NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.Mishra Found 28 matches. 2021LA06 Phys.Rev. C 104, L011301 (2021) Md.S.R.Laskar, R.Palit, E.Ideguchi, T.Inakura, S.N.Mishra, F.S.Babra, S.Bhattacharya, D.Choudhury, B.Das, B.Das, P.Dey, U.Garg, A.K.Jain, A.Kundu, D.Kumar, D.Negi, S.C.Pancholi, S.Rajbanshi, S.Sihotra Enhanced B(E3) strength observed in 137La NUCLEAR REACTIONS 130Te(11B, 4n)137La, E=40 MeV; measured Eγ, Iγ, γγ-coin, level half-life by γγ(t) using an array of 11 Compton-suppressed HPGe clover and 14 LaBr3(Ce) detectors at the Pelletron Linac Facility of TIFR-Mumbai. 137La; deduced levels, J, π, half-life of 1005, 11/2- level, B(E3), sudden increase of B(E3) strength at N=80. Comparison with random-phase approximation (RPA) calculations. Systematics of B(E3) strengths in 129,133La and 132,134,136,138Ba.
doi: 10.1103/PhysRevC.104.L011301
2020LA06 Phys.Rev. C 101, 034315 (2020) Md.S.R.Laskar, R.Palit, S.N.Mishra, N.Shimizu, Y.Utsuno, E.Ideguchi, U.Garg, S.Biswas, F.S.Babra, R.Gala, C.S.Palshetkar, Z.Naik Structure of the 11/2- isomeric state in 133La NUCLEAR REACTIONS 126Te(11B, 4n)133La, E=52 MeV; measured Eγ, Iγ, spin precession, g factor of the 11/2- isomeric state in 133La by time differential perturbed angular distribution (TDPAD) technique, and its half-life by γ(t) at the Pelletron Linac Facility of BARC-TIFR. 133La; deduced levels, J, π, spectroscopic quadrupole moment, β2. Analysis of spin rotation data by magnetic dipole and electric quadrupole hyperfine interactions. Comparison with large scale shell model calculations.
doi: 10.1103/PhysRevC.101.034315
2019LA01 Phys.Rev. C 99, 014308 (2019) Md.S.R.Laskar, S.Saha, R.Palit, S.N.Mishra, N.Shimizu, Y.Utsuno, E.Ideguchi, Z.Naik, F.S.Babra, S.Biswas, S.Kumar, S.K.Mohanta, C.S.Palshetkar, P.Singh, P.C.Srivastava g-factor measurement of the 2738 keV isomer in 135La NUCLEAR REACTIONS 128Te(11B, 4n), E=52 MeV; measured delayed γ spectra, g factor by hyperfine interactions using TDPAD technique, half-life of the 23/2+ nanosecond isomer at the heavy-ion accelerator facility of TIFR, Mumbai. 135La; deduced level, configuration. Comparison with large-scale shell model calculations with SNV interaction. NUCLEAR MOMENTS 135La; measured g factor of the 2738-keV, 23/2+ isomer by hyperfine interactions using TDPAD technique, using 128Te(11B, 4n) reaction. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.99.014308
2017MI13 Pramana 89, 22 (2017) Ab-initio calculations of electric field gradient in Ru compounds and their implication on the nuclear quadrupole moments of 99Ru and 101Ru NUCLEAR STRUCTURE 99,101Ru; calculated nuclear quadrupole moments for the ground and first excited states. The ab-initio calculations of electric field gradient, comparison with available data.
doi: 10.1007/s12043-017-1425-9
2015KA16 Phys.Rev. A 91, 053852 (2015) Y.B.Kale, S.R.Mishra, V.B.Tiwari, S.Singh, H.S.Rawat Resolution of hyperfine transitions in metastable 83Kr using electromagnetically induced transparency ATOMIC PHYSICS 83Kr; measured electromagnetically induced transparency signals; deduced hyperfine transitions, the magnetic hyperfine constant and the electric quadrupole hyperfine constant.
doi: 10.1103/PhysRevA.91.053852
2013ZI01 Acta Phys.Pol. B44, 651 (2013) M.Zieblinski, M.Jastrzab, N.Dokania, V.Nanal, S.Brambilla, P.Bednarczyk, M.Ciemala, E.Dutkiewicz, M.Kmiecik, M.Krzysiek, J.Lekki, A.Maj, Z.Szklarz, B.Wasilewska, M.Dudelo, K.Hadynska-Klek, P.Napiorkowski, B.Genolini, Ch.Schmitt, W.Catford, M.Nakhostin, N.Yavuzkanat, O.Dorvaux, R.G.Pillay, M.S.Pose, S.Mishra, S.Mathimalar, V.Singh, N.Katyan, D.R.Chakrabarty, V.M.Datar, S.Kumar, G.Mishra, S.Mukhopadhyay, D.Pandit, S.Erturk Testing of the PARIS LaBr3-NaI Phoswich Detector with High Energy Gamma-rays
doi: 10.5506/APhysPolB.44.651
2008MI17 Phys.Rev. C 78, 024307 (2008) S.Mishra, A.Shukla, R.Sahu, V.K.B.Kota Deformed shell model calculations of half lives for β+/EC decay and 2ν β+ β+ β+EC/ECEC decay in medium-heavy N ∼ Z nuclei RADIOACTIVITY 64,66,68,70Ge, 68,70,72,74Se, 76,78,80,82Sr, 72,74,76Kr(β+)(EC); 78Kr(β+)(EC)(2β+)(β+EC)(2EC); calculated half-lives, Gamow-Teller strength distributions. Deformed-shell model based on Hartree-Fock states. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.024307
2007MI18 Can.J.Phys. 85, 269 (2007) S.Mishra, K.C.Tripathy, R.Sahu Collective bands in 80, 82Kr NUCLEAR STRUCTURE 80,82Kr; calculated level energies, J, π and B(E2) using deformed shell model to study the structure of collective bands.
doi: 10.1139/P07-047
2007MI20 Prog.Theor.Phys.(Kyoto) 118, 59 (2007) Deformed Shell Model for T = 1/2 Bands in 51Mn NUCLEAR STRUCTURE 51Mn; calculated level energies and B(E2) using deformed configuration mixing shell model.
doi: 10.1143/PTP.118.59
2006TR04 Pramana 66, 389 (2006) K.C.Tripathy, R.Sahu, S.Mishra Microscopic study of low-lying collective bands in 77Kr NUCLEAR STRUCTURE 77Kr; calculated levels, J, π, configurations, rotational bands, B(M1), B(E2). Deformed shell model.
doi: 10.1007/BF02704392
2000PA57 Phys.Rev. C62, 055802 (2000) Effects of Vacuum Structure on Neutron Stars
doi: 10.1103/PhysRevC.62.055802
2000TA05 Nucl.Phys. A663-664, 344c (2000) B.H.Tamminga, T.Adams, A.Alton, C.G.Arroyo, S.Avvakumov, L.de Barbaro, P.de Barbaro, A.O.Bazarko, R.H.Bernstein, A.Bodek, T.Bolton, J.Brau, D.Buchholz, H.Budd, L.Bugel, J.Conrad, R.B.Drucker, J.A.Formaggio, R.Frey, J.Goldman, M.Goncharov, D.A.Harris, R.A.Johnson, J.H.Kim, B.J.King, T.Kinnel, S.Koutsoliotas, M.J.Lamm, W.Marsh, D.Mason, K.S.McFarland, C.McNulty, S.R.Mishra, D.Naples, P.Nienaber, A.Romosan, W.K.Sakumoto, H.Schellman, F.J.Sciulli, W.G.Seligman, M.H.Shaevitz, W.H.Smith, P.Spentzouris, E.G.Stern, M.Vakili, A.Vaitaitis, V.Wu, U.K.Yang, J.Yu, G.P.Zeller, E.D.Zimmerman Low-Q2 Low-x Structure Function Analysis of CCFR Data for F2
doi: 10.1016/S0375-9474(99)00613-2
2000VA01 Phys.Rev. D61, 052003 (2000) M.Vakili, C.G.Arroyo, P.Auchincloss, L.de Barbaro, P.de Barbaro, A.O.Bazarko, R.H.Bernstein, A.Bodek, T.Bolton, H.Budd, J.Conrad, D.A.Harris, R.A.Johnson, J.H.Kim, B.J.King, T.Kinnel, G.Koizumi, S.Koutsoliotas, M.J.Lamm, W.C.Lefmann, W.Marsh, K.S.McFarland, C.McNulty, S.R.Mishra, D.Naples, P.Nienaber, M.J.Oreglia, L.Perera, P.Z.Quintas, A.Romosan, W.K.Sakumoto, B.A.Schumm, F.J.Sciulli, W.G.Seligman, M.H.Shaevitz, W.H.Smith, P.Spentzouris, R.Steiner, E.G.Stern, U.K.Yang, J.Yu Nuclear Structure Functions in the Large-x Large-Q2 Kinematic Region in Neutrino Deep Inelastic Scattering NUCLEAR REACTIONS Fe(ν, μ), E not given; analyzed Bjorken x distributions; deduced nuclear effects at large x.
doi: 10.1103/PhysRevD.61.052003
1998KI16 Phys.Rev.Lett. 81, 3595 (1998) J.H.Kim, D.A.Harris, C.G.Arroyo, L.de Barbaro, P.de Barbaro, A.O.Bazarko, R.H.Bernstein, A.Bodek, T.Bolton, H.Budd, J.Conrad, R.A.Johnson, B.J.King, T.Kinnel, M.J.Lamm, W.C.Lefmann, W.Marsh, K.S.McFarland, C.McNulty, S.R.Mishra, D.Naples, P.Z.Quintas, A.Romosan, W.K.Sakumoto, H.Schellman, F.J.Sciulli, W.G.Seligman, M.H.Shaevitz, W.H.Smith, P.Spentzouris, E.G.Stern, M.Vakili, U.K.Yang, J.Yu Measurement of αs(Q2) from the Gross-Llewellyn Smith Sum Rule NUCLEAR REACTIONS Fe(ν, X), E not given; analyzed data; deduced strong coupling constant. Gross-Llewellyn Smith sum rule, deep-inelastic scattering.
doi: 10.1103/PhysRevLett.81.3595
1997SE08 Phys.Rev.Lett. 79, 1213 (1997) W.G.Seligman, C.G.Arroyo, L.de Barbaro, P.de Barbaro, A.O.Bazarko, R.H.Bernstein, A.Bodek, T.Bolton, H.Budd, J.Conrad, D.A.Harris, R.A.Johnson, J.H.Kim, B.J.King, T.Kinnel, M.J.Lamm, W.C.Lefmann, W.Marsh, K.S.McFarland, C.McNulty, S.R.Mishra, D.Naples, P.Z.Quintas, A.Romosan, W.K.Sakumoto, H.Schellman, F.J.Sciulli, M.H.Shaevitz, W.H.Smith, P.Spentzouris, E.G.Stern, M.Vakili, U.K.Yang, J.Yu Improved Determination of α(s) from Neutrino-Nucleon Scattering NUCLEAR REACTIONS Fe(ν, X), E=30-360 GeV; analyzed data; deduced strong coupling constant α(s)(M(Z)2). 1H deduced F2, xF3 structure functions.
doi: 10.1103/PhysRevLett.79.1213
1996DA02 Phys.Rev. C53, 1009 (1996) P.Das, R.G.Pillay, V.V.Krishnamurthy, S.N.Mishra, S.H.Devare g-Factor Measurement of 132Ba in the Backbending Region NUCLEAR REACTIONS 124Sn(12C, 4n), E=60 MeV; measured γ(θ, H, t). 132Ba level deduced g factor, configuration.
doi: 10.1103/PhysRevC.53.1009
1996TU03 Phys.Rev. C54, 2904 (1996) A.A.Tulapurkar, P.Das, S.N.Mishra, R.G.Pillay, J.A.Sheikh Lifetime and g-Factor Measurements of the 11- Isomer in 92Tc NUCLEAR REACTIONS 68Zn(28Si, 3np), E=100 MeV; measured γγ-coin, Iγ(θ, t). 92Tc deduced isomer T1/2, g factor, configuration. Shell model.
doi: 10.1103/PhysRevC.54.2904
1996YA06 J.Phys.(London) G22, 775 (1996) U.K.Yang, P.Auchincloss, P.de Barbaro, A.Bodek, H.Budd, D.A.Harris, W.K.Sakumoto, W.C.Lefmann, R.Steiner, M.J.Oreglia, B.A.Schumm, R.A.Johnson, M.Nussbaum, L.Perera, M.Vakili, G.Arroyo, A.O.Bazarko, J.Conrad, J.H.Kim, B.J.King, S.Koutsoliotas, C.McNulty, S.R.Mishra, P.Z.Quintas, A.Romosan, F.J.Sciulli, W.G.Seligman, M.H.Shaevitz, P.Spentzouris, E.G.Stern, R.H.Bernstein, G.Koizumi, M.J.Lamm, W.Marsh, K.S.McFarland, T.Bolton, W.B.Lowery, D.Naples, R.B.Drucker, T.Kinnel, W.H.Smith, P.Nienaber A Measurement of R = σ(L)/σ(T) in Deep Inelastic Neutrino-Nucleon Scattering at the Tevatron
1995MC04 Phys.Rev.Lett. 75, 3993 (1995) K.S.McFarland, D.Naples, C.G.Arroyo, P.Auchincloss, P.de Barbaro, A.O.Bazarko, R.H.Bernstein, A.Bodek, T.Bolton, H.Budd, J.Conrad, R.B.Drucker, D.A.Harris, R.A.Johnson, J.H.Kim, B.J.King, T.Kinnel, G.Koizumi, S.Koutsoliotas, M.J.Lamm, W.C.Lefmann, W.Marsh, C.McNulty, S.R.Mishra, P.Nienaber, M.Nussbaum, M.J.Oreglia, L.Perera, P.Z.Quintas, A.Romosan, W.K.Sakumoto, B.A.Schumm, F.J.Sciulli, W.G.Seligman, M.H.Shaevitz, W.H.Smith, P.Spentzouris, R.Steiner, E.G.Stern, M.Vakili, U.K.Yang Limits on ν(μ)((ν-bar)(μ)) → ν(τ)((ν-bar)(τ)) and ν(μ)((ν-bar)(μ)) → ((ν-bar)(e))ν(e) Oscillations from a Precision Measurement of Neutrino-Nucleon Neutral Current Interactions
doi: 10.1103/PhysRevLett.75.3993
1994AR09 Phys.Rev.Lett. 72, 3452 (1994) C.G.Arroyo, B.J.King, K.T.Bachmann, A.O.Bazarko, T.Bolton, C.Foudas, W.C.Lefmann, W.C.Leung, S.R.Mishra, E.Oltman, P.Z.Quintas, S.A.Rabinowitz, F.J.Sciulli, W.G.Seligman, M.H.Shaevitz, F.S.Merritt, M.J.Oreglia, B.A.Schumm, R.H.Bernstein, F.Borcherding, H.E.Fisk, M.J.Lamm, W.Marsh, K.W.B.Merritt, H.M.Schellman, D.D.Yovanovitch, A.Bodek, H.S.Budd, P.de Barbaro, W.K.Sakumoto, T.Kinnel, P.H.Sandler, W.H.Smith Precise Measurement of the Weak Mixing Angle in Neutrino-Nucleon Scattering
doi: 10.1103/PhysRevLett.72.3452
1994KR01 Phys.Rev. C49, 705 (1994) V.V.Krishnamurthy, S.N.Mishra, R.G.Pillay, S.H.Devare, H.G.Devare, J.A.Sheikh Nuclear g-Factor Measurement for the (21/2)+ Isomeric State in 89Nb NUCLEAR REACTIONS 66Zn(30Si, 2npα), E=115 MeV; measured Eγ, Iγ, γ(t), γ(θ, H, t). 89Nb deduced isomer g-factor, configuration.
doi: 10.1103/PhysRevC.49.705
1993KH10 Hyperfine Interactions 78, 547 (1993) S.Khatua, S.N.Mishra, S.H.Devare, H.G.Devare Formation and Stability of Magnetic Moment on Isolated Rh Impurities in Dilute PtFe Alloys RADIOACTIVITY 100Pd(EC) [from 89Y(16O, 4np)]; measured γγ(θ, H, t); deduced isolated Rh impurities local susceptibilities in dilute Pt(Fe) paramagnetic alloys.
doi: 10.1007/BF00568190
1993KH11 Hyperfine Interactions 78, 553 (1993) S.Khatua, S.N.Mishra, S.H.Devare, H.G.Devare Measurement of Local Susceptibility at 100Rh in Some Metallic Hosts RADIOACTIVITY 100Pd(EC) [from 89Y(16O, 4np), E=95 MeV]; measured γγ(θ, H, t); deduced isolated Rh impurities local susceptibilities in Pb, Ru, Au, Pd, Pt, Yb hosts.
doi: 10.1007/BF00568191
1993KR26 Hyperfine Interactions 78, 541 (1993) V.V.Krishnamurthy, S.N.Mishra, R.Kumar, S.H.Devare, H.G.Devare Local Magnetism of Rh in Ni-Rh Alloys Near the Critical Composition for Ferromagnetism RADIOACTIVITY 100Pd(EC) [from 89Y(16O, 4np), E=95 MeV]; measured γγ(θ, H, t); deduced isolated Rh local magnetism in Ni-Rh alloys near ferromagnetism critical composition.
doi: 10.1007/BF00568189
1993KR29 Hyperfine Interactions 80, 1005 (1993) V.V.Krishnamurthy, S.N.Mishra, S.H.Devare, H.G.Devare, S.Ramakrishan, V.Srinivas, G.Chandra TDPAC Measurement of Quadrupole Interaction at 111Cd in the Nearly Heavy Fermion System USn(2.9) RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced quadrupole interaction at 111Cd probe in USn(2.9).
doi: 10.1007/BF00567455
1987MI22 Hyperfine Interactions 34, 373 (1987) S.N.Mishra, S.H.Devare, H.G.Devare Magnetic Behaviour of Eu(x)(Rh(1-y)Fe(y))3B2; x = 0.6, 0.75, 1.04 and y = 0.02 NUCLEAR REACTIONS 151Eu(γ, γ), E=21.54 keV; measured Mossbauer emission spectra. 151Eu deduced isomer shift temperature dependence. Ternary bromide alloys.
doi: 10.1007/BF02072738
1983MI03 Phys.Lett. 94A, 317 (1983) S.N.Mishra, R.G.Pillay, P.N.Tandon, H.G.Devare Quadrupole Interactions at 111Cd Nuclei in Light Rare Earths RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced quadrupole interaction at 111Cd in Pr, Nd hosts.
doi: 10.1016/0375-9601(83)90728-4
1983MI31 Hyperfine Interactions 15/16, 701 (1983) S.N.Mishra, R.G.Pillay, P.N.Tandon, H.G.Devare Quadrupole Interaction at 111Cd in Rare-Earth Intermetallics RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced 111Cd quadrupole interaction in rare earth intermetallics.
doi: 10.1007/BF02147346
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