NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Singh Found 77 matches. 2022CI04 Phys.Rev. C 106, 014317 (2022) A.A.Ciemny, C.Mazzocchi, W.Dominik, A.Fijalkowska, J.Hooker, C.Hunt, H.Jayatissa, L.Janiak, G.Kaminski, E.Koshchiy, M.Pfutzner, M.Pomorski, B.Roeder, G.V.Rogachev, A.Saastamoinen, S.Sharma, N.Sokolowska, W.Satula, J.Singh β-delayed charged-particle decay of 22, 23Si RADIOACTIVITY 22,23Si(β+), (β+p), (β+2p); 23Si(β+3p), (β+α)[22,23Si activities from Ni(28Si, X), E=45 MeV/nucleon at the Texas A and M University K500 superconducting cyclotron, followed by separation of fragments using momentum achromat recoil separator (MARS)]; measured reaction fragments, particle spectra, E(p), I(p) using optical-readout time-projection chamber (OTPC). 23Al, 22Mg, 21Na; deduced levels, J, π. 22Si, 23Si; deduced T1/2 of ground states, and absolute branching ratios for the observed decay modes; calculated Gamow-Teller matrix elements using angular-momentum-projected (AMP) method with DFT-NCCI module. 23Al; calculated levels, J, π using multireference density-functional-rooted (DFT) calculations, and compared with shell-model calculations in literature. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.106.014317
2022DE19 Nucl.Phys. B983, 115903 (2022) P.Deka, J.Singh, N.Sarma, K.Bora Uncertainties in the oscillation parameters measurement due to multi-nucleon effects at NOνA experiment NUCLEAR REACTIONS C(ν, X), (ν-bar, X), E<5 MeV; calculated σ using QE, RPA and 2p2h; deduced multi-nucleon effects impact on uncertainties. Comparison with available data.
doi: 10.1016/j.nuclphysb.2022.115903
2022SI04 Phys.Rev. C 105, 014328 (2022) G.Singh, J.Singh, J.Casal, L.Fortunato Exploring the halo character and dipole response in the dripline nucleus 31F NUCLEAR STRUCTURE 30F; calculated phase shifts. 31F; calculated matter radius, nn distance, core-nn distance, E1 sum rule, contribution by different energy orbitals in different configurations for the ground state, ground state probability density distributions for all the configurations. 19,20,21,22,23,24,25,26,27,28,29,30,31,32F; calculated matter radii. Analytical, transformed harmonic oscillator basis under the aegis of a hyperspherical formalism for the ground-state three-body wave function of 31F, with the nn interaction defined by the Gogny-Pires-Tourreil potential. Comparison with available experimental data.
doi: 10.1103/PhysRevC.105.014328
2022SI21 Nucl.Phys. A1027, 122508 (2022) Pion couplings with low-lying nucleon resonances
doi: 10.1016/j.nuclphysa.2022.122508
2021AB12 Phys.Rev. C 104, L061901 (2021) M.S.Abdallah, B.E.Aboona, J.Adam, L.Adamczyk, J.R.Adams, J.K.Adkins, G.Agakishiev, I.Aggarwal, M.M.Aggarwal, Z.Ahammed, I.Alekseev, D.M.Anderson, A.Aparin, E.C.Aschenauer, M.U.Ashraf, F.G.Atetalla, A.Attri, G.S.Averichev, V.Bairathi, W.Baker, J.G.Ball Cap, K.Barish, A.Behera, R.Bellwied, P.Bhagat, A.Bhasin, J.Bielcik, J.Bielcikova, I.G.Bordyuzhin, J.D.Brandenburg, A.V.Brandin, I.Bunzarov, J.Butterworth, X.Z.Cai, H.Caines, M.Calderon de la Barca Sanchez, D.Cebra, I.Chakaberia, P.Chaloupka, B.K.Chan, F.-H.Chang, Z.Chang, N.Chankova-Bunzarova, A.Chatterjee, S.Chattopadhyay, D.Chen, J.Chen, J.H.Chen, X.Chen, Z.Chen, J.Cheng, M.Chevalier, S.Choudhury, W.Christie, X.Chu, H.J.Crawford, M.Csanad, M.Daugherity, T.G.Dedovich, I.M.Deppner, A.A.Derevschikov, A.Dhamija, L.Di Carlo, L.Didenko, P.Dixit, X.Dong, J.L.Drachenberg, E.Duckworth, J.C.Dunlop, N.Elsey, J.Engelage, G.Eppley, S.Esumi, O.Evdokimov, A.Ewigleben, O.Eyser, R.Fatemi, F.M.Fawzi, S.Fazio, P.Federic, J.Fedorisin, C.J.Feng, Y.Feng, P.Filip, E.Finch, Y.Fisyak, A.Francisco, C.Fu, L.Fulek, C.A.Gagliardi, T.Galatyuk, F.Geurts, N.Ghimire, A.Gibson, K.Gopal, X.Gou, D.Grosnick, A.Gupta, W.Guryn, A.I.Hamad, A.Hamed, Y.Han, S.Harabasz, M.D.Harasty, J.W.Harris, H.Harrison, S.He, W.He, X.H.He, Y.He, S.Heppelmann, S.Heppelmann, N.Herrmann, E.Hoffman, L.Holub, Y.Hu, H.Huang, H.Z.Huang, S.L.Huang, T.Huang, X.Huang, Y.Huang, T.J.Humanic, G.Igo, D.Isenhower, W.W.Jacobs, C.Jena, A.Jentsch, Y.Ji, J.Jia, K.Jiang, X.Ju, E.G.Judd, S.Kabana, M.L.Kabir, S.Kagamaster, D.Kalinkin, K.Kang, D.Kapukchyan, K.Kauder, H.W.Ke, D.Keane, A.Kechechyan, M.Kelsey, Y.V.Khyzhniak, D.P.Kikola, C.Kim, B.Kimelman, D.Kincses, I.Kisel, A.Kiselev, A.G.Knospe, H.S.Ko, L.Kochenda, L.K.Kosarzewski, L.Kramarik, P.Kravtsov, L.Kumar, S.Kumar, R.Kunnawalkam Elayavalli, J.H.Kwasizur, R.Lacey, S.Lan, J.M.Landgraf, J.Lauret, A.Lebedev, R.Lednicky, J.H.Lee, Y.H.Leung, C.Li, C.Li, W.Li, X.Li, Y.Li, X.Liang, Y.Liang, R.Licenik, T.Lin, Y.Lin, M.A.Lisa, F.Liu, H.Liu, H.Liu, P.Liu, T.Liu, X.Liu, Y.Liu, Z.Liu, T.Ljubicic, W.J.Llope, R.S.Longacre, E.Loyd, N.S.Lukow, X.F.Luo, L.Ma, R.Ma, Y.G.Ma, N.Magdy, D.Mallick, S.Margetis, C.Markert, H.S.Matis, J.A.Mazer, N.G.Minaev, S.Mioduszewski, B.Mohanty, M.M.Mondal, I.Mooney, D.A.Morozov, A.Mukherjee, M.Nagy, J.D.Nam, Md.Nasim, K.Nayak, D.Neff, J.M.Nelson, D.B.Nemes, M.Nie, G.Nigmatkulov, T.Niida, R.Nishitani, L.V.Nogach, T.Nonaka, A.S.Nunes, G.Odyniec, A.Ogawa, S.Oh, V.A.Okorokov, B.S.Page, R.Pak, J.Pan, A.Pandav, A.K.Pandey, Y.Panebratsev, P.Parfenov, B.Pawlik, D.Pawlowska, H.Pei, C.Perkins, L.Pinsky, R.L.Pinter, J.Pluta, B.R.Pokhrel, G.Ponimatkin, J.Porter, M.Posik, V.Prozorova, N.K.Pruthi, M.Przybycien, J.Putschke, H.Qiu, A.Quintero, C.Racz, S.K.Radhakrishnan, N.Raha, R.L.Ray, R.Reed, H.G.Ritter, M.Robotkova, O.V.Rogachevskiy, J.L.Romero, D.Roy, L.Ruan, J.Rusnak, N.R.Sahoo, H.Sako, S.Salur, J.Sandweiss, S.Sato, W.B.Schmidke, N.Schmitz, B.R.Schweid, F.Seck, J.Seger, M.Sergeeva, R.Seto, P.Seyboth, N.Shah, E.Shahaliev, P.V.Shanmuganathan, M.Shao, T.Shao, A.I.Sheikh, D.Shen, S.S.Shi, Y.Shi, Q.Y.Shou, E.P.Sichtermann, R.Sikora, M.Simko, J.Singh, S.Singha, M.J.Skoby, N.Smirnov, Y.Sohngen, W.Solyst, P.Sorensen, H.M.Spinka, B.Srivastava, T.D.S.Stanislaus, M.Stefaniak, D.J.Stewart, M.Strikhanov, B.Stringfellow, A.A.P.Suaide, M.Sumbera, B.Summa, X.M.Sun, X.Sun, Y.Sun, Y.Sun, B.Surrow, D.N.Svirida, Z.W.Sweger, P.Szymanski, A.H.Tang, Z.Tang, A.Taranenko, T.Tarnowsky, J.H.Thomas, A.R.Timmins, D.Tlusty, T.Todoroki, M.Tokarev, C.A.Tomkiel, S.Trentalange, R.E.Tribble, P.Tribedy, S.K.Tripathy, T.Truhlar, B.A.Trzeciak, O.D.Tsai, Z.Tu, T.Ullrich, D.G.Underwood, I.Upsal, G.Van Buren, J.Vanek, A.N.Vasiliev, I.Vassiliev, V.Verkest, F.Videbaek, S.Vokal, S.A.Voloshin, F.Wang, G.Wang, J.S.Wang, P.Wang, Y.Wang, Y.Wang, Z.Wang, J.C.Webb, P.C.Weidenkaff, L.Wen, G.D.Westfall, H.Wieman, S.W.Wissink, J.Wu, Y.Wu, B.Xi, Z.G.Xiao, G.Xie, W.Xie, H.Xu, N.Xu, Q.H.Xu, Y.Xu, Z.Xu, Z.Xu, C.Yang, Q.Yang, S.Yang, Y.Yang, Z.Ye, Z.Ye, L.Yi, K.Yip, Y.Yu, H.Zbroszczyk, W.Zha, C.Zhang, D.Zhang, J.Zhang, S.Zhang, S.Zhang, X.P.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, Z.J.Zhang, Z.Zhang, Z.Zhang, J.Zhao, C.Zhou, X.Zhu, M.Zurek, M.Zyzak Global Λ-hyperon polarization in Au+Au collisions at √ sNN = 3 GeV
doi: 10.1103/PhysRevC.104.L061901
2021MA27 Nucl.Phys. A1010, 122194 (2021) Manju, M.Dan, G.Singh, J.Singh, Shubhchintak, R.Chatterjee Exploring the structure of 29Ne NUCLEAR REACTIONS 208Pb(29Ne, X), E=244 MeV/nucleon; calculated several reaction observables to quantify its structural parameters, one-neutron removal σ, σ(θ, E). 28,29Ne; deduced moderate halo.
doi: 10.1016/j.nuclphysa.2021.122194
2021SI23 Prog.Theor.Exp.Phys. 2021, 073D01 (2021) Systematic study on the role of various higher-order processes in the breakup of weakly-bound projectiles NUCLEAR REACTIONS 208Pb(11Be, X), (17F, X), E=100, 250, 520 MeV/nucleon; calculated breakup σ(E) using an eikonal version of a three-body continuum-discretized coupled-channels (CDCC) reaction model. Comparison with available data.
doi: 10.1093/ptep/ptab055
2021SI27 Phys.Rev. C 104, 034612 (2021) J.Singh, T.Matsumoto, T.Fukui, K.Ogata Three-body description of 9C: Role of low-lying resonances in breakup reactions NUCLEAR STRUCTURE 9C; calculated energies of the ground state and complex eigenenergies of continuum states by coupling of valence proton to 0+, 1- and 2+ states of 8B core nucleus using Gaussian-expansion method (GEM) and complex-scaling method (CSM) in the four-body version of continuum-discretized coupled-channels (CDCC) formalism. Comparison with experimental data. NUCLEAR REACTIONS 208Pb(9C, X), E=65, 160 MeV/nucleon; calculated breakup σ(E) of 9C in 7Be+p+p using continuum-discretized coupled-channels (CDCC) method based on 7Be+p+p+208Pb four-body model. Comparison with experimental data. Relevance to 8B(p, γ)9C reaction of interest in astrophysical scenario.
doi: 10.1103/PhysRevC.104.034612
2021SU25 Nat.Phys. 17, 687 (2021), Erratum Nat.Phys. 18, 473 (2022) V.Sulkosky, C.Peng, J.Chen, A.Deur, S.Abrahamyan, K.A.Aniol, D.S.Armstrong, T.Averett, S.L.Bailey, A.Beck, P.Bertin, F.Butaru, W.Boeglin, A.Camsonne, G.D.Cates, C.-C.Chang, S.Choi, E.Chudakov, L.Coman, J.C.Cornejo, B.Craver, F.Cusanno, R.De Leo, C.W.de Jager, J.D.Denton, S.Dhamija, R.Feuerbach, J.M.Finn, S.Frullani, K.Fuoti, H.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, C.Glashausser, J.Gomez, J.-O.Hansen, D.Hayes, F.W.Hersman, D.W.Higinbotham, T.Holmstrom, T.B.Humensky, C.E.Hyde, H.Ibrahim, M.Iodice, X.Jiang, L.J.Kaufman, A.Kelleher, K.E.Keister, W.Kim, A.Kolarkar, N.Kolb, W.Korsch, K.Kramer, G.Kumbartzki, L.Lagamba, V.Laine, G.Laveissiere, J.J.Lerose, D.Lhuillier, R.Lindgren, N.Liyanage, H.-J.Lu, B.Ma, D.J.Margaziotis, P.Markowitz, K.R.McCormick, M.Meziane, Z.-E.Meziani, R.Michaels, B.Moffit, P.Monaghan, S.Nanda, J.Niedziela, M.Niskin, R.Pandolfi, K.D.Paschke, M.Potokar, A.Puckett, V.A.Punjabi, Y.Qiang, R.D.Ransome, B.Reitz, R.Roche, A.Saha, A.Shabetai, S.Sirca, J.T.Singh, K.Slifer, R.Snyder, P.Solvignon, R.Stringer, R.Subedi, W.A.Tobias, N.Ton, P.E.Ulmer, G.M.Urciuoli, A.Vacheret, E.Voutier, K.Wang, L.Wan, B.Wojtsekhowski, S.Woo, H.Yao, J.Yuan, X.Zhan, X.Zheng, L.Zhu Measurement of the generalized spin polarizabilities of the neutron in the low-Q2 region NUCLEAR REACTIONS 3He(polarized e-, e-), E=1.1-4.4 GeV; measured reaction products, Eβ, Iβ. 1NN; deduced transverse-transverse and longitudinal-transverse interference σ, generalized neutron spin polarizabilities. Comparison with chiral effective field theory calculations.
doi: 10.1038/s41567-021-01245-9
2020CA29 Phys.Rev. C 102, 064627 (2020) J.Casal, J.Singh, L.Fortunato, W.Horiuchi, A.Vitturi Electric dipole response of low-lying excitations in the two-neutron halo nucleus 29F NUCLEAR STRUCTURE 29F; calculated convergence of the ground-state energy as a function of hypermomentum Kmax and number of basis functions N, ground-state probability density using three-body model 27F+n+n, convergence of B(E1) distribution as function of Kmax, B(E1) distribution as a function of the continuum energy, energies of the 0+, 1-, and 2+ states; deduced two-neutron halo for 29F. Hyperspherical harmonics expansion formalism. NUCLEAR REACTIONS 208Pb(29F, X), E=235 MeV/nucleon; calculated B(E1) distribution as a function of the continuum energy. 120Sn(29F, X), E=84 MeV; calculated form factors for quadrupole couplings involving the bound states, monopole, dipole, and quadrupole couplings connecting the ground state with continuum pseudostates, σ(θ), B(E1) distributions. Glauber-model calculations for high-energy reactions, and four-body continuum-discretized coupled-channels (CDCC) calculations at low energy.
doi: 10.1103/PhysRevC.102.064627
2020FO12 Commun. Phys. 3, 132 (2020) L.Fortunato, J.Casal, W.Horiuchi, J.Singh, A.Vitturi The 29F nucleus as a lighthouse on the coast of the island of inversion NUCLEAR STRUCTURE 27,28,29F; analyzed available data; deduced phase shifts, ground-state probability density, estimate of relativistic Coulomb excitation σ.
doi: 10.1038/s42005-020-00402-5
2020SI06 Phys.Rev. C 101, 024310 (2020) J.Singh, J.Casal, W.Horiuchi, L.Fortunato, A.Vitturi Exploring two-neutron halo formation in the ground state of 29F within a three-body model NUCLEAR STRUCTURE 29F; calculated configuration mixing, matter radius as function of S(2n), probability density for the ground state using three-body (27F+n+n) calculations with hyperspherical formalism, analytical transformed harmonic oscillator basis, and Gogny-Pires-Tourreil (GPT) nn interaction; deduced presence of a moderate halo structure in the ground state. Comparison with available experimental data.
doi: 10.1103/PhysRevC.101.024310
2019AB12 J.Phys.(London) G46, 100501 (2019) E.P.Abel, M.Avilov, V.Ayres, E.Birnbaum, G.Bollen, G.Bonito, T.Bredeweg, H.Clause, A.Couture, J.DeVore, M.Dietrich, P.Ellison, J.Engle, R.Ferrieri, J.Fitzsimmons, M.Friedman, D.Georgobiani, S.Graves, J.Greene, S.Lapi, C.S.Loveless, T.Mastren, C.Martinez-Gomez, S.McGuinness, W.Mittig, D.Morrissey, G.Peaslee, F.Pellemoine, J.D.Robertson, N.Scielzo, M.Scott, G.Severin, D.Shaughnessy, J.Shusterman, J.Singh, M.Stoyer, L.Sutherlin, A.Visser, J.Wilkinson Isotope harvesting at FRIB: additional opportunities for scientific discovery
doi: 10.1088/1361-6471/ab26cc
2019LO07 Phys.Rev. C 99, 065805 (2019) B.Loseth, R.Fang, D.Frisbie, K.Parzuchowski, C.Ugalde, J.Wenzl, J.T.Singh Detection of atomic nuclear reaction products via optical imaging NUCLEAR REACTIONS 22Ne(α, n)25Mg, E at Gamow window; 91Nb(p, γ)92Mo, E at Gamow window; calculated yields, capture and detection efficiency of single reaction product atoms captured in optically transparent solid noble gas, followed by selective identification by laser-induced fluorescence and individual counting via optical imaging to determine the low-yield cross section. Single-atom microscope (SAM) technique. ATOMIC PHYSICS Li, Be, Na, Al, S, Mg, K, Ca, Zn, Rb, Sr, Mo, Cd, Cs, Ba, Yb, Hg; compiled matrix-isolated absorption and emission atomic spectra of SAM-friendly species.
doi: 10.1103/PhysRevC.99.065805
2019MA19 Eur.Phys.J. A 55, 5 (2019) Manju, J.Singh, Shubhchintak, R.Chatterjee Low-lying dipole strengths for probable p-wave one-neutron halos in the medium mass region NUCLEAR STRUCTURE 31Ne, 34Na, 37Mg; calculated p-wave one-neutron halo nuclei at zero deformation radius, dipole strength distribution vs energy in continuum for low-lying state with and without correction factor using relative energy spectra in Coulomb dissociation of 31Ne, 34Na, 37Mg on 208Pb at 100, 234, 244 MeV/nucleon as a base to calculate dipole strength distribution. FRDWBA theory.
doi: 10.1140/epja/i2019-12679-4
2019SI29 Few-Body Systems 60, 50 (2019) J.Singh, W.Horiuchi, L.Fortunato, A.Vitturi Two-Neutron Correlations in a Borromean 20C + n + n System: Sensitivity of Unbound Subsystems NUCLEAR STRUCTURE 22C; analyzed available data; deduced components of the ground state, two-particle density, total E1 strength distribution, total monopole transition strength distribution.
doi: 10.1007/s00601-019-1518-8
2016BI10 Phys.Rev. C 94, 025501 (2016) M.Bishof, R.H.Parker, K.G.Bailey, J.P.Greene, R.J.Holt, M.R.Kalita, W.Korsch, N.D.Lemke, Z.-T.Lu, P.Mueller, T.P.O'Connor, J.T.Singh, M.R.Dietrich Improved limit on the 225Ra electric dipole moment NUCLEAR MOMENTS 225Ra; measured Larmor precession in a uniform magnetic field using nuclear-spin-dependent laser light scattering for laser-cooled and trapped 225Ra atoms; deduced upper limit of electric dipole moment (EDM); discussed future improvement of experimental methods in lowering the limit by five orders of magnitude. Comparison with previous experimental results. Relevance to CP violation.
doi: 10.1103/PhysRevC.94.025501
2016KU08 Hyperfine Interactions 237, 95 (2016) F.Kuchler, E.Babcock, M.Burghoff, T.Chupp, S.Degenkolb, I.Fan, P.Fierlinger, F.Gong, E.Kraegeloh, W.Kilian, S.Knappe-Gruneberg, T.Lins, M.Marino, J.Meinel, B.Niessen, N.Sachdeva, Z.Salhi, A.Schnabel, F.Seifert, J.Singh, S.Stuiber, L.Trahms, J.Voigt A new search for the atomic EDM of 129Xe at FRM-II NUCLEAR MOMENTS 129Xe; measured spin precession signals; deduced permanent electric dipole moment sensitivity.
doi: 10.1007/s10751-016-1302-9
2016SI05 Acta Phys.Pol. B47, 833 (2016) New Experiments Demand for a More Precise Analysis of Continuum Spectrum in 6He: Technical Details and Formalism NUCLEAR STRUCTURE 5,6He; calculated 5He sd-continuum waves, coefficients of ground and continuum states of 6He.
doi: 10.5506/APhysPolB.47.833
2016SI19 Eur.Phys.J. A 52, 209 (2016) J.Singh, L.Fortunato, A.Vitturi, R.Chatterjee Electric multipole response of the halo nucleus 6He NUCLEAR STRUCTURE 6He; calculated halo nucleus configuration of 0+1 gs, radius, mean-square distance between valence neutrons, distance between their centre and the core, monopole E0, dipole E1, octupole E3 transition strength distributions, B(E1), B(E3), levels, J, π. Model using different continuum components of weakly bound 6He halo nucleus with unbound 5He spd waves. Compared with published calculations.
doi: 10.1140/epja/i2016-16209-8
2015PA30 Phys.Rev.Lett. 114, 233002 (2015) R.H.Parker, M.R.Dietrich, M.R.Kalita, N.D.Lemke, K.G.Bailey, M.Bishof, J.P.Greene, R.J.Holt, W.Korsch, Z-T.Lu, P.Mueller, T.P.O'Connor, J.T.Singh First Measurement of the Atomic Electric Dipole Moment of 225Ra ATOMIC PHYSICS 225Ra; measured precession curves; deduced electric dipole moment limit. Optical dipole trap, comparison with available data.
doi: 10.1103/PhysRevLett.114.233002
2015SI09 Phys.Rev. C 91, 055205 (2015) J.T.Singh, P.A.M.Dolph, W.A.Tobias, T.D.Averett, A.Kelleher, K.E.Mooney, V.V.Nelyubin, Y.Wang, Y.Zheng, G.D.Cates Development of high-performance alkali-hybrid polarized 3He targets for electron scattering
doi: 10.1103/PhysRevC.91.055205
2014AG07 At.Data Nucl.Data Tables 100, 859 (2014) S.Aggarwal, J.Singh, A.K.S.Jha, M.Mohan Energy levels and radiative transition rates for Ge XXXI, As XXXII, and Se XXXIII ATOMIC PHYSICS Ge, As, Se; calculated fine-structure energies, lifetimes. General-Purpose Relativistic Atomic Structure Package (GRASP).
doi: 10.1016/j.adt.2013.11.005
2014FO20 Phys.Rev. C 90, 064301 (2014) L.Fortunato, R.Chatterjee, J.Singh, A.Vitturi Pairing in the continuum: The quadrupole response of the Borromean nucleus 6He NUCLEAR STRUCTURE 6He; calculated levels, J, π, B(E2) strength distribution, Borromean character of the bound ground state. Shell model calculations in a basis of two-particle states built out of continuum p states of the unbound 5He nucleus, and using a simple pairing contact-delta interaction. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.064301
2012PA41 Phys.Rev. C 86, 065503 (2012) R.H.Parker, M.R.Dietrich, K.Bailey, J.P.Greene, R.J.Holt, M.R.Kalita, W.Korsch, Z.-T.Lu, P.Mueller, T.P.O'Connor, J.Singh, I.A.Sulai, W.L.Trimble Efficient, tightly-confined trapping of 226Ra ATOMIC PHYSICS 226Ra; measured transfer efficiencies from three-dimensional magneto-optical trap (MOT) to standing wave optical dipole trap (ODT). Electric dipole moment (EDM) measurements at Argonne National Laboratory.
doi: 10.1103/PhysRevC.86.065503
2011DO17 Phys.Rev. C 84, 065201 (2011) P.A.M.Dolph, J.Singh, T.Averett, A.Kelleher, K.E.Mooney, V.Nelyubin, W.A.Tobias, B.Wojtsekhowski, G.D.Cates Gas dynamics in high-luminosity polarized 3He targets using diffusion and convection
doi: 10.1103/PhysRevC.84.065201
2007SI34 Phys.Rev. C 76, 065210 (2007) Mass and width of strange baryon resonances using QCD sum rules
doi: 10.1103/PhysRevC.76.065210
2005CH04 Eur.Phys.J. A 23, 223 (2005) R.Chandra, J.Singh, P.K.Rath, P.K.Raina, J.G.Hirsch Two-neutrino double-β decay of 94 ≤ A ≤ 110 nuclei for the 0+ → 0+ transition NUCLEAR STRUCTURE 94,96Zr, 94,96,98,100Mo, 98,100,104Ru, 104,110Pd, 110Cd; calculated levels, J, π, B(E2), quadrupole moments, g-factors. Projected Hartree-Fock-Bogoliubov model, comparison with data. RADIOACTIVITY 94,96Zr, 98,100Mo, 104Ru, 110Pd(2β-); calculated 2νββ-decay T1/2, deformation effects. Projected Hartree-Fock-Bogoliubov model, comparisons with data.
doi: 10.1140/epja/i2004-10087-7
2005KR14 Phys.Rev.Lett. 95, 142002 (2005) K.Kramer, D.S.Armstrong, T.D.Averett, W.Bertozzi, S.Binet, C.Butuceanu, A.Camsonne, G.D.Cates, J.-P.Chen, S.Choi, E.Chudakov, F.Cusanno, A.Deur, P.Djawotho, D.Dutta, J.M.Finn, H.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, V.Gorbenko, K.A.Griffioen, J.-O.Hansen, D.W.Higinbotham, W.Hinton, T.Horn, C.W.de Jager, X.Jiang, W.Korsch, J.LeRose, D.Lhuillier, N.Liyanage, D.J.Margaziotis, K.McCormick, Z.-E.Meziani, R.Michaels, B.Milbrath, B.Moffit, S.Nanda, C.F.Perdrisat, R.Pomatsalyuk, V.Punjabi, B.Reitz, J.Roche, R.Roche, M.Roedelbronn, N.Savvinov, J.Secrest, J.Singh, S.Sirca, K.Slifer, P.Solvignon, D.J.Steiner, R.Suleiman, V.Sulkosky, A.Tobias, A.Vacheret, Y.Xiao, X.Zheng, J.Zhou, L.Zhu, X.Zhu, P.A.Zolnierczuk Q2 Dependence of the Neutron Spin Structure Function gn2 at Low Q2 NUCLEAR REACTIONS 3He(polarized e, e'), E=3.465-5.727 GeV; measured parallel and perpendicular cross section differences. 1n, 3He deduced momentum transfer dependence of spin structure function.
doi: 10.1103/PhysRevLett.95.142002
2005SI38 Pramana 65, 517 (2005) J.Singh, R.Chandra, P.K.Raina, P.K.Rath Two-neutrino double β decay of 96Zr to excited 2+ state of 96Mo RADIOACTIVITY 96Zr(2β-); calculated 2νββ-decay T1/2 for decay to excited state. NUCLEAR STRUCTURE 96Zr, 96Mo; calculated 2+ levels B(E2), quadrupole moments, g factors.
doi: 10.1007/BF02704209
2005UP01 J.Phys.(London) G31, 987 (2005) Isospin breaking in diagonal pion-nucleon coupling constant: QCD sum rule approach
doi: 10.1088/0954-3899/31/9/001
2004SI14 J.Phys.(London) G30, 881 (2004) Spin studies of nucleons in a statistical model
doi: 10.1088/0954-3899/30/7/005
2002PU02 Pramana 59, 19 (2002) Fragment Production in 16O + 80Br Reaction within Dynamical Microscopic Theory NUCLEAR REACTIONS 80Br(16O, X), E=50-200 MeV/nucleon; calculated fragment mass and charge distributions, multiplicities. Quantum molecular dynamics, simulated annealing clusterization algorithm.
doi: 10.1007/s12043-002-0030-7
2002PU05 Acta Phys.Hung.N.S. 16, 233 (2002) Multi-Fragmentation in Heavy-Ion Collisions: Role of System-Size Effects, Cross-Section and Equation of State
doi: 10.1556/APH.16.2002.1-4.45
2002SI02 Phys.Rev. C65, 024602 (2002) Mass Dependence in the Production of Light Fragments in Heavy-Ion Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), 58Ni(58Ni, X), 93Nb(93Nb, X), 131Xe(131Xe, X), 168Er(168Er, X), 197Au(197Au, X), 238U(238U, X), E=50-1000 MeV/nucleon; calculated light and medium mass fragment yields; deduced dependence on mass of system. Quantum molecular dynamics, minimum spanning tree clusterization.
doi: 10.1103/PhysRevC.65.024602
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
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
2001SI19 Phys.Rev. C63, 054603 (2001) Momentum Dependent Interactions and the Asymmetry of the Reaction: Multifragmentation as an Example NUCLEAR REACTIONS Ag, Br(16O, X), E=25-200 MeV/nucleon; calculated fragments spectra, mass and multiplicity distributions; deduced role of momentum dependent interactions. Quantum molecular dynamics approach.
doi: 10.1103/PhysRevC.63.054603
2001SI40 J.Phys.(London) G27, 2091 (2001) Study of the Formation of Fragments with Different Clusterization Methods NUCLEAR REACTIONS Ag, Br(O, X), E=50, 200 MeV/nucleon; calculated fragments mass yields, charge distributions, time evolution features. Quantum molecular dynamics model, different clusterization methods compared.
doi: 10.1088/0954-3899/27/10/310
2001SI41 Phys.Lett. 519B, 46 (2001) Study of System-Size Effects in Multi-Fragmentation using Quantum Molecular Dynamics Model NUCLEAR REACTIONS 40Ca(40Ca, X), 58Ni(58Ni, X), 93Nb(93Nb, X), 131Xe(131Xe, X), 168Er(168Er, X), 197Au(197Au, X), 238U(238U, X), E=50-1000 MeV/nucleon; calculated light and intermediate mass fragments multiplicities; deduced system size effects, power law parameterization. Quantum molecular dynamics model.
doi: 10.1016/S0370-2693(01)01073-5
2000SI22 Pramana 54, 519 (2000) Large Hadron Collider Physics Program: Compact muon solenoid experiment NUCLEAR REACTIONS 1H(p, X), E(cm)=14 TeV; calculated Higgs boson production σ vs mass, observability features. Compact muon solenoid experiment.
doi: 10.1007/s12043-000-0147-5
2000SI34 Phys.Rev. C62, 044617 (2000) Model Ingredients and Multifragmentation in Symmetric and Asymmetric Heavy Ion Collisions NUCLEAR REACTIONS Ag, Br(O, X), E=50, 200 MeV/nucleon; Sn(Xe, X), E=400 MeV/nucleon; calculated fragment charge distributions, time evolution of light, intermediate mass fragment multiplicities; deduced role of momentum-dependent interactions.
doi: 10.1103/PhysRevC.62.044617
2000SI35 Phys.Rev. C62, 054602 (2000) Dynamical Multifragmentation and Spatial Correlations NUCLEAR REACTIONS 197Au(197Au, X), E=100, 600 MeV/nucleon; Ag, Br(O, X), E=200 MeV/nucleon; Sn(Xe, X), E=400 MeV/nucleon; calculated fragment mass yields vs impact parameter; deduced role of spatial correlations.
doi: 10.1103/PhysRevC.62.054602
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
1997KA03 Phys.Rev. C55, 512 (1997) H.Kaur, J.Singh, A.Sharma, J.Goswamy, D.Mehta, N.Singh, P.N.Trehan, E.S.Paul, R.K.Bhowmik Collective Structures in Doubly Odd 120I NUCLEAR REACTIONS 108Pd(16O, X), E=84 MeV; 114Cd(11B, X), E=60 MeV; measured γγ-coin, DCO ratios. 120I deduced high-spin levels, J, π, band structure, configuration, γ-multipolarity.
doi: 10.1103/PhysRevC.55.512
1997KA21 Phys.Rev. C55, 2234 (1997) H.Kaur, J.Singh, A.Sharma, D.Mehta, N.Singh, P.N.Trehan, H.C.Jain, S.D.Paul, E.S.Paul, R.K.Bhowmik High Spin States in Doubly Odd 122I NUCLEAR REACTIONS 116Cd(11B, 5n), E=64 MeV; measured γγ-energy correlation. 110Pd(16O, 3np), E=81 MeV; measured pγ-coin. 122I deduced high-spin levels, J, π, configurations, band terminating features. TRS calculations.
doi: 10.1103/PhysRevC.55.2234
1996SH04 Z.Phys. A354, 347 (1996) A.Sharma, J.Singh, H.Kaur, J.Goswamy, D.Mehta, N.Singh, P.N.Trehan, E.S.Paul, R.K.Bhowmik High Spin States in 116,118Te NUCLEAR REACTIONS 102Ru(19F, 4np), E=90 MeV; 110Pd(13C, 5n), E=66 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 108Pd(12C, 4n), E=69 MeV; 110Pd(12C, 4n), E=66 MeV; measured Iγ(θ). 116,118Te deduced high-spin levels, J, π, γ-multipolarity, configuration.
doi: 10.1007/s002180050057
1996SI24 Z.Phys. A356, 125 (1996) J.Singh, H.Kaur, A.Sharma, J.Goswamy, D.Mehta, N.Singh, P.N.Trehan, E.S.Paul, R.K.Bhowmik High Spin States in 121Te NUCLEAR REACTIONS 114Cd(11B, 3np), E=64 MeV; measured γγ-coin, Eγ, Iγ, DCO ratios. 121Te deduced high-spin levels, J, π, γ-branching, γ multipolarity, configuration. Total Routhian surface calculations, other Te isotopes considered.
doi: 10.1007/s002180050158
1995KA17 Z.Phys. A352, 11 (1995) H.Kaur, J.Singh, A.Sharma, J.Goswamy, D.Mehta, N.Singh, R.K.Bhowmik, P.N.Trehan Band Structures in Doubly-Odd 120I Nucleus NUCLEAR REACTIONS 108Pd(16O, 3np), E=84 MeV; 114Cd(11B, 5n), E=60 MeV; measured γγ-coin. 120I deduced levels, J, π, B(λ) ratios, band structures, configuration.
doi: 10.1007/BF01292755
1995SH11 Z.Phys. A351, 131 (1995) A.Sharma, J.Singh, H.Kaur, J.Goswamy, D.Mehta, N.Singh, R.K.Bhowmik, P.N.Trehan Quasiparticle Structures in 118Te NUCLEAR REACTIONS 110Pd(13C, 5n), E=66 MeV; measured γγ-coin. 118Te deduced high-spin levels, J, π, configuration, band structure.
doi: 10.1007/BF01289521
1995SI10 Z.Phys. A351, 3 (1995) J.Singh, J.Goswamy, A.Sharma, H.Kaur, D.Mehta, N.Singh, P.N.Trehan, R.K.Bhowmik, R.S.Chakrawarthy, P.Singh, B.Srinivasan High Spin Structures in 119Te NUCLEAR REACTIONS 110Pd(13C, 4n), E=66 MeV; 110Pd(12C, 3n), E=55 MeV; measured γγ-coin. 119Te deduced levels, J, π, high-spin, band structure, configurations.
doi: 10.1007/BF01292776
1995SI28 Z.Phys. A353, 125 (1995) J.Singh, H.Kaur, A.Sharma, J.Goswamy, D.Mehta, N.Singh, R.K.Bhowmik, P.N.Trehan Non-Collective Oblate States in 121Te NUCLEAR REACTIONS 114Cd(11B, 3np), E=60 MeV; measured γγ-coin. 121Te deduced high-spin levels, J, π, configuration.
doi: 10.1007/BF01295889
1995SI29 Z.Phys. A353, 239 (1995) J.Singh, H.Kaur, A.Sharma, J.Goswamy, D.Mehta, N.Singh, P.N.Trehan, E.S.Paul, R.K.Bhowmik Non-Collective Oblate States in 119Te NUCLEAR REACTIONS 110Pd(13C, 4n), E=66 MeV; measured γγ-coin, Eγ, Iγ, DCO ratios. 110Pd(12C, 3n), E=55 MeV; measured Eγ, Iγ, γ(θ). 119Te deduced high-spin levels, J, π, γ multipolarity, configuration. Total routhian surface calculations.
doi: 10.1007/BF01292327
1994KA39 Z.Phys. A350, 183 (1994) H.Kaur, J.Goswamy, J.Singh, A.Sharma, D.Mehta, N.Singh, R.K.Bhowmik, P.N.Trehan A New Band in Doubly-Odd 118I NUCLEAR REACTIONS 105Pd(16O, 2np), E=85 MeV; 106Pd(16O, 3np), E=89 MeV; measured Eγ, Iγ, DCO ratios, γγ-coin. 118I deduced high-spin levels, possible J, π, band structure, configuration.
doi: 10.1007/BF01289579
1994SI01 Phys.Rev. C49, 1066 (1994) G.Singh, H.S.Hans, T.S.Cheema, K.P.Singh, D.C.Tayal, J.Singh, S.Ghosh Systematics of Preequilibrium Contributions in (n, p) Reactions at 14 MeV NUCLEAR REACTIONS 19F, 24Mg, 27Al, 28Si, 31P, 32S, 40Ca, 46,47,48,50Ti, 51V, 50,52Cr, 54,56Fe, 59Co, 58,60Ni, 63,65Cu, 64,66Zn, 89Y, 90Zr, 93Nb, 92,94,95,96Mo, 103Rh, 106,108Pd, 107,109Ag, 115In(n, p), E ≈ 14 MeV; analyzed angle integrated σ, spectra; deduced preequilibrium contribution systematics.
doi: 10.1103/PhysRevC.49.1066
1993SH20 Z.Phys. A346, 321 (1993) A.Sharma, J.Goswamy, D.Mehta, J.Singh, H.Kaur, B.Chand, N.Singh, R.K.Bhowmik, P.N.Trehan High Spin States in 116Te NUCLEAR REACTIONS 102Ru(19F, 4np), E=90 MeV; measured γγ-coin, DCO. 116Te deduced levels, J, π, band structure, configuration.
doi: 10.1007/BF01292525
1989AD13 Phys.Rev.Lett. 63, 2349 (1989) M.Aderholz, M.M.Aggarwal, H.Akbari, P.P.Allport, P.V.K.S.Baba, S.K.Badyal, M.Barth, J.P.Baton, H.H.Bingham, E.B.Brucker, R.A.Burnstein, R.C.Campbell, R.Cence, T.K.Chatterjee, E.F.Clayton, G.Corrigan, C.Coutures, D.Deprospo, Devanand, E.De Wolf, P.J.W.Faulkner, W.B.Fretter, V.K.Gupta, J.Guy, J.Hanlon, G.Harigel, F.Harris, M.A.Jabiol, P.Jacques, V.Jain, G.T.Jones, M.D.Jones, R.W.L.Jones, T.Kafka, M.Kalelkar, P.Kasper, P.Kasper, G.L.Kaul, M.Kaur, J.M.Kohli, E.L.Koller, R.J.Krawiec, M.Lauko, J.Lys, W.A.Mann, P.Marage, R.H.Milburn, D.B.Miller, I.S.Mittra, M.M.Mobayyen, J.Moreels, D.R.O.Morrison, G.Myatt, P.Nailor, R.Naon, A.Napier, M.Neveu, D.Passmore, M.W.Peters, V.Z.Peterson, R.Plano, N.K.Rao, H.A.Rubin, J.Sacton, B.Saitta, P.Schmid, N.Schmitz, J.Schneps, R.Sekulin, S.Sewell, J.B.Singh, P.M.Sood, W.Smart, P.Stamer, K.E.Varvell, W.Venus, L.Verluyten, L.Voyvodic, H.Wachsmuth, S.Wainstein, S.Willocq, W.Wittek, G.P.Yost Coherent Production of π+ and π- Mesons by Charged-Current Interactions of Neutrinos and Antineutrinos on Neon Nuclei at the Fermilab Tevatron NUCLEAR REACTIONS 1H, Ne(ν, X), (ν-bar, X), E=40-300 GeV; measured coherent single π+, π- production σ, kinematic distributions. Meson dominance, partial axial-vector current conservation model.
doi: 10.1103/PhysRevLett.63.2349
1986ME07 Nucl.Instrum.Methods Phys.Res. A245, 447 (1986); see 1986Me10 D.Mehta, M.L.Garg, J.Singh, N.Singh, T.S.Cheema, P.N.Trehan Precision Measurements of X- and Gamma-Ray Intensities in 192Ir, 160Tb, 169Yb and 152Eu Decays
doi: 10.1016/0168-9002(86)91281-7
1986ME10 Nucl.Instrum.Methods Phys.Res. A245, 447 (1986) D.Mehta, M.L.Garg, J.Singh, N.Singh, T.S.Cheema, P.N.Trehan Precision Measurements of X- and Gamma-Ray Intensities in 192Ir, 160Tb, 169Yb and 152Eu Decays RADIOACTIVITY 192Ir(EC), (β-); 160Tb(β-); 169Yb(EC); 152Eu(EC), (β+), (β-); measured Eγ, Iγ, E X-ray, I X-ray. 152Sm, 152Gd, 169Tm, 160Dy, 192Os, 192Pt levels deduced relative Iγ, I(X-ray). High precision, Ge, hyperpure Ge detectors.
doi: 10.1016/0168-9002(86)91281-7
1984GA05 J.Phys.(London) B17, 577 (1984) M.L.Garg, J.Singh, H.R.Verma, N.Singh, P.C.Mangal, P.N.Trehan Relative Intensity Measurements of L-Shell X-Rays for Ta, Au, Pb and Bi in the Energy Range 17-60 keV NUCLEAR REACTIONS Ta, 197Au, Pb, 209Bi(p, X), E=17.8, 25.8, 46.9, 59.5 keV; measured E(L X-ray), relative I(L X-ray). Si-Li detector system.
doi: 10.1088/0022-3700/17/4/013
1984SI16 J.Phys.Soc.Jpn. 53, 2485 (1984) J.Singh, M.L.Garg, D.Mehta, N.Singh, P.N.Trehan Gamma-Gamma Directional Correlations in 160Dy RADIOACTIVITY 160Tb(β-) [from 159Tb(n, γ)]; measured γγ(θ), oriented nuclei. 160Dy levels deduced J, π, δ. NaI(Tl), Ge(Li) coincidence set up.
doi: 10.1143/JPSJ.53.2485
1983SI08 J.Phys.Soc.Jpn. 52, 796 (1983) J.Singh, M.L.Garg, R.Kaur, S.S.Sooch, N.Singh, P.N.Trehan The Level Structure of 105Pd RADIOACTIVITY 105Ag(β+), (EC) [from 103Rh(α, 2n)]; measured Eγ, Iγ, γγ(θ). 105Pd deduced levels, δ, γ-branching, J, π.
doi: 10.1143/JPSJ.52.796
1972BR32 Nucl.Phys. A191, 663 (1972) R.C.Brown, J.A.R.Griffith, O.Karban, S.Roman, J.Singh Elastic and Inelastic Scattering of 12 MeV Polarized Deuterons by 24Mg NUCLEAR REACTIONS 24Mg(polarized d, d), 24Mg(polarized d, d'), E=12.1 MeV; measured iT11(θ), σ(θ). 24Mg deduced deformation β2. Enriched target.
doi: 10.1016/0375-9474(72)90639-2
1972SI31 Trans.Amer.Nucl.Soc. 15, 147 (1972) Neutron Reaction Cross Sections of Iron at 14.5 MeV NUCLEAR REACTIONS 54,57,58Fe(n, p), 54Fe(n, α), E=14.5 MeV; measured Eγ, Iγ; deduced reaction σ. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10309. 1972SI50 Indian J.Pure Appl.Phys. 10, 289 (1972) Determination of Half-Life of 14O and Value of Beta Decay Coupling Constant G(v) RADIOACTIVITY 14O; measured T1/2; deduced log ft, coupling constant.
1970SI15 Nucl.Phys. A155, 443 (1970) Excitation Functions for 3He Induced Reactions with 12C RADIOACTIVITY 14O, 13N; measured T1/2. NUCLEAR REACTIONS 12C(3He, n), E=2.0-30.6 MeV; 12C(3He, d), E=6.5-30.6 MeV; 12C(3He, p)14N, E(3He)=16.0-30.6 MeV; measured σ(E). Natural carbon target.
doi: 10.1016/0375-9474(70)90905-X
1970SI16 Nucl.Phys. A155, 453 (1970) Resonances in the Interaction of 3He Particles with 12C and 10B NUCLEAR REACTIONS 12C(3He, 3He'), , E=threshold to 30.6 MeV; 12C(3He, t), E=22.3 to 30.6 MeV; 10B(3He, n), E=6.9 to 30.6 MeV; measured σ(E). 15O deduced resonance structure. Natural carbon, enriched boron targets.
doi: 10.1016/0375-9474(70)90906-1
1964SI19 NASA TN D-2454 (1964) Tables of X-Coefficients and LAMBDA-Factors for Triple Angular Correlation Analysis
1963PR03 Phys.Rev. 129, 1716 (1963) F.W.Prosser, Jr., R.W.Krone, J.J.Singh C13(p, γ)N14 Reacdtion and the 9.17-, 7.03-, and 6.44-MeV States in N14 NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.1716
1960KR01 Phys.Rev. 117, 1562 (1960) Properties of the Excited States of Na22 from the Ne21(p, γ) Reaction NUCLEAR STRUCTURE 22Na; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.117.1562
1959KR65 Bull.Am.Phys.Soc. 4, No.4, 219, AB10 (1959) R.W.Krone, J.J.Singh, F.W.Prosser, Jr. 9.18-MeV Level in N14
1959SI76 Bull.Am.Phys.Soc. 4, No.6, 367, Q10 (1959) Gamma Rays from Si29(p, γ)
1959SI77 Bull.Am.Phys.Soc. 4, No.1, 17, EA9 (1959) J.J.Singh, V.W.Davis, R.W.Krone Energy Levels of Na23 from the Ne22(p, γ) Reaction
1959SI78 Phys.Rev. 115, 170 (1959) J.J.Singh, V.W.Davis, R.W.Krone Energy Levels in Na23 from the Ne22(p, γ)Na23 Reaction
doi: 10.1103/PhysRev.115.170
1959SI82 Phys.Rev. 115, 445 (1959) Gamma Rays from Si29 + p
doi: 10.1103/PhysRev.115.445
1957BR25 Phil.Mag. 2, 499 (1957) C.Broude, L.L.Green, J.J.Singh, J.C.Willmott The γ-Rays from the 8.06 MeV Level in 14N
doi: 10.1080/14786435708243839
1957BR33 Phil.Mag. 2, 1006 (1957) C.Broude, L.L.Green, J.J.Singh, J.C.Willmott On the 8.06 and 8.70 MeV States in 14N
doi: 10.1080/14786435708238206
Back to query form Note: The following list of authors and aliases matches the search parameter J.Singh: , J.B.SINGH, J.J.SINGH, J.P.SINGH, J.T.SINGH |