, S.Neupane, A.Nowicki, T.H.Ogunbeku, W.-J.Ong, C.Porzio, C.J.Prokop, B.C.Rasco, E.K.Ronning, E.Rubino, T.J.Ruland, K.P.Rykaczewski, L.Schaedig, D.Seweryniak, K.Siegl, M.Singh, A.E.Stuchbery, S.L.Tabor, T.L.Tang, T.Wheeler, J.A.Winger, J.L.Wood Microsecond Isomer at the N=20 Island of Shape Inversion Observed at FRIB RADIOACTIVITY 32Na(IT), (β-) [from 9Be(48Ca, X), E=172.3 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced γ-ray energies, partial level scheme, isomeric T1/2, B(E2), single-particle occupancies. Comparison with calculations. The Advanced Rare Isotope Separator (ARIS), the FRIB Decay Station initiator (FDSi).
doi: 10.1103/PhysRevLett.130.242501
2023KA04 Phys.Rev. C 107, 014913 (2023) Confronting anomalous kaon correlations measured in Pb-Pb collisions at √ sNN = 2.76 TeV
doi: 10.1103/PhysRevC.107.014913
2023LU07 Phys.Rev. C 108, 014329 (2023) R.S.Lubna, S.N.Liddick, T.H.Ogunbeku, A.Chester, J.M.Allmond, S.Bhattacharya, C.M.Campbell, M.P.Carpenter, K.L.Childers, P.Chowdhury, J.Christie, B.R.Clark, R.M.Clark, I.Cox, H.L.Crawford, B.P.Crider, A.A.Doetsch, P.Fallon, A.Frotscher, T.Gaballah, T.J.Gray, R.Grzywacz, J.T.Harke, A.C.Hartley, R.Jain, T.T.King, N.Kitamura, K.Kolos, F.G.Kondev, E.Lamere, R.Lewis, B.Longfellow, S.Lyons, S.Luitel, M.Madurga, R.Mahajan, M.J.Mogannam, C.Morse, S.K.Neupane, W.-J.Ong, D.Perez-Loureiro, C.Porzio, C.J.Prokop, A.L.Richard, E.K.Ronning, E.Rubino, K.Rykaczewski, D.Seweryniak, K.Siegl, U.Silwal, M.Singh, D.P.Siwakoti, D.C.Smith, M.K.Smith, S.L.Tabor, T.L.Tang, V.Tripathi, A.Volya, T.Wheeler, Y.Xiao, Z.Xu β decay of 36Mg and 36Al: Identification of a β-decaying isomer in 36Al RADIOACTIVITY 36Mg, 36Al(β-)[from 9Be(48Ca, X), E=140 MeV/nucleon for experiment at NSCL and 9Be(48Ca, X), E=172.3 MeV/nucleon for experiment at FRIB]; 36Al, 36mAl(β-)[from 36Mg(β-); measured Eγ, Iγ; deduced T1/2. 36Al; deduced levels, J, π, newly-observed β-decaying isomer, T1/2 of the isomer. 36Si; deduced levels, J, π. Comparison to shell model calculations performed with the FSU interaction using code CoSMo. For experiment at NSCL - CeBr3 based implantation detector with position-sensitive photomultiplier tube was surrounded by 16 segmented germanium detectors (SeGa) and 15 LaBr3 detectors. For experiment at FRIB - YSO scintillator based implantation detector segmented into 48x48 pixels was surrounded by 11 HPGe clover detectors and LaBr3 detectors from one side and the neutron detector array VANDLE from the other side.
doi: 10.1103/PhysRevC.108.014329
2023SI24 Phys.Rev. C 108, 054901 (2023) M.Singh, M.Kurian, S.Jeon, C.Gale Open charm phenomenology with a multistage approach to relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.108.054901
2023XU06 Phys.Rev.Lett. 131, 022501 (2023) Z.Y.Xu, M.Madurga, R.Grzywacz, T.T.King, A.Algora, A.N.Andreyev, J.Benito, T.Berry, M.J.G.Borge, C.Costache, H.De Witte, A.Fijalkowska, L.M.Fraile, H.O.U.Fynbo, A.Gottardo, C.Halverson, L.J.Harkness-Brennan, J.Heideman, M.Huyse, A.Illana, L.Janiak, D.S.Judson, A.Korgul, T.Kurtukian-Nieto, I.Lazarus, R.Lica, R.Lozeva, N.Marginean, R.Marginean, C.Mazzocchi, C.Mihai, R.E.Mihai, A.I.Morales, R.D.Page, J.Pakarinen, M.Piersa-Silkowska, Z.Podolyak, P.Sarriguren, M.Singh, C.Sotty, M.Stepaniuk, O.Tengblad, A.Turturica, P.Van Duppen, V.Vedia, S.Vinals, N.Warr, R.Yokoyama, C.X.Yuan 133In: A Rosetta Stone for Decays of r-Process Nuclei RADIOACTIVITY 133In(IT), (β-), (β-n); measured decay products, En, In, Eβ, Iβ, Eγ, Iγ; deduced excitation energy and decay strength, partial T1/2. Comparison with large-scale shell model (LSSM) calculations. The ISOLDE Decay Station (IDS), The Isotope Separator On-Line (ISOLDE) facility at CERN.
doi: 10.1103/PhysRevLett.131.022501
2023XU08 Phys.Rev. C 108, 014314 (2023) Z.Y.Xu, M.Madurga, R.Grzywacz, T.T.King, A.Algora, A.N.Andreyev, J.Benito, T.Berry, M.J.G.Borge, C.Costache, H.De Witte, A.Fijalkowska, L.M.Fraile, H.O.U.Fynbo, A.Gottardo, C.Halverson, L.J.Harkness-Brennan, J.Heideman, M.Huyse, A.Illana, L.Janiak, D.S.Judson, A.Korgul, T.Kurtukian-Nieto, I.Lazarus, R.Lica, R.Lozeva, N.Marginean, R.Marginean, C.Mazzocchi, C.Mihai, R.E.Mihai, A.I.Morales, R.D.Page, J.Pakarinen, M.Piersa-Silkowska, Zs.Podolyak, P.Sarriguren, M.Singh, Ch.Sotty, M.Stepaniuk, O.Tengblad, A.Turturica, P.Van Duppen, V.Vedia, S.Vinals, N.Warr, R.Yokoyama, C.X.Yuan β-delayed neutron spectroscopy of 133In RADIOACTIVITY 133,133mIn(β-)(β-n); decay products, neutron time-of-flight, En, In, Eβ, Iβ, Eγ, Iγ, βγ-coin, nβ-coin; deduced feeding intensities, neutron-emission probabilities, logft, β-decay strength distribution, Gamow-Teller transition. 133Sn; deduced levels, J, π, configurations. Comparison of 133Sn and 131Sn level schemes. The ISOLDE Decay Station (IDS) at The Isotope Separator On-Line (ISOLDE) facility at CERN.
doi: 10.1103/PhysRevC.108.014314
2023YO04 Phys.Rev. C 108, 064307 (2023) R.Yokoyama, R.Grzywacz, B.C.Rasco, N.Brewer, K.P.Rykaczewski, I.Dillmann, J.L.Tain, S.Nishimura, D.S.Ahn, A.Algora, J.M.Allmond, J.Agramunt, H.Baba, S.Bae, C.G.Bruno, R.Caballero-Folch, F.Calvino, P.J.Coleman-Smith, G.Cortes, T.Davinson, C.Domingo-Pardo, A.Estrade, N.Fukuda, S.Go, C.J.Griffin, J.Ha, O.Hall, L.J.Harkness-Brennan, J.Heideman, T.Isobe, D.Kahl, M.Karny, T.Kawano, L.H.Khiem, T.T.King, G.G.Kiss, A.Korgul, S.Kubono, M.Labiche, I.Lazarus, J.Liang, J.Liu, G.Lorusso, M.Madurga, K.Matsui, K.Miernik, F.Montes, A.I.Morales, P.Morrall, N.Nepal, R.D.Page, V.H.Phong, M.Piersa-Silkowska, M.Prydderch, V.F.E.Pucknell, M.M.Rajabali, B.Rubio, Y.Saito, H.Sakurai, Y.Shimizu, J.Simpson, M.Singh, D.W.Stracener, T.Sumikama, H.Suzuki, H.Takeda, A.Tarifeno-Saldivia, S.L.Thomas, A.Tolosa-Delgado, M.Wolinska-Cichocka, P.J.Woods, X.X.Xu β-delayed neutron emissions from N>50 gallium isotopes
doi: 10.1103/PhysRevC.108.064307
2022AN01 Nucl.Phys. A1017, 122343 (2022) X.An, M.Bluhm, L.Du, G.V.Dunne, H.Elfner, C.Gale, J.Grefa, U.Heinz, A.Huang, J.M.Karthein, D.E.Kharzeev, V.Koch, J.Liao, S.Li, M.Martinez, M.McNelis, D.Mroczek, S.Mukherjee, M.Nahrgang, A.R.Nava Acuna, J.Noronha-Hostler, D.Oliinychenko, P.Parotto, I.Portillo, M.S.Pradeep, S.Pratt, K.Rajagopal, C.Ratti, G.Ridgway, T.Schafer, B.Schenke, C.Shen, S.Shi, M.Singh, V.Skokov, D.T.Son, A.Sorensen, M.Stephanov, R.Venugopalan, V.Vovchenko, R.Weller, H.-U.Yee, Y.Yin The BEST framework for the search for the QCD critical point and the chiral magnetic effect
doi: 10.1016/j.nuclphysa.2021.122343
2022CR03 Phys.Rev.Lett. 129, 212501 (2022) H.L.Crawford, V.Tripathi, J.M.Allmond, B.P.Crider, R.Grzywacz, S.N.Liddick, A.Andalib, E.Argo, C.Benetti, S.Bhattacharya, C.M.Campbell, M.P.Carpenter, J.Chan, A.Chester, J.Christie, B.R.Clark, I.Cox, A.A.Doetsch, J.Dopfer, J.G.Duarte, P.Fallon, A.Frotscher, T.Gaballah, T.J.Gray, J.T.Harke, J.Heideman, H.Heugen, R.Jain, T.T.King, N.Kitamura, K.Kolos, F.G.Kondev, A.Laminack, B.Longfellow, R.S.Lubna, S.Luitel, M.Madurga, R.Mahajan, M.J.Mogannam, C.Morse, S.Neupane, A.Nowicki, T.H.Ogunbeku, W.-J.Ong, C.Porzio, C.J.Prokop, B.C.Rasco, E.K.Ronning, E.Rubino, T.J.Ruland, K.P.Rykaczewski, L.Schaedig, D.Seweryniak, K.Siegl, M.Singh, S.L.Tabor, T.L.Tang, T.Wheeler, J.A.Winger, Z.Xu Crossing N = 28 Toward the Neutron Drip Line: First Measurement of Half-Lives at FRIB RADIOACTIVITY 44,45P, 42,43Si, 39,40,41Al, 36,37,38Mg, 35Na, 32Ne, 29F(β-), (β-n), (β-2n) [from 9Be(48Ca, X), E=172.3 MeV/nucleon]; measured decay products, Eβ, Iβ, En, In; deduced T1/2. Comparison with the latest quasiparticle random phase approximation and shell-model calculations and available data. The Facility for Rare Isotope Beams (FRIB) with the FRIB decay station initiator.
doi: 10.1103/PhysRevLett.129.212501
2022DE29 Phys.Rev. C 106, 054906 (2022) A.De, J.I.Kapusta, M.Singh, T.Welle Comprehensive simulation of heavy-ion collisions at nonzero baryon chemical potential
doi: 10.1103/PhysRevC.106.054906
2022KI23 Astrophys.J. 936, 107 (2022) G.G.Kiss, A.Vitez-Sveiczer, Y.Saito, A.Tarifeno-Saldivia, M.Pallas, J.L.Tain, I.Dillmann, J.Agramunt, A.Algora, C.Domingo-Pardo, A.Estrade, C.Appleton, J.M.Allmond, P.Aguilera, H.Baba, N.T.Brewer, C.Bruno, R.Caballero-Folch, F.Calvino, P.J.Coleman-Smith, G.Cortes, T.Davinson, N.Fukuda, Z.Ge, S.Go, C.J.Griffin, R.K.Grzywacz, O.Hall, A.Horvath, J.Ha, L.J.Harkness-Brennan, T.Isobe, D.Kahl, T.T.King, A.Korgul, S.Kovacs, R.Krucken, S.Kubono, M.Labiche, J.Liu, J.Liang, M.Madurga, K.Miernik, F.Molina, A.I.Morales, M.R.Mumpower, E.Nacher, A.Navarro, N.Nepal, S.Nishimura, M.Piersa-Silkowska, V.Phong, B.C.Rasco, B.Rubio, K.P.Rykaczewski, J.Romero-Barrientos, H.Sakurai, L.Sexton, Y.Shimizu, M.Singh, T.Sprouse, T.Sumikama, R.Surman, H.Suzuki, T.N.Szegedi, H.Takeda, A.Tolosa, K.Wang, M.Wolinska-Cichocka, P.Woods, R.Yokoyama, Z.Xu Measuring the β-decay Properties of Neutron-rich Exotic Pm, Sm, Eu, and Gd Isotopes to Constrain the Nucleosynthesis Yields in the Rare-earth Region NUCLEAR REACTIONS 9Be(238U, X), E=345 MeV/nucleon; measured reaction products, TOF, Eβ, Iβ. 159,160,161,162,163,164,165,166Pm, 161,162,163,164,165,166,167,168Sm, 165,166,167,168,169,170Eu, 167,168,169,170,171,172Gd; deduced new isotopes T1/2 and β-delayed neutron emission probabilities, relative r-process abundance pattern for the neutron-star merger scenario. RIKEN Nishina Center, the Advanced Implantation Detector Array (AIDA) and the BRIKEN neutron detector array.
doi: 10.3847/1538-4357/ac80fc
2022KU25 Int.J.Mod.Phys. E31, 2250061 (2022) B.Kumari, M.K.Singh, R.Singh, V.Singh Emission feature of the shower particles produced in backward hemisphere in the interaction of 84Kr36 + Em at 1 A GeV NUCLEAR REACTIONS Ag, Br(84Kr, X), E=1 GeV/nucleon; measured reaction products; deduced emission probability of the shower particle, correlations, fitting parameters. The nuclear emulsion detector (NED), GSI, Germany.
doi: 10.1142/S0218301322500616
2022PA29 Phys.Rev. C 106, 034901 (2022) D.Pablos, M.Singh, S.Jeon, C.Gale Minijet quenching in a concurrent jet + hydro evolution and the nonequilibrium quark-gluon plasma
doi: 10.1103/PhysRevC.106.034901
2022SI11 Phys.Part. and Nucl.Lett. 19, 87 (2022) M.Singh, Y.Singh, A.K.Varshney, K.K.Gupta Rigid Triaxial Rotor Model Description of γγ-Band in Some Even Nuclei NUCLEAR STRUCTURE 104,106,108Mo, 112Ru, 154,156Gd, 160,162Dy, 192Os, 178Hf; calculated odd-even staggering (OES) in γγ-band in rigid triaxial rotor model (RTRM); deduced the OES in γ-band and γγ-band obtained from rigid triaxial rotor model (RTRM) are constant for an axial rotor and staggering appears in same phase for a rotor with large triaxial deformation. Comparison with experimental data.
doi: 10.1134/S154747712202011X
2021KA40 Int.J.Mod.Phys. E30, 2130008 (2021) Current status of different detector technologies in the searches of 0νββ RADIOACTIVITY 76Ge, 130Te, 136Xe, 100Mo, 82Se, 116Cd(2β-); analyzed available data; deduced experimental facilities requirements.
doi: 10.1142/S0218301321300083
2021RA22 Phys.Rev. C 104, L042801 (2021) J.S.Randhawa, R.Kanungo, J.Refsgaard, P.Mohr, T.Ahn, M.Alcorta, C.Andreoiu, S.S.Bhattacharjee, B.Davids, G.Christian, A.A.Chen, R.Coleman, P.E.Garrett, G.F.Grinyer, E.G.Fuakye, G.Hackman, J.Hollett, R.Jain, K.Kapoor, R.Krucken, A.Laffoley, A.Lennarz, J.Liang, Z.Meisel, B.Nikhil, A.Psaltis, A.Radich, M.Rocchini, N.Saei, M.Saxena, M.Singh, C.Svensson, P.Subramaniam, A.Talebitaher, S.Upadhyayula, C.Waterfield, J.Williams, M.Williams First direct measurement of 59Cu(p, α)56Ni: step towards constraining the Ni-Cu cycle in the cosmos NUCLEAR REACTIONS 1H(59Cu, α)56Ni, E=8.5 MeV/nucleon, [secondary 59Cu beam from Nb(p, X), E=480 MeV at the TRIUMF cyclotron, followed by re-acceleration of 59Cu beam by ISAC-II superconducting LINAC, solid H2 target]; measured protons and α particles, angle-integrated σ using thick single-sided silicon strip detectors and a layer of thick CsI(Tl) detectors; deduced ratio of integrated σ to total σ, exclusive population of the ground state of 56Ni in (p, α). Comparison with Hauser-Feshbach based statistical model calculations; deduced overestimation of (p, α) cross section in this region. Discussed impact on νp process and x-ray bursts (XRBs). Relevance to Ni-Cu cycle in nucleosynthesis, with competing 59Cu(p, α)56Ni and 59Cu(p, γ)60Zn reactions.
doi: 10.1103/PhysRevC.104.L042801
2021SI13 Eur.Phys.J.Plus 136, 419 (2021) M.K.Singh, S.Karmakar, V.Singh Multiplicity characteristics of target fragments and shower particles with noninteracting projectile nucleons emitted in 84Kr-Em interaction at 1 A GeV NUCLEAR REACTIONS H, C, N, O, Ag, Br, 127I(84Kr, X)4He/7Li/84Kr, E=1 GeV/nucleon; analyzed available data; deduced multiplicities.
doi: 10.1140/epjp/s13360-021-01429-5
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
2020KU27 Phys.Rev. C 102, 044907 (2020) M.Kurian, M.Singh, V.Chandra, S.Jeon, C.Gale Charm quark dynamics in quark-gluon plasma with 3 + 1D viscous hydrodynamics
doi: 10.1103/PhysRevC.102.044907
2020KU30 Int.J.Mod.Phys. E29, 2050077 (2020) S.Kumar, M.K.Singh, R.K.Jain, V.Singh Characteristics of the projectile and target fragments produced in 84Kr36 - emulsion interaction at 1 GeV per nucleon NUCLEAR REACTIONS H, C, Ag(84Kr, X), E=1 GeV/nucleon; analyzed available data; deduced variation of the fragmentation parameter for charged fragments.
doi: 10.1142/S0218301320500779
2020SI07 Eur.Phys.J.Plus 135, 373 (2020) M.K.Singh, U.Singh, B.R.K.Gupta, N.Bhatnagar, V.Singh Emission characteristics of intermediate mass fragments by the 8436Kr projectile in nuclear emulsion detector at 1 GeV per nucleon NUCLEAR REACTIONS H, C, Ag(84Kr, X), E=1 GeV/nucleon; measured reaction products; deduced correlation between intermediate mass fragments and the total charge confined in fragments, anti-correlation between the mean multiplicities of particles emitted from the target and the bound system charge.
doi: 10.1140/epjp/s13360-020-00381-0
2020SI18 Chin.J.Phys.(Taiwan) 67, 107 (2020) M.K.Singh, S.Kumar, R.K.Jain, V.Singh Study of emission characteristics of the projectile fragments produced in the interaction of 84Kr36 with nuclear emulsion detector at 1 GeV NUCLEAR REACTIONS Ag, C, H, O(84Kr, X), E=1 GeV/nucleon; measured reaction products; deduced average charge distribution, multiplicity distribution of the projectile fragments, variation of the fragment parameters with respect to mass of the projectile beam. Comparison with available data.
doi: 10.1016/j.cjph.2020.06.017
2020SI30 Chin.J.Phys.(Taiwan) 67, 107 (2020) M.K.Singh, S.Kumar, R.K.Jain, V.Singh Study of emission characteristics of the projectile fragments produced in the interaction of 84Kr36 with nuclear emulsion detector at 1 GeV NUCLEAR REACTIONS C, Ag(84Kr, X), E=1 GeV/nucleon; measured reaction products; deduced that the emission of projectile fragments is strongly dependent on the interaction with different type of the target groups of nuclear emulsion detector as well as on the mass of the projectile beam, multiplicity distributions, parameters.
doi: 10.1016/j.cjph.2020.06.017
2019MA73 Int.J.Mod.Phys. E28, 1950058 (2019) N.Marimuthu, R.Prajapati, M.K.Singh, V.Singh, S.S.R.Inbanathan Study of relativistic charged particles production in 84Kr36 emulsion interactions ∼ 1GeV per nucleon with wounded nucleon model NUCLEAR REACTIONS Ag, Br(84Kr, X)π+/π-, E ∼ 1 GeV/nucleon; measured reaction products; deduced multiplicity and probability distribution of charged pions.
doi: 10.1142/S0218301319500587
2019RA21 Nucl.Phys. A990, 149 (2019) N.Rani, P.Singh, M.Singh, R.Kumar, R.Kumar, R.Kharab Influence of coupling of excited states and of deuteron transfer on fusion reactions induced by 6, 7Li on 64Ni, 152Sm and 209Bi targets
doi: 10.1016/j.nuclphysa.2019.07.007
2019SI04 Nucl.Phys. A982, 319c (2019) M.Singh, C.Shen, S.McDonald, S.Jeon, C.Gale Hydrodynamic Fluctuations in Relativistic Heavy-Ion Collisions
doi: 10.1016/j.nuclphysa.2018.10.061
2019SI35 Int.J.Mod.Phys. E28, 1950063 (2019) M.K.Singh, U.Singh, N.Bhatnagar, V.Singh Projectile fragmentation study in peripheral collision for the interaction of the 84Kr with nuclear emulsion at relativistic energy NUCLEAR REACTIONS Ag, Br(84Kr, X), E ∼ 1 GeV/nucleon; measured reaction products; deduced multiplicity distribution of single-charged, double-charged and multi-charged projectile fragments in peripheral events.
doi: 10.1142/S0218301319500630
2019YO03 Phys.Rev. C 100, 031302(R) (2019) R.Yokoyama, R.Grzywacz, B.C.Rasco, N.Brewer, K.P.Rykaczewski, I.Dillmann, J.L.Tain, S.Nishimura, D.S.Ahn, A.Algora, J.M.Allmond, J.Agramunt, H.Baba, S.Bae, C.G.Bruno, R.Caballero-Folch, F.Calvino, P.J.Coleman-Smith, G.Cortes, T.Davinson, C.Domingo-Pardo, A.Estrade, N.Fukuda, S.Go, C.J.Griffin, J.Ha, O.Hall, L.J.Harkness-Brennan, J.Heideman, T.Isobe, D.Kahl, M.Karny, T.Kawano, L.H.Khiem, T.T.King, G.G.Kiss, A.Korgul, S.Kubono, M.Labiche, I.Lazarus, J.Liang, J.Liu, G.Lorusso, M.Madurga, K.Matsui, K.Miernik, F.Montes, A.I.Morales, P.Morrall, N.Nepal, R.D.Page, V.H.Phong, M.Piersa, M.Prydderch, V.F.E.Pucknell, M.M.Rajabali, B.Rubio, Y.Saito, H.Sakurai, Y.Shimizu, J.Simpson, M.Singh, D.W.Stracener, T.Sumikama, R.Surman, H.Suzuki, H.Takeda, A.Tarifeno-Saldivia, S.L.Thomas, A.Tolosa-Delgado, M.Wolinska-Cichocka, P.J.Woods, X.X.Xu Strong one-neutron emission from two-neutron unbound states in β decays of the r-process nuclei 86, 87Ga RADIOACTIVITY 84,85,86,87Ga(β-), (β-n), (β-2n)[from 9Be(238U, F), E=345 MeV/nucleon, followed by separation and identification of fragments using the BigRIPS in-flight separator at RIBF-RIKEN facility]; measured secondary ions implanted into active stoppers made of double-sided silicon-strip detectors (DSSSDs), neutrons by BRIKEN array of 3He counters, WAS3ABi for β and ion detection, and γ rays by two clover-type HPGe detectors, (ions)βn-coin, half-lives of decays of 84,85,86,87Ga; deduced decay curves, %β-n (P1n) and %β-2n (P2n). Comparison with shell-model and QRPA calculations. Relevance to r-process modeling.
doi: 10.1103/PhysRevC.100.031302
2018SO16 Phys.Rev. C 98, 024602 (2018) A.Sonay, M.Deniz, H.T.Wong, M.Agartioglu, G.Asryan, J.H.Chen, S.Kerman, H.B.Li, J.Li, F.K.Lin, S.T.Lin, B.Sevda, V.Sharma, L.Singh, M.K.Singh, M.K.Singh, V.Singh, A.K.Soma, S.W.Yang, Q.Yue, I.O.Yildirim, M.Zeyrek, for the TEXONO Collaboration Neutron background measurements with a hybrid neutron detector at the Kuo-Sheng Reactor Neutrino Laboratory RADIOACTIVITY 212Bi(β-)[from 232Th decay in the background]; 212,218Po, 222Rn(α)[from 232Th and 238U in the background]; measured βα-coin and αα-coin events. 232Th, 238U; estimated contributions from their decays in the background spectra for neutrino measurements. 68Ga, 68,71Ge(EC)[from thermal neutron capture in 70Ge]; measured Eγ and Iγ; deduced contribution to background spectra of neutrino measurements. In situ measurements of neutron-induced background at the Kuo-Sheng Reactor Neutrino Laboratory (KSNL) using a Hybrid Neutron Detector (HND), with and without cosmic ray and anti-Compton veto detectors, and under identical active and passive shielding configurations for the neutrino measurements.
doi: 10.1103/PhysRevC.98.024602
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
2015SI17 Phys.Atomic Nuclei 78, 720 (2015) Effects of first-order correction to eikonal approximation in the analysis of 9Be(15C, 14C + n)9Be stripping reaction NUCLEAR REACTIONS 9Be(15C, n14C), E=54 MeV/nucleon; calculated eikonal phases, longitudinal momentum distribution of 14C. Comparison with available data.
doi: 10.1134/S1063778815050142
2014SI07 Phys.Atomic Nuclei 77, 206 (2014) Contribution of electric quadrupole and dipole-quadrupole interference terms in Coulomb breakup of 15C NUCLEAR REACTIONS 181Ta(15C, 14C), E=85 MeV/nucleon; Pb(15C, 14C), E=68 MeV/nucleon; analyzed available data; calculated σ(E), longitudinal momentum distribution.
doi: 10.1134/S1063778814010189
2013KH18 Int.J.Mod.Phys. E22, 1350082 (2013) Analysis of p-4, 6, 8He and p-6, 9, 11Li scattering NUCLEAR REACTIONS 4,6,8He, 6,9,11Li(p, p), E=60, 72 MeV; analyzed available data; calculated σ(θ), polarization. Coulomb modified Glauber model, comparison with available data.
doi: 10.1142/S0218301313500821
2013SI01 Nucl.Phys. A897, 179 (2013) Analysis of fusion excitation functions of various systems using modified Woods-Saxon potential NUCLEAR REACTIONS 46,48,50Ti(40Ca, X), E(cm)=53-85 MeV;60Ni(50Ti, X), E(cm)=72-95 MeV;64Ni(46Ti, X), E(cm)=72-95 MeV;90Zr(40Ca, X), E(cm)=93-112 MeV;(48Ca, X), E(cm)=91-113 MeV;(46Ti, X), E(cm)=100-120 MeV;(50Ti, X), E(cm)=100-120 MeV;154Sm(16O, X), E(cm)=52-100 MeV;calculated fusion σ using CC code CCFULL; deduced parameters of Woods-Saxon nuclear potential using published data on these reactions.
doi: 10.1016/j.nuclphysa.2012.11.007
2013SI02 Nucl.Phys. A897, 198 (2013) Analysis of fusion excitation function data by using an energy dependent potential model NUCLEAR REACTIONS 54Fe(58Ni, X), E(cm)=65-105 MeV;70Ge(16O, X), E(cm)=30-55 MeV;70Ge(27Al, X), E(cm)=50-60 MeV;70Ge(37Cl, X), E(cm)=62-77 MeV;72Ge(16O, X), E(cm)=30-53 MeV;72Ge(27Al, X), E(cm)=50-60 MeV;72Ge(37Cl, X), E(cm)=62-77 MeV;74Ge(16O, X), E(cm)=30-60 MeV;74Ge(27Al, X), E(cm)=48-63 MeV;74Ge(37Cl, X)E(cm)=63-75 MeV;76Ge(16O, X), E(cm)=30-60 MeV;76Ge(27Al, X), E(cm)=48-63 MeV;76Ge(37Cl, X), E(cm)=63-77 MeV;90Zr(40Ca, X), E not given;90Zr(48Ca, X), E(cm)=90-115 MeV;92Zr(16O, X), E(cm)=35-70 MeV;92Zr(28Si, X), E(cm)=65-90 MeV;96Zr(48Ca, X), E(cm)=85-115 MeV;186W(16O, X), E(cm)=60-95 MeV;144,148Sm(16O, X), E(cm)=55-95 MeV;208Pb(16O, X), E(cm)=70-115 MeV;calculated fusion σ using Wong's formula and energy dependent potential; deduced potential parameters.
doi: 10.1016/j.nuclphysa.2012.11.002
2013SI24 Can.J.Phys. 91, 777 (2013) Y.Singh, S.K.Dhiman, M.Singh, C.Bihari, A.K.Varshney, K.K.Gupta, D.K.Gupta In search of empirical rule relating E2+1 and B(E2; 0+1 → 2+1) in asymmetric even-even nuclei of mass region A = 90-120
doi: 10.1139/cjp-2013-0107
2012DU13 Int.J.Mod.Phys. E21, 1250054 (2012) Effects of nuclear induced breakup on the fusion of 6Li + 12C and 6He + 12C systems around barrier energies NUCLEAR REACTIONS 12C(6Li, X), (6He, X), E not given; calculated fusion σ. Dynamic polarization potential approach.
doi: 10.1142/S0218301312500541
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
2011VA01 Phys.Scr. 83, 015201 (2011) M.Varshney, M.Singh, Y.Singh, C.Bihari, A.K.Varshney, K.K.Gupta, D.K.Gupta Seeking asymmetric rotors in mass region A ∼ 100-110 NUCLEAR STRUCTURE 98,100,102,104,106,108,110,112Ru, 108,110,112,114,116Pd, 86,94,100,102,104,106,108Mo; calculated asymmetry parameters, ground and γ-band levels, staggering index. Comparison with experimental data.
doi: 10.1088/0031-8949/83/01/015201
2009KH07 Nucl.Technology 168, 381 (2009) Shielding Analysis for X-Ray Sources Generated in Target Chamber of the National Ignition Facility
doi: 10.13182/NT09-A9213
2008BI08 Phys.Scr. 77, 055201 (2008) C.Bihari, M.Singh, Y.Singh, A.K.Varshney, K.K.Gupta, D.K.Gupta A new signature of the triaxial region in even nuclei NUCLEAR STRUCTURE 104Ru, 106Ru, 108Ru, 110Ru, 112Ru, 108Pd, 110Pd, 112Pd, 114Pd, 116Pd, 120Xe, 122Xe, 124Xe, 126Xe, 128Xe, 130Xe, 124Ba, 126Ba, 128Ba, 130Ba, 132Ba, 152Sm, 152Gd, 154Gd, 156Gd, 158Gd, 154Dy, 156Dy, 158Dy, 160Dy, 162Dy, 164Dy, 162Er, 164Er, 166Er, 168Er, 182Os, 184Os, 186Os, 182Os; analyzed yrast γ-band level energies; deduced parameters; 104Ru, 106Ru, 108Ru, 110Ru, 112Ru, 108Pd, 110Pd, 112Pd, 114Pd, 116Pd, 120Xe, 122Xe, 124Xe, 126Xe, 128Xe, 130Xe, 124Ba, 126Ba, 128Ba, 130Ba, 132Ba, 152Sm, 152Gd, 154Gd, 156Gd, 158Gd, 154Dy, 156Dy, 158Dy, 160Dy, 162Dy, 164Dy, 162Er, 164Er, 166Er, 168Er, 182Os, 184Os, 186Os, 182Os; calculated levels, J, π, γ-parameter. Two parameter formula, compared with phenomenologial asymmetric rotor model.
doi: 10.1088/0031-8949/77/05/055201
2008BI13 Phys.Scr. 78, 045201 (2008) C.Bihari, Y.Singh, M.Singh, A.K.Varshney, K.K.Gupta, D.K.Gupta Evidence of rigid triaxiality in some even nuclei NUCLEAR STRUCTURE 136,138Nd, 150Sm, 164,166,168,170Yb, 176,178Hf, 180,182,184W, 180,190,192Os, 182,184,188,190,192,194Pt, 232Th; calculated γ-band energies. 130Ba, 152Sm, 154,156Gd, 156,158Dy, 164,166Er, 166,170Yb, 180W, 182Os, 232Th; calculated γ-band staggering indices.
doi: 10.1088/0031-8949/78/04/045201
2007KH12 Int.J.Mod.Phys. E16, 1741 (2007) Proton-nucleus elastic scattering at ∼ 1 GeV and the NN amplitude NUCLEAR REACTIONS 4He, 12C, 16O, 40Ca(p, p), E=1 GeV; analyzed σ, angular distributions and polarization data using the Glauber formalism.
doi: 10.1142/S0218301307006915
2007SI12 Radiat.Meas. 42, 420 (2007) M.Singh, G.Singh, B.S.Sandhu, B.Singh Angular distribution of 662 keV multiply-Compton scattered gamma rays in copper NUCLEAR REACTIONS Cu(γ, γ'), E=662 keV; measured angular distribution and saturation depth in copper of multiply-Compton scattered γ rays.
doi: 10.1016/j.radmeas.2007.01.037
2007VA04 Phys.Scr. 75, 451 (2007) M.Varshney, C.Bihari, Y.Singh, M.Singh, A.K.Varshney, K.K.Gupta, D.K.Gupta An empirical relation for rotational energies in neutron rich transitional nuclei around A ≈ 100 NUCLEAR STRUCTURE 104,106,108,110,112Ru, 108,110,112,114,116Pd; calculated rotational band level energies. Rigid triaxial rotor model.
doi: 10.1088/0031-8949/75/4/014
2005KH14 Int.J.Mod.Phys. E14, 787 (2005) Proton-4He elastic scattering at ∼ 1 GeV NUCLEAR REACTIONS 1n, 1H(p, p), E ≈ 1 GeV; analyzed σ(θ), polarization observables; deduced parameters. 4He(p, p), E ≈ 1 GeV; calculated σ(θ), polarization observables. Glauber model.
doi: 10.1142/S0218301305003557
1996KA55 Nucl.Instrum.Methods Phys.Res. A372, 311 (1996) D.O.Kataria, J.J.Das, N.Madhavan, P.Sugathan, A.K.Sinha, G.Dayanand, M.C.Radhakrishna, A.M.Vinodkumar, K.M.Varier, M.Singh, N.V.S.V.Prasad A Modular Focal Plane Detector System for the Heavy Ion Reaction Analyzer at NSC, New Delhi NUCLEAR REACTIONS 48Ti(32S, X), E=80 MeV; 68Zn(28Si, X), E=78 MeV; 60Ni(48Ti, X), E=160 MeV; 27Al(28Si, X), E=150 MeV; measured evaporation residue energy spectra; deduced detector characteristics. Low pressure multi-wire proportional counter plus split anode ionization detector.
doi: 10.1016/0168-9002(95)01242-7
1994DH01 J.Phys.(London) G20, 135 (1994) A.S.Dhaliwal, M.S.Powar, M.Singh Internal Bremsstrahlung Spectra of 170Tm and 89Sr RADIOACTIVITY 170Tm(β-); 89Sr(β-); measured internal bremsstrahlung spectra. Models comparison.
doi: 10.1088/0954-3899/20/1/013
1993DH03 Phys.Rev. A48, 1308 (1993) A.S.Dhaliwal, M.S.Powar, M.Singh Thick-Target External-Bremsstrahlung Spectra of 147Pm and 35S β Rays NUCLEAR REACTIONS 27Al, Cu, Sn, Pb(e-, γ), E ≤ 167 keV; measured external bremsstrahlung spectra. Models comparison. Soft β-particles from 147Pm, 35S decay. ATOMIC PHYSICS 27Al, Cu, Sn, Pb(e-, γ), E ≤ 167 keV; measured external bremsstrahlung spectra. Models comparison. Soft β-particles from 147Pm, 35S decay.
doi: 10.1103/PhysRevA.48.1308
1992SI24 Appl.Radiat.Isot. 43, 907 (1992) Energy Dependence of Total Photon Attenuation Coefficients of Composite Materials
doi: 10.1016/0883-2889(92)90154-7
1991DH01 Appl.Radiat.Isot. 42, 427 (1991) A.S.Dhaliwal, M.S.Powar, M.Singh Attenuation of 203Tl and 32P Beta Ray Bremsstrahlung in Thick Targets of Al, Cu, Sn and Pb NUCLEAR REACTIONS 27Al, Cu, Sn, Pb(γ, X), E=radioactive source; measured β-ray bremsstrahlung attenuation.
doi: 10.1016/0883-2889(91)90100-F
1991DH02 Nuovo Cim. 104A, 121 (1991) A.S.Dhaliwal, M.S.Powar, M.Singh Study of Bremsstrahlung Spectra Excited by 170Tm Beta-Particles in Thick Targets NUCLEAR REACTIONS 27Al, Cu, Sn, Pb(e, γ), E=0.97 MeV; measured external bremsstrahlung spectra. Thick targets, 170Tm β-particles.
doi: 10.1007/BF02822272
1990DH01 Nucl.Instrum.Methods Phys.Res. B47, 370 (1990) A.S.Dhaliwal, M.S.Powar, M.Singh External Bremsstrahlung Spectra of Al, Cu, Sn and Pb Targets Excited by 32P Beta Particles NUCLEAR REACTIONS 27Al, Cu, Sn, Pb(e, γ), E ≈ 1.706 MeV; measured external bremsstrahlung spectra. β- particles from 32P-decay. ATOMIC PHYSICS 27Al, Cu, Sn, Pb(e, γ), E ≈ 1.706 MeV; measured external bremsstrahlung spectra. β- particles from 32P-decay.
doi: 10.1016/0168-583X(90)90614-Z
1990DH02 Nucl.Instrum.Methods Phys.Res. B51, 339 (1990) A.S.Dhaliwal, M.S.Powar, M.Singh Spectral Distribution of External Bremsstrahlung in Thick Targets of Al, Cu, Sn and Pb Excited by Beta Particles of 204Tl NUCLEAR REACTIONS 27Al, Cu, Sn, Pb(e, γ), E=0.766 MeV; measured external bremsstrahlung spectra. Thick targets, β-particles from 204Tl. ATOMIC PHYSICS 27Al, Cu, Sn, Pb(e, γ), E=0.766 MeV; measured external bremsstrahlung spectra. Thick targets, β-particles from 204Tl.
doi: 10.1016/0168-583X(90)90551-5
1976PO04 J.Phys.(London) G2, 43 (1976) Internal Bremsstrahlung Spectra of the Allowed Beta Emitters 32P, 35S and 45Ca RADIOACTIVITY 32P, 35S, 45Ca; measured IB spectra.
doi: 10.1088/0305-4616/2/1/006
1976PO10 Curr.Sci.(India) 45, 131 (1976) Photon Yield and Energy in Internal Bremsstrahlung RADIOACTIVITY 32P, 35S, 45Ca, 90Y, 204Tl; measured γ-yield, IBS.
1975PO06 J.Phys.(London) G1, 453 (1975) Measurement of the Internal Bremsstrahlung Spectrum of 90Y RADIOACTIVITY 90Y; measured IBS, photon yield.
doi: 10.1088/0305-4616/1/4/010
1972DE01 Nucl.Phys. A178, 417 (1972) R.M.Devries, J.W.Sunier, J.-L.Perrenoud, M.Singh, G.Paic, I.Slaus Measurement of the (p, α) Reactions on 9Be and 11B at 45 MeV NUCLEAR REACTIONS 9Be(p, α)6Li, 11B(p, α)8Be, Ep=45.0 MeV; measured σ(θ=20-160° cms). Natural targets.
doi: 10.1016/0375-9474(72)90469-1
1972PO03 J.Phys.(London) A5, 460 (1972) Contribution of Detour Transitions to Internal Bremsstrahlung Spectrum Of 204Tl RADIOACTIVITY 204Tl; measured IB spectrum.
doi: 10.1088/0305-4470/5/3/015
1972SI28 Nucl.Phys. A193, 449 (1972) M.Singh, J.W.Sunier, R.M.Devries, G.E.Thompson Decay of the Light Antimony Isotopes 110,111,112,113,114Sb Following the 112,114Sn(p, xn) Reactions RADIOACTIVITY 110,111,112,113,114Sb[from 112,114Sn(p, xn)]; measured T1/2, Eγ, Eβ, βγ-, γγ-coin; deduced Q, log ft. 110,111,112,113,114Sn deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(72)90332-6
1972SI56 Nuovo Cim. B 8, 261 (1972) L-shell photoelectric cross-sections for heavy atoms at 145 and 279 keV NUCLEAR REACTIONS Hg, Au, Tl, Pb, Bi, Th, U(γ, E), E=145, 279 keV; measured reaction products, X-rays; deduced σ using measurement of the total intensity of fluorescent L X-rays that follow the photoelectric absorption and fluorescent L X-ray detector. Comparison with theoretical predictions of Schmickley and Pratt.
doi: 10.1007/bf02743521
1970DE17 Phys.Lett. 32B, 193 (1970) R.M.Devries, G.Paic, J.L.Perrenoud, M.Singh, J.W.Sunier A Study of the Reactions (p, 6Li) and (p, 6He) on 9Be at 45 MeV NUCLEAR REACTIONS 9Be(p, 6Li), (p, 6He), E=45 MeV; measured σ(E(6Li), θ), σ(E(6He), θ).
doi: 10.1016/0370-2693(70)90471-5
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