NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = S.K.Gupta Found 56 matches. 2016GH02 J.Radioanal.Nucl.Chem. 307, 1481 (2016) R.Ghosh, S.Badwar, B.M.Lawriniang, V.Vansola, H.Naik, Y.Naik, S.V.Suryanarayana, N.S.Tawade, S.Padmakumar, S.C.Sharma, S.K.Gupta, B.Jyrwa, S.Ganesan, P.Singh, A.Goswa Determination of 110Cd(n, γ)111mCd and 111Cd(n, n')111mCd reaction cross-sections at the neutron energies of 1.12-4.12 MeV NUCLEAR REACTIONS 110Cd(n, γ), 111Cd(n, n'), E=1.12-4.12 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS 1.6 nuclear reaction code calculations, experimental data.
doi: 10.1007/s10967-015-4244-9
2015VA19 Radiochim.Acta 103, 817 (2015) V.Vansola, R.Ghosh, S.Badwar, B.M.Lawriniang, A.Gopalakrishna, H.Naik, Y.Naik, N.S.Tawade, S.C.Sharma, J.P.Bhatt, S.K.Gupta, S.Sarode, S.Mukherjee, N.L.Singh, P.Singh, A.Goswami Measurement of 197Au(n, γ)198gAu reaction cross-section at the neutron energies of 1.12, 2.12, 3.12 and 4.12-MeV NUCLEAR REACTIONS 197Au(n, γ), E=1.12, 2.12, 3.12, 4.12 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with EXFOR data, TALYS 1.6 nuclear model code calculations.
doi: 10.1515/ract-2015-2431
2007SH15 Pramana 68, 307 (2007) M.Sharma, V.Kumar, H.Kumawat, J.Adam, V.S.Barashenkov, S.Ganesan, S.Golovatiouk, S.K.Gupta, S.Kailas, M.I.Krivopustov, H.S.Palsania, V.Pronskikh, V.M.Tsoupko-Sitnikov, N.Vladimirova, H.Westmeier, W.Westmeier Measurement of neutron-induced activation cross-sections using spallation source at JINR and neutronic validation of the Dubna code NUCLEAR REACTIONS 232Th(n, γ), (n, 2n), 197Au(n, γ), (n, α), (n, 2n), (n, 4n), (n, 6n), (n, 7n), (n, 8n), (n, 6np), 59Co(n, α), (n, 2n), (n, 4n), (n, 5n), 181Ta(n, γ), (n, 2n), (n, 4n), (n, 5n), (n, np), E=spectrum; measured spectrum-averaged σ. Spallation neutrons from proton-induced reaction.
doi: 10.1007/s12043-007-0035-3
2005AD40 Kerntechnik 70, 127 (2005) J.Adam, V.S.Barashenkov, S.Ganesan, S.Golovatiouk, S.K.Gupta, S.Kailas, M.I.Krivopustov, V.Kumar, H.Kumawat, H.S.Palsania, V.Pronskikh, M.Sharma, V.M.Tsoupko-Sitnikov, N.Vladimirova, H.Westmeier, W.Westmeier Measurement of the neutron fluence on the spallation source at Dubna NUCLEAR REACTIONS 232Th, 197Au, 209Bi, 59Co, 115In, 181Ta(n, γ), (n, X), E<1 GeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, neutron fluence, σ. Comparison with the CASCADE code predictions.
doi: 10.3139/124.100234
2001SK01 Phys.Rev. D63, 014012 (2001) P.Skukla, A.K.Mohanty, S.K.Gupta Dynamical Growth of the Hadron Bubbles during the Quark-Hadron Phase Transition
doi: 10.1103/PhysRevD.63.014012
2000SH43 Phys.Rev. C62, 054904 (2000) P.Shukla, A.K.Mohanty, S.K.Gupta, M.Gleiser Inhomogeneous Nucleation in a Quark-Hadron Phase Transition
doi: 10.1103/PhysRevC.62.054904
1999SH10 Phys.Rev. C59, 914 (1999); Erratum Phys.Rev. C62, 039901 (2000) P.Shukla, S.K.Gupta, A.K.Mohanty Supercooling in Viscous Hydrodynamics for QCD Phase Transition
doi: 10.1103/PhysRevC.59.914
1997CH23 Phys.Rev. C56, 1171 (1997) Nucleus-Nucleus Elastic Scattering at Intermediate Energies: Glauber model approach NUCLEAR REACTIONS 12C(16O, 16O), E=139, 216, 311, 608, 1503 MeV; 40Ca, 90Zr, 208Pb(16O, 16O), E=1503 MeV; 208Pb(12C, 12C), E=1440 MeV; analyzed σ(θ); deduced effectiveness of Glauber model approach.
doi: 10.1103/PhysRevC.56.1171
1995GU16 Phys.Rev. C52, 3212 (1995) Trajectory Modifications in the Glauber Model for Heavy Ions NUCLEAR REACTIONS, ICPND 28Si(16O, X), E ≈ 50-250 MeV; calculated reaction σ(E). Other reactions σ discussed. Glauber model, trajectory modifications.
doi: 10.1103/PhysRevC.52.3212
1993CH30 Phys.Rev. C48, 1152 (1993) S.K.Charagi, S.K.Gupta, M.G.Betigeri, C.V.Fernandes, Kuldeep Elastic Scattering of 28Si from 27Al at 70, 80, 90, and 100 MeV NUCLEAR REACTIONS 27Al(28Si, 28Si), E=70-100 MeV; measured σ(E, θ); deduced reaction σ, optical model parameters. Different theoretical models.
doi: 10.1103/PhysRevC.48.1152
1992CH34 Phys.Rev. C46, 1982 (1992) Coulomb-Modified Glauber Model Description of Heavy-Ion Elastic Scattering at Low Energies NUCLEAR REACTIONS 62Ni(12C, 12C), E=48 MeV; 29Si(14N, 14N), E=39.8 MeV; 28Si(15N, 15N), E=44 MeV; 27Al(16O, 16O), E=46-49 MeV; 48Ca(32S, 32S), E=83.3 MeV; 40Ca(32S, 32S), E=100 MeV; 27Al(32S, 32S), E=100 MeV; 40Ca(16O, 16O), E=40-214 MeV; 48Ca(16O, 16O), E=40, 56 MeV; 235U(16O, 16O), E=140 MeV; 235U(20Ne, 20Ne), E=175, 252 MeV; 209Bi(40Ar, 40Ar), E=286, 340 MeV; analyzed σ(θ). Coulomb modified Glauber model.
doi: 10.1103/PhysRevC.46.1982
1991SI04 Phys.Rev. C43, 1867 (1991) P.Singh, A.Chatterjee, S.K.Gupta, S.S.Kerekatte Elastic Scattering of Alpha Particles from 209Bi at 24.8, 28.5, 34.7, 38.8, and 69.5 MeV NUCLEAR REACTIONS 209Bi(α, α), E=24-70 MeV; measured σ(θ); deduced model parameters.
doi: 10.1103/PhysRevC.43.1867
1990CH09 Phys.Rev. C41, 1610 (1990) Coulomb-Modified Glauber Model Description of Heavy-Ion Reaction Cross Sections NUCLEAR REACTIONS 208Pb(40Ar, X), E=6-44 MeV/nucleon; 208Pb(12C, X), E=6-30 MeV/nucleon; 58,62Ni(35Cl, X), E=80-160 MeV; 24Mg(32S, X), E=60-140 MeV; 40Ca, 59Co(16O, X), E=40-160 MeV; 40Ca(40Ca, X), E=120-180 MeV; 16O, 9Be(28Si, X), E=40-200 MeV; 90Zr(6Li, X), E=40-160 MeV; 27Al(32S, X), E=80-120 MeV; 40Ca(20Ne, X), E ≤ 80 MeV; 209Bi(84Kr, X), E=600-700 MeV; 238U, 209Bi(40Ar, X), E ≈ 250-350 MeV; 109Ag(40Ar, X), E=150-350 MeV; 58Ni(16O, X), E=50-300 MeV; 65Cu(84Kr, X), E=400-600 MeV; 209Bi(136Xe, X), E=700-1300 MeV; calculated reaction σ(E). Coulomb modified Glauber model.
doi: 10.1103/PhysRevC.41.1610
1989AN05 Ann.Nucl.Energy 16, 87 (1989) R.P.Anand, H.M.Jain, S.Kailas, S.K.Gupta, V.S.Ramamurthy Neutron Capture Cross Section Measurement of 232Th in the Energy Range of 400-900 keV NUCLEAR REACTIONS 232Th(n, γ), E=400-950 keV; measured capture σ(E). Activation analysis.
doi: 10.1016/0306-4549(89)90032-7
1988CH10 Phys.Rev. C37, 1420 (1988) A.Chatterjee, S.K.Gupta, S.Kailas, S.S.Kerekatte Alpha Scattering from 209Bi at 50.5 MeV NUCLEAR REACTIONS 209Bi(α, α), (α, α'), E=50.5 MeV; measured σ(E, θ); deduced optical model parameters, deformation lengths. Nearside-Farside decomposition, DWBA analysis, Notch test.
doi: 10.1103/PhysRevC.37.1420
1987GU03 Z.Phys. A326, 221 (1987) A New Macroscopic-Microscopic Description of the Double-Humped Fission Barriers NUCLEAR STRUCTURE 228Ra, 228Ac, 228Th, 229Pa, 234U, 238Np, 239Pu, 241Am, 243Cm, 248Bk, 250Cf, 254Es, 255Fm, 256Md, 257No, 259Lr, 261Rf; calculated binding energies; Z=90-98; calculated doubled-humped fission barriers, shell energies. New mass relation.
1986AN15 Radiat.Eff. 93, 189 (1986) R.P.Anand, H.M.Jain, S.Kailas, S.K.Gupta, V.S.Ramamurthy, S.S.Kapoor Neutron Capture Cross Section of Th-232 NUCLEAR REACTIONS 232Th(n, γ), E=400-935 keV; measured σ. Gold standard.
doi: 10.1080/00337578608207449
1986GU17 Indian J.Phys. 60A, 323 (1986) S.K.Gupta, R.K.Mohindra, H.K.Sahajwani Establishment of Shell Effects in (n, α) Cross-Sections at 14 MeV NUCLEAR STRUCTURE Z=17-22; analyzed σ(n, α); deduced shell effects.
1986KA22 Phys.Rev. C34, 357 (1986) Nucleus-Nucleus Potential from Fusion and Elastic Scattering NUCLEAR REACTIONS, ICPND 28Si(6Li, X), 9Be(12C, X), E(cm)=10-40 MeV; 12C(12C, X), E(cm)=10-30 MeV; calculated σ(E); deduced nucleus-nucleus potentials.
doi: 10.1103/PhysRevC.34.357
1986KA41 Radiat.Eff. 95, 157 (1986) Volume Integrals of Real and Imaginary Parts of Optical Potentials for Light Projectiles NUCLEAR REACTIONS 208Pb(p, p), (d, d), (t, t), (α, α), (3He, 3He), (6Li, 6Li), (n, n), E ≤ 50 MeV/nucleon; calculated optical potential real, imaginary part volume integrals. Empirical, global formulas.
doi: 10.1080/00337578608208685
1985GU11 Phys.Rev. C31, 1965 (1985) S.K.Gupta, S.Kailas, N.Lingappa, A.Shridhar Systematics in the Volume Integrals of the Imaginary Part of the Light Ion Optical Potentials NUCLEAR REACTIONS 12C(α, α), (3He, 3He), E=4-217 MeV; 12C(d, d), E=2-80 MeV; 12C(n, n), E=4-40 MeV; 12C(p, p), E=40-180 MeV; 12C(6Li, 6Li), E=12-156 MeV; 58Ni(6Li, 6Li), (3He, 3He), 208Pb(d, d), 90Zr(α, α), 208Pb(n, n), E ≤ 150 MeV; analyzed imaginary potential volume integral energy dependence; deduced global parameters.
doi: 10.1103/PhysRevC.31.1965
1985GU17 Indian J.Phys. 59A, 541 (1985) S.K.Gupta, R.K.Mohindra, H.K.Sahajwani Establishment of Shell Effects in (n, p) Cross Sections at 14 MeV NUCLEAR REACTIONS 44,48Ca, 40Ar, 48,47Ti, 60,62Ni, 64,66Zn, 56,58Fe, 70Ge, 112Sn, 124Te, 106Cd, 208Pb, 209Bi, 205Tl(n, p), E=14 MeV; analyzed σ; deduced shell effects role.
1985KA09 Pramana 24, 629 (1985) S.Kailas, S.K.Gupta, S.S.Kerekatte, C.V.Fernandes 51V(p, n)51Cr Reaction from E(p) 1-9 to 4-5 MeV RADIOACTIVITY 51Cr(EC) [from 51V(p, n)]; measured Eγ, Iγ. NUCLEAR REACTIONS, ICPND 51V(p, n), E=1.9-4.5 MeV; measured σ(E); deduced thermonuclear reaction rates. Direct neutron detection, activation technique, 4π neutron counter.
doi: 10.1007/BF02846732
1984CH15 Z.Phys. A317, 209 (1984) A.Chatterjee, S.Kailas, S.Saini, S.K.Gupta, M.K.Mehta Resonance Spectroscopy of 44Ti in the Excitation Energy Range 9.05 to 10.28 MeV NUCLEAR REACTIONS 40Ca(α, α), E=4.33-5.68 MeV; measured absolute σ(θ) vs E. 44Ti deduced resonances, J, π, Γα. R-matrix analysis.
doi: 10.1007/BF01421256
1984GU09 Z.Phys. A317, 75 (1984) Heavy-Ion Total Reaction Cross Sections NUCLEAR REACTIONS, ICPND 40Ca(6Li, 6Li), 59Co, 40Ca(16O, 16O), E=40-160 MeV; 28Si(9Be, 9Be), (16O, 16O), E=40-200 MeV; 40Ca(40Ca, 40Ca), E=120-240 MeV; 27Al(32S, 32S), E=70-120 MeV; 40Ca(20Ne, 20Ne), E ≈ 50-80 MeV; 209Bi(84Kr, 84Kr), E=600-700 MeV; 90Zr(6Li, 6Li), E=40-160 MeV; 208Pb(20Ne, 20Ne), E=100-250 MeV; 62,58Ni(35Cl, 35Cl), E=100-160 MeV; 24Mg(32S, 32S), E=60-140 MeV; 208Pb(16O, 16O), 235U(20Ne, 20Ne), E=100-300 MeV; 139La(86Kr, 86Kr), 208Pb(84Kr, 84Kr), E=300-700 MeV; 209Bi(136Xe, 136Xe), E=700-1300 MeV; 238U, 209Bi(40Ar, 40Ar), E=200-350 MeV; 65Cu(84Kr, 84Kr), E=300-600 MeV; 58Ni(16O, 16O), E=50-300 MeV; 109Ag(40Ar, 40Ar), E=150-350 MeV; analyzed data; deduced reaction σ(E). One parameter fit, strong absorption model.
doi: 10.1007/BF01420450
1984GU17 Phys.Rev. C30, 1093 (1984) Intrinsic Density and Energy Dependence: Exchange effects in alpha-nucleus scattering NUCLEAR REACTIONS 58Ni(α, α), E=172.5 MeV; calculated effective exchange interaction parameters; deduced density, energy dependences.
doi: 10.1103/PhysRevC.30.1093
1984JH01 Acta Phys.Acad.Sci.Hung. 55, 195 (1984) M.L.Jhingan, R.P.Anand, S.K.Gupta, M.K.Mehta Pre-Equilibrium Effect in (n, xn) Reactions NUCLEAR REACTIONS 89Y, 90Zr, 93Nb, 103Rh, 107Ag(n, 2n), (n, 3n), 151Eu, 169Tm, 175Lu, 181Ta, 191Ir, 197Au, 203Tl, 209Bi(n, 2n), (n, 3n), (n, 4n), E=threshold-28 MeV; 232Th, 238U(n, 2n), (n, 3n), E=threshold-20 MeV; calculated σ(E). Preequilibrium effect.
1984KA41 Pramana 23, 495 (1984) S.Kailas, S.K.Gupta, S.Bhattacharya, S.N.Chintalapudi, Y.P.Viyogi Elastic Scattering of 36 MeV Alpha Particles from 197Au NUCLEAR REACTIONS 197Au(α, α), E=36 MeV; measured σ(θ); deduced optical potential parameters.
doi: 10.1007/BF02846625
1984SH22 Phys.Rev. C30, 1760 (1984) A.Shridhar, N.Lingappa, S.K.Gupta, S.Kailas Systematics in the Volume Integrals of the Imaginary Part of the Alpha-Nucleus Optical Potentials NUCLEAR REACTIONS 12C, 27Al, 40Ca, 58Ni, 90Zr, 208Pb(α, α), E=0-200 MeV; calculated potential imaginary part volume integral systematics. Phenomenological optical model.
doi: 10.1103/PhysRevC.30.1760
1983CH28 Z.Phys. A313, 93 (1983) Angular Distributions in Pre-Equilibrium Reactions NUCLEAR REACTIONS 31P, 55Mn, 59Co, 93Nb, 127I, 181Ta, 197Au, 209Bi(n, xn), E=14.6 MeV; calculated σ(θ, En). Multi-step direct, compound emission differing emission rate angular dependence.
doi: 10.1007/BF02115846
1983KA02 Z.Phys. A309, 267 (1983) S.Kailas, S.K.Gupta, M.K.Mehta Intermediate Width Structures in the Reaction 50Ti(p, n)50V NUCLEAR REACTIONS 50Ti, 54Cr, 59Co(p, n), E=threshold-4.92 MeV; measured σ(total) vs E. 51V deduced intermediate resonances, parameters. Autocorrelation analysis.
doi: 10.1007/BF01413759
1982CH18 Z.Phys. A307, 269 (1982) Exciton Model Description of Energy Spectra following Pion Absorption in 40Ca NUCLEAR REACTIONS 40Ca(π-, n), (π-, d), (π-, t), (π-,3He), (π-, α), E at rest; calculated particle spectra. Exciton Model.
doi: 10.1007/BF01438648
1982KA23 Phys.Rev. C26, 830 (1982) S.Kailas, S.K.Gupta, M.K.Mehta, G.Singh Microscopic Nucleon Optical Model Potential at Low Energies NUCLEAR REACTIONS 27Al, 59Co, 115In, 197Au(n, n), E=8.05 MeV; analyzed σ(θ). 51V, 80Se, 65Cu, 119Sn(p, n), E=threshold-7 MeV; analyzed σ(total) vs E. Microscopic optical potential.
doi: 10.1103/PhysRevC.26.830
1982MU03 Z.Phys. A305, 73 (1982) K.H.N.Murthy, S.K.Gupta, A.Chatterjee Transmission Coefficients for Light Projectiles NUCLEAR REACTIONS 20Ne, 159Tb(n, n), E=2, 20, 36, 50 MeV; 89Y(n, n), E=8, 20, 36, 50 MeV; 209Bi(n, n), E=2, 20, 40, 50 MeV; 89Y, 159Tb(p, p), 20Ne(3He, 3He), E=8, 12, 20, 36, 50 MeV; 20Ne(p, p), (d, d), (t, t), E=2, 8, 20, 36, 50 MeV; 209Bi(p, p), (d, d), 197Au(t, t), 89Y(3He, 3He), E=12, 16, 20, 32, 50 MeV; 89Y, 159Tb(t, t), (d, d), E=8, 16, 20, 36, 50 MeV; 159Tb(3He, 3He), E=16, 20, 28, 36, 50 MeV; 144Nd(α, α), E=16, 20, 26, 38, 46 MeV; 197Au(3He, 3He), E=20, 24, 28, 36, 50 MeV; 20Ne(α, α), E=4, 8, 16, 30, 46 MeV; 85Rb(α, α), E=12, 18, 26, 38, 46 MeV; 206Pb(α, α), E=20, 24, 30, 38, 46 MeV; calculated transmission factors. 209Bi, 20Ne(n, X), (p, X), E=2, 20, 50 MeV; 209Bi, 20Ne(d, X), (t, X), E=8, 28, 50 MeV; 209Bi, 20Ne(3He, X), E=16, 28, 50 MeV; 20Ne, 206Pb(α, X), E=20, 30, 46 MeV; calculated σ(reaction). Global optical potentials.
doi: 10.1007/BF01415082
1981CH20 Pramana 16, 391 (1981) A.Chatterjee, K.H.N.Murthy, S.K.Gupta Optical Reaction Cross-Sections for Light Projectiles NUCLEAR REACTIONS 45Sc(n, n), (p, p), (d, d), (t, t), (3He, 3He), (α, α), E=1-50 MeV; calculated σ(E); 103Rh, 181Ta, 197Au(n, p), E=14 MeV; calculated σ(Ep). Empirical parametrization, evaporation preequilibrium models.
doi: 10.1007/BF02848235
1981CH22 Z.Phys. A301, 271 (1981) Closed Expressions for Mean Lifetimes in the Exciton Model NUCLEAR REACTIONS 46Ti(n, n'), (n, p), E=14.6 MeV; calculated σ(En'), σ(Ep). Exciton model, time-integrated Pauli mass equation.
doi: 10.1007/BF01416303
1981GU17 Z.Phys. A303, 329 (1981) Two-component equilibration in the exciton model of nuclear reactions
doi: 10.1007/BF01421531
1981KA33 Z.Phys. A302, 355 (1981) Empirical Description of Heavy-Ion Fusion Cross Sections NUCLEAR REACTIONS 40Ca, 27Al(16O, X), E(cm)=50-130 MeV; 14,15N, 19F(12C, X), E(cm)=10-30 MeV; 109Ag(40Ar, X), E(cm)=130-250 MeV; Cu(24Mg, X), E(cm)=110-250 MeV; 27Al(32S, X), E(cm)=30-60 MeV; 116,124Sn(35Cl, X), E(cm)=110-130 MeV; 235U(α, X), E(cm)=170-190 MeV; 198Pt(6Li, X), E(cm)=210-220 MeV; 27Al(35Cl, X), E(cm)=40-70 MeV; 152Sm(12C, X), E(cm)=50-60 MeV; 148Nd(16O, X), E(cm)=60-70 MeV; calculated σ(fusion, E). Empirical model, mass, geometrical dependences.
doi: 10.1007/BF01414268
1981MU07 Ann.Nucl.Energy 8, 299 (1981) Optical-Model Description of 14 MeV Neutron Cross Sections NUCLEAR REACTIONS 7Li, 9Be, 11B, 14N, 16O, 28Si, 40Ar, 56Fe, 181Ta, 209Bi(n, n), (n, X), E=14 MeV; analyzed σ(θ), σ(nonelastic), σ(total). Modified Wilmore-Hodgson potential.
doi: 10.1016/0306-4549(81)90096-7
1979CH15 Phys.Lett. 83B, 271 (1979) Fast Neutron Capture and the Microscopic Isovector Optical Potential NUCLEAR REACTIONS 89Y, Ce, 208Pb(n, γ), E=6-16 MeV; calculated σ. direct-semidirect model, complex microscopic optical potential.
doi: 10.1016/0370-2693(79)91105-5
1979JH01 Ann.Nucl.Energy 6, 495 (1979) M.L.Jhingan, R.P.Anand, S.K.Gupta, M.K.Mehta Semi-Empirical Approach for Predicting Neutron-Induced Fission Cross-Sections in the Energy Range, 1-18 MeV NUCLEAR REACTIONS 232,233Th, 233Pa, 235,238U, 237Np, 239Pu(n, F), E=1-18 MeV; calculated σ. Semi-empirical approach.
doi: 10.1016/0306-4549(79)90022-7
1979KA20 Phys.Rev. C20, 1272 (1979) S.Kailas, M.K.Mehta, S.K.Gupta, Y.P.Viyogi, N.K.Ganguly Proton Optical Model Potential at Sub-Coulomb Energies for Medium Weight Nuclei NUCLEAR REACTIONS 45Sc, 48Ca, 51V, 54Cr, 55Mn, 59Co, 61Ni, 65Cu, 71Ga, 75As, 80Se(p, n), E ≤ 5 MeV; analyzed σ; deduced optical model parameters.
doi: 10.1103/PhysRevC.20.1272
1978AG05 Prog.Theor.Phys. 60, 1922 (1978) Analysis of p-Wave Neutron-Reduced Widths COMPILATION 40Ar, 39K, 40Ca, 88Sr, 89Y, 93Nb, 92Mo, 103Rh, 207Pb, 209Bi, 232Th, 238U, 94,98Mo; analyzed data on p-wave neutron widths. Parker-Thomas model.
doi: 10.1143/PTP.60.1922
1978CI01 Phys.Rev. C17, 12 (1978) S.Cierjacks, S.K.Gupta, I.Schouky Isobaric Analog Impurity from Total and Differential Neutron Scattering Cross Sections of Silicon NUCLEAR REACTIONS 28Si(n, X), (n, n), E=1.05-1.40 MeV; measured total neutron σ(E), σ(E, θ). 29Si deduced resonances, J, π, Γ. R-matrix analyses.
doi: 10.1103/PhysRevC.17.12
1978GU06 Phys.Lett. 73B, 398 (1978) Real and Imaginary Parts of the Nucleus-Nucleus Interaction Using a Microscopic Approach NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=40 MeV; 40Ca(16O, 16O), E(cm)=30 MeV; calculated potential.
doi: 10.1016/0370-2693(78)90749-9
1978GU29 Nucl.Instrum.Methods 148, 77 (1978) Radiative Capture Cross Section Measurements For Fast Neutrons Using A Large Gd-Loaded Liquid Scintillator- NUCLEAR REACTIONS 197Au(n, γ), 238U(n, f), 238U(n, γ), E=1.6-2.4 MeV; measured products, 239U, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 21216.
doi: 10.1016/0029-554X(78)90338-5
1977RA21 Pramana 8, 478 (1977) M.A.Rahman, M.A.Awal, M.Rahman, H.M.Sengupta, S.K.Gupta High Resolution Gamma-Ray Spectroscopy of the 27Al(p, γ)28Si Resonance Reaction NUCLEAR REACTIONS 27Al(p, γ), E=2.4-2.75 MeV; measured Eγ, Iγ. 28Si deduced resonances, J, π, γ-branching.
doi: 10.1007/BF02862903
1976NA06 Phys.Rev. C13, 915 (1976) L.V.Namjoshi, S.K.Gupta, M.K.Mehta, S.S.Kerekatte Resonance Spectroscopy of 30Si Nucleus in the Excitation Energy Range 14.27 to 15.02 MeV NUCLEAR REACTIONS 26Mg(α, α), E=4.18-5.14 MeV; measured σ(E, θ). 28Si deduced resonances, J, π, Γα. R-matrix analysis.
doi: 10.1103/PhysRevC.13.915
1975GU22 Pramana 5, 37 (1975) S.K.Gupta, S.Saini, L.V.Namjoshi, M.K.Mehta Spectroscopy of 50V with (p, nγ) Reaction NUCLEAR REACTIONS 50Ti(p, nγ); measured Eγ, Iγ, γγ-coin. 50V deduced levels, J, π, γ-branching.
doi: 10.1007/BF02875150
1975KA31 Phys.Rev. C12, 1789 (1975) S.Kailas, S.K.Gupta, M.K.Mehta, S.S.Kerekatte, L.V.Namjoshi, N.K.Ganguly, S.Chintalapudi Total (p, n) Reaction Cross-Section Measurements on 50Ti, 54Cr, and 59Co NUCLEAR REACTIONS 54Cr(p, n), E=2.2-5.2 MeV; 50Ti(p, n), E=3.0-4.9 MeV; 59Co(p, n), E=2-5.1 MeV; measured total σ(E, En). 50V, 54Mn, 59Ni deduced average Γ. Optical model, Hauser-Feshbach analysis.
doi: 10.1103/PhysRevC.12.1789
1975RA04 Lett.Nuovo Cim. 12, 290 (1975) M.A.Rahman, M.A.Awal, M.Rahman, H.M.Sen Gupta, S.K.Gupta A Note on the Possible 4+ Analogue-Antianalogue States in 28Si NUCLEAR REACTIONS 27Al(p, γ), E > 2 MeV; measured σ(E, Eγ, θ). 28Si deduced resonance, J, π, L.
doi: 10.1007/BF02790602
1967IY02 Nucl.Phys. A93, 257(1967) K.V.K.Iyengar, B.Lal, S.K.Gupta, M.D.Deshpande A Search for the Level at 803 keV in 51Cr NUCLEAR REACTIONS 51V(p, nγ), E = 2.310-3.100 MeV; deduced threshold for 747 keV level of 51Cr; measured Iγ of 803 keV level w.r.t. Iγ of 747 keV level.
doi: 10.1016/0375-9474(67)90269-2
1967IY03 Nucl.Phys. A96, 417(1967) K.V.K.Iyengar, S.K.Gupta, B.Lal The Study of the 51V(p, n)51Cr Reaction NUCLEAR REACTIONS 51V(p, n), E = 2.3-5.5 MeV; measured σ(E, Eγ), σ(E;En, Eγ, θ(n), θ(γ)). 51Cr levels deduced J.
doi: 10.1016/0375-9474(67)90724-5
1967IY04 Nucl.Phys. A96, 521 (1967) K.V.K.Iyengar, S.K.Gupta, K.K.Sekharan, M.K.Mehta, A.S.Divatia Fluctuations in the Integrated Cross Section of the Reaction 45Sc(p, n)45Ti NUCLEAR REACTIONS 45Sc(p, n), E = 2.910-5.250 MeV; measured σ(E). 46Ti deduced mean level width. Natural target.
doi: 10.1016/0375-9474(67)90602-1
1967IY05 Nucl.Phys. A103, 592(1967) K.V.K.Iyengar, B.Lal, S.K.Gupta Gamma Rays from the Reaction 55Mn(p, nγ)55Fe NUCLEAR REACTIONS 55Mn(p, nγ) E=1.80-3.50 MeV; measured σ(E; Eγ, θ). 55Fe deduced levels. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(67)90925-6
1966IY01 Nucl.Phys. 76, 433(1966) K.V.K.Iyengar, S.K.Gupta, B.Lal, E.Kondaiah Study of the 37Cl(p, n)37Ar Reaction NUCLEAR REACTIONS 37Cl(p, nγ), E = 3.0-5.5 MeV; measured σ(E, Eγ), σ(E, En, t. Eta) 37Ar level deduced J. Natural target.
doi: 10.1016/0029-5582(66)90035-6
Back to query form |