NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = U.Singh Found 28 matches. 2024AB01 Eur.Phys.J. A 60, 18 (2024) R.Abou Yassine, O.Arnold, M.Becker, P.Bergmann, A.Blanco, C.Blume, M.Bohmer, N.Carolino, L.Chlad, P.Chudoba, I.Ciepal, J.Dreyer, W.Esmail, L.Fabbietti, P.Fonte, J.Friese, I.Frohlich, T.Galatyuk, J.A.Garzon, M.Grunwald, M.Gumberidze, S.Harabasz, C.Hohne, F.Hojeij, R.Holzmann, H.Huck, M.Idzik, B.Kampfer, B.Kardan, V.Kedych, I.Koenig, W.Koenig, M.Kohls, J.Kolas, G.Korcyl, G.Kornakov, R.Kotte, W.Krueger, A.Kugler, T.Kunz, R.Lalik, F.Linz, L.Lopes, M.Lorenz, A.Malige, J.Markert, V.Metag, J.Michel, A.Molenda, C.Muntz, M.Nabroth, L.Naumann, K.Nowakowski, J. Orlinski, J.-H.Otto, Y.Parpottas, M.Parschau, V.Pechenov, O.Pechenova, K.Piasecki, J.Pietraszko, A.Prozorov, W.Przygoda, B.Ramstein, N.Rathod, J.Ritman, A.Rost, A.Rustamov, P.Salabura, N.Schild, E.Schwab, F.Seck, U.Singh, S.Spies, M.Stefaniak, H.Strobele, J.Stroth, C.Sturm, K.Sumara, O.Svoboda, M.Szala, P.Tlusty, M.Traxler, H.Tsertos, V.Wagner, A.A.Weber, C.Wendisch, H.P.Zbroszczyk, E.Zherebtsova, M.Zielinski, P.Zumbruch Investigation of the Σ0 Production Mechanism in p(3.5 GeV)+p Collisions
doi: 10.1140/epja/s10050-023-01214-1
2023AB26 Phys.Rev. C 108, 064902 (2023) R.Abou Yassine, O.Arnold, M.Becker, P.Bergmann, A.Blanco, C.Blume, M.Bohmer, N.Carolino, L.Chlad, P.Chudoba, I.Ciepal, J.Dreyer, W.A.Esmail, L.Fabbietti, P.Fonte, J.Friese, I.Frohlich, T.Galatyuk, J.A.Garzon, M.Grunwald, M.Gumberidze, S.Harabasz, C.Hohne, F.Hojeij, R.Holzmann, H.Huck, M.Idzik, B.Kampfer, B.Kardan, V.Kedych, I.Koenig, W.Koenig, M.Kohls, G.Korcyl, G.Kornakov, F.Kornas, R.Kotte, W.Krueger, A.Kugler, T.Kunz, R.Lalik, L.Lopes, M.Lorenz, A.Malige, J.Markert, V.Metag, J.Michel, A.Molenda, C.Muntz, L.Naumann, K.Nowakowski, J.-H.Otto, Y.Parpottas, M.Parschau, V.Pechenov, O.Pechenova, J.Pietraszko, A.Prozorov, W.Przygoda, K.Pysz, B.Ramstein, N.Rathod, A.Rost, A.Rustamov, P.Salabura, N.Schild, E.Schwab, F.Seck, U.Singh, S.Spies, M.Stefaniak, H.Strobele, J.Stroth, C.Sturm, K.Sumara, O.Svoboda, M.Szala, P.Tlusty, M.Traxler, H.Tsertos, V.Wagner, A.A.Weber, C.Wendisch, H.P.Zbroszczyk, E.Zherebtsova, Zumbruch, P., B.Kamys, S.Sharma Production of hydrogen isotopes and charged pions in p(3.5 GeV) + 93Nb reactions
doi: 10.1103/PhysRevC.108.064902
2021SI02 Nucl.Phys. A1006, 122066 (2021) U.K.Singh, R.Sharma, P.K.Sharma, M.Kaushik, S.K.Jain, G.Saxena Structural properties and α-decay chains of transfermium nuclei (101 ≤ Z ≤ 110) RADIOACTIVITY 235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287Md, 238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288No, 241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289Lr, 243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290Rf, 245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291Db, 248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292Sg, 250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293Bh, 253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294Hs, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295Mt, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296Ds(α), (SF); calculated potential energy surfaces (PESs), occupancies of neutron single particle states, rms α-decay T1/2, T1/2. Comparison with available data.
doi: 10.1016/j.nuclphysa.2020.122066
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
2020SI27 Nucl.Phys. A1004, 122035 (2020) U.K.Singh, P.K.Sharma, M.Kaushik, S.K.Jain, D.T.Akrawy, G.Saxena Study of decay modes in transfermium isotopes RADIOACTIVITY 245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260Md, 250,251,252,253,254,255,256,257,258,259,260,261,262No, 252,253,254,255,256,257,258,259,260,261,262,263,264,265,266Lr, 253,254,255,256,257,258,259,260,261,262,263,264,265Rf, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270Db, 258,259,260,261,262,263,264,265,266,267,268,269,270,271Sg, 260,261,262,263,264,265,266,267,268,269,270,271,272,273,274Bh, 263,264,265,266,267,268,269,270,271,272,273,274,275,276,277Hs, 266,267,268,269,270,271,272,273,274,275,276,277,278Mt(EC), (β-), (α), (SF); calculated T1/2. Comparison with available data.
doi: 10.1016/j.nuclphysa.2020.122035
2019SI30 Acta Phys.Pol. B50, 1451 (2019) U.Singh, B.Kamys, S.K.Sharma, K.Pysz Odd-Even Staggering in the Yields of Intermediate Mass Fragments from p+Ag collisions at Ep = 480 MeV NUCLEAR REACTIONS Ag(p, X)Li/Be/B/C/N/O/F/Ne/Na/Mg, E=480 MeV; measured reaction products; deduced total production σ. Comparison with intranuclear cascade INCL++ and the second stage by GEMINI++ model or by two other models, namely ABLA07 and SMM.
doi: 10.5506/aphyspolb.50.1451
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
2018OS02 Nucl.Instrum.Methods Phys.Res. B416, 110 (2018) M.Oswal, S.Kumar, U.Singh, G.Singh, K.P.Singh, D.Mehta, D.Mitnik, C.C.Montanari, T.Nandi L x-ray production cross sections in high-Z atoms by 3-5 MeV/u silicon ions NUCLEAR REACTIONS W, 197Au, Pb, Bi(28Si, X), E=3-5 MeV/nucleon; measured reaction products, Eγ, Iγ, X-rays; deduced X-ray production σ.
doi: 10.1016/j.nimb.2017.11.025
2018SA44 Int.J.Mod.Phys. E27, 1850074 (2018) G.Saxena, U.K.Singh, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal Distinct ground state features and the decay chains of Z=121 superheavy nuclei NUCLEAR STRUCTURE Z=121; calculated separation energies, shell corrections, deformation parameters, radial variation of charge density and neutron density using RMF+BCS approach. RADIOACTIVITY 293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312121(α); calculated Q-values, T1/2. Comparison with available data.
doi: 10.1142/S021830131850074X
2018SI19 Eur.Phys.J. A 54, 109 (2018) U.Singh, D.Filges, F.Goldenbaum, B.Kamys, Z.Rudy, S.K.Sharma The predictive power of spallation models for isotopic cross sections NUCLEAR REACTIONS 1H(136Xe, x), E=1000 MeV/nucleon; calculated isotopic σ of IMFs with Z=3-56 using INCL++ coupled to ABLA07, GEM2, GEMINI++ and SMM. Compared to available data.
doi: 10.1140/epja/i2018-12546-x
2017KU02 Nucl.Instrum.Methods Phys.Res. B395, 39 (2017) S.Kumar, U.Singh, M.Oswal, G.Singh, N.Singh, D.Mehta, T.Nandi, G.Lapicki L shell x ray production in high-Z elements using 4-6 MeV/u fluorine ions NUCLEAR REACTIONS Pt, 197Au, Pb, 209Bi, Th, U(19F, X), E=4-6 MeV/nucleon; measured reaction products, X-rays, Eγ, Iγ; deduced L shell line and total x ray production σ. Comparison with available theories for L shell ionization using single- and multiple-hole fluorescence and the Coster-Kronig yields.
doi: 10.1016/j.nimb.2017.01.044
2017SA69 Int.J.Mod.Phys. E26, 1750072 (2017) G.Saxena, M.Kumawat, M.Kaushik, U.K.Singh, S.K.Jain, S.Somorendro Singh, M.Aggarwal Implications of occupancy of 2s1/2 state in sd-shell within RMF+BCS approach NUCLEAR STRUCTURE 22C, 22,24O, 34,36Ca, 26S, 36S, 56S, 22,34,48Si; calculated quadrupole deformation parameters, neutron single particle states, neutron density. Comparison with available data.
doi: 10.1142/S0218301317500720
1979LI08 Nucl.Sci.Eng. 70, 150 (1979) H.I.Liou, R.E.Chrien, R.C.Block, U.N.Singh The Transmission of Neutrons Through Iron-56 at 24.37 keV NUCLEAR REACTIONS 56Fe(n, X), E=24.37, 27.85 keV; measured σ. 57Fe deduced resonance parameters. Isotropically pure target.
doi: 10.13182/NSE79-A19647
1978SI07 Nucl.Sci.Eng. 67, 54 (1978) U.N.Singh, R.C.Block, Y.Nakagome Neutron Capture and Transmission Measurements on Fission Product Palladium-107 NUCLEAR REACTIONS Pd, 107Pd(n, γ), (n, n'γ), E < 700 eV; measured capture, transmission yields. 108Pd deduced neutron resonances, parameters.
doi: 10.13182/NSE78-A27236
1976HA15 Phys.Rev. C13, 1884 (1976) G.Hacken, J.Rainwater, H.I.Liou, U.N.Singh Neutron Resonance Spectroscopy: 139La NUCLEAR REACTIONS 139La(n, X), E=0.003-76 keV; measured total σ(E); deduced resonance parameters.
doi: 10.1103/PhysRevC.13.1884
1976SI01 Phys.Rev. C13, 124 (1976) U.N.Singh, J.Rainwater, H.I.Liou, G.Hacken, J.B.Garg Neutron Resonance Spectroscopy: 209Bi NUCLEAR REACTIONS 209Bi(n, X), E=0.5-75 keV; measured total σ(E). 210Bi deduced resonances, L, J, Γ, strength functions.
doi: 10.1103/PhysRevC.13.124
1975LI01 Phys.Rev. C11, 457 (1975) H.I.Liou, J.Rainwater, G.Hacken, U.N.Singh Neutron Resonance Spectroscopy: Argon NUCLEAR REACTIONS 40Ar(n, n), (n, γ), E=1-580 keV; measured total σ(E). 41Ar deduced resonances, n-width, J, S, L.
doi: 10.1103/PhysRevC.11.457
1975LI02 Phys.Rev. C11, 462 (1975) H.I.Liou, G.Hacken, J.Rainwater, U.N.Singh Neutron Resonance Spectroscopy: The Separated Isotopes of Dy NUCLEAR REACTIONS 160,161,162,163,164Dy(n, n), (n, γ), E=1-2.5 keV; measured total σ(E). 161,162,163,164,165Dy deduced resonances, n-width, γ-width.
doi: 10.1103/PhysRevC.11.462
1975LI07 Phys.Rev. C11, 1231 (1975) H.I.Liou, J.Rainwater, G.Hacken, U.N.Singh Neutron Resonance Spectroscopy: 175Lu NUCLEAR REACTIONS 175Lu(n, n), (n, γ), E=1 eV-3 keV; measured total σ(E), σ(E, Eγ). 176Lu deduced resonances, level-width.
doi: 10.1103/PhysRevC.11.1231
1975LI10 Phys.Rev. C11, 2022 (1975) H.I.Liou, J.Rainwater, G.Hacken, U.N.Singh Neutron Resonance Spectroscopy: 177Hf NUCLEAR REACTIONS 177Hf(n, n), (n, γ), E=3-700 eV; measured total σ(E). 178Hf deduced resonances, level-width.
doi: 10.1103/PhysRevC.11.2022
1975LI15 Phys.Rev. C12, 102 (1975) H.I.Liou, J.Rainwater, G.Hacken, U.N.Singh Neutron Resonance Spectroscopy: 203,205Tl NUCLEAR REACTIONS 203,205Tl(n, n), (n, γ), E=15 eV-104 keV; measured σ(E). 203,204,205,206Tl deduced resonances, Γ, L, J, π, S.
doi: 10.1103/PhysRevC.12.102
1975SI05 Phys.Rev. C11, 1117 (1975) U.N.Singh, J.Rainwater, H.I.Liou, G.Hacken, J.B.Garg Neutron Resonance Spectroscopy: Aluminum NUCLEAR REACTIONS 27Al(n, n), (n, γ), E=4-420 keV; measured total σ(E), σ(E, Eγ). 28Al deduced resonances, J, L, n-width, S.
doi: 10.1103/PhysRevC.11.1117
1974SI25 Phys.Rev. C10, 2138 (1974) U.N.Singh, H.I.Liou, G.Hacken, M.Slagowitz, F.Rahn, J.Rainwater, W.Makofske, J.B.Garg Neutron Resonance Spectroscopy: Chlorine NUCLEAR REACTIONS 35,37Cl(n, n), (n, γ), E=20 eV-400 keV; measured total σ(E). 36,38Cl deduced resonances, J, L, S, n-width.
doi: 10.1103/PhysRevC.10.2138
1974SI26 Phys.Rev. C10, 2143 (1974) U.N.Singh, H.I.Liou, J.Rainwater, G.Hacken, W.Makofske, J.B.Garg Neutron Resonance Spectroscopy: Calcium NUCLEAR REACTIONS 40Ca(n, n), (n, γ), E=0-550 keV; measured σ(E). 41Ca resonances deduced E, level-width, S.
doi: 10.1103/PhysRevC.10.2143
1974SI27 Phys.Rev. C10, 2147 (1974) U.N.Singh, H.I.Liou, J.Rainwater, G.Hacken, J.B.Garg Neutron Resonance Spectroscopy: Fluorine NUCLEAR REACTIONS 19F(n, n), (n, γ), E=0.5-200 keV; measured total σ(E). 20F resonances deduced L, J, level-width, S.
doi: 10.1103/PhysRevC.10.2147
1974SI28 Phys.Rev. C10, 2150 (1974) U.N.Singh, H.I.Liou, J.Rainwater, G.Hacken, J.B.Garg Neutron Resonance Spectroscopy: Magnesium NUCLEAR REACTIONS Mg(n, n), (n, γ), E approx 4 eV-500 keV; measured σ(E). 25,26,27Mg resonances deduced E, L, J, level-width, S.
doi: 10.1103/PhysRevC.10.2150
1973RA31 Phys.Rev. C8, 1827 (1973) F.Rahn, H.S.Camarda, G.Hacken, W.W.Havens, Jr., H.I.Liou, J.Rainwater, U.N.Singh, M.Slagowitz, S.Wynchank Neutron Resonance Spectroscopy. XIII. Na to 320 keV NUCLEAR REACTIONS 23Na(n, X), E=0-320 keV; measured σ(E). 24Na deduced resonances, J, L, level-width.
doi: 10.1103/PhysRevC.8.1827
1973SI32 Phys.Rev. C8, 1833 (1973) U.N.Singh, H.I.Liou, G.Hacken, M.Slagowitz, F.Rahn, J.Rainwater, W.Makofske, J.B.Garg Neutron Resonance Spectroscopy. XIV. Potassium NUCLEAR REACTIONS 39,41K(n, X), E=0-400 keV; measured σ(E). 40,42K deduced resonances, J, L, level-width. Natural K.
doi: 10.1103/PhysRevC.8.1833
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