NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = K.Krishan Found 47 matches. 2007DE46 Phys.Rev. C 76, 034608 (2007) A.Dey, C.Bhattacharya, S.Bhattacharya, S.Kundu, K.Banerjee, S.Mukhopadhyay, D.Gupta, T.Bhattacharjee, S.R.Banerjee, S.Bhattacharyya, T.K.Rana, S.K.Basu, R.Saha, K.Krishan, A.Mukherjee, D.Bandopadhyay, C.Beck Characterization of fragment emission in 20Ne(7-10 Mev/nucleon)+12C reactions NUCLEAR REACTIONS 12C(20Ne, X), E=7-10 MeV/nucleon; measured fragment inclusive energy distributions, yields and cross sections.
doi: 10.1103/PhysRevC.76.034608
2005BH09 Phys.Rev. C 72, 021601 (2005) C.Bhattacharya, A.Dey, S.Kundu, K.Banerjee, S.Bhattacharya, S.Mukhopadhyay, D.Gupta, T.Bhattacharjee, S.R.Banerjee, S.Bhattacharyya, T.Rana, S.K.Basu, R.Saha, S.Bhattacharjee, K.Krishan, A.Mukherjee, D.Bandopadhyay, C.Beck Survival of orbiting in 20Ne (7-10 MeV/nucleon) + 12C reactions NUCLEAR REACTIONS 12C(20Ne, X), E=145-200 MeV; measured fragment yields, charge distributions, energy spectra, σ(E, θ); deduced survival of orbiting mechanism. Comparison with equilibrium model predictions.
doi: 10.1103/PhysRevC.72.021601
2004BH03 Phys.Rev. C 69, 024607 (2004) C.Bhattacharya, S.Bhattacharya, T.Bhattacharjee, A.Dey, S.Kundu, S.R.Banerjee, P.Das, S.K.Basu, K.Krishan Dissipation of angular momentum in light heavy-ion collision NUCLEAR REACTIONS 27Al(16O, X), E=116 MeV; 27Al, 59Co(28Si, X), (20Ne, X), E=145 MeV; measured fragments energy spectra, σ(E, θ); deduced angular momentum dissipation effects.
doi: 10.1103/PhysRevC.69.024607
2003BB07 Pramana 61, 529 (2003) P.Banerjee, K.Krishan, S.Bhattacharya, C.Bhattacharya Fusion of light exotic nuclei at near-barrier energies: Effect of inelastic excitation NUCLEAR REACTIONS Pb(17F, X), E(cm)=80-100 MeV; Pb(11Be, X), E(cm)=30-50 MeV; calculated fusion σ; deduced role of inelastic and breakup channels. Coupled-channels approach, comparison with data.
doi: 10.1007/BF02705476
2002BA50 Eur.Phys.J. A 14, 53 (2002) D.Bandyopadhyay, C.Bhattacharya, K.Krishan, S.Bhattacharya, S.K.Basu, A.Chatterjee, S.Kailas, A.Shrivastava, K.Mahata Light-Charged-Particle Evaporation from Hot 31P Nucleus at E* ∼ 60 MeV NUCLEAR REACTIONS 24Mg(7Li, X), E=47 MeV; 12C(19F, X), E=96 MeV; measured light-charged particle spectra, σ(θ) following compound nucleus decay. Comparison with statistical model predictions.
doi: 10.1140/epja/iepja1269
2002BB07 Int.J.Mod.Phys. E11, 491 (2002) P.Banerjee, K.Krishan, S.Bhattacharya, C.Bhattacharya Fusion of Light Proton-Rich Exotic Nuclei at Near-Barrier Energies NUCLEAR REACTIONS Pb(17F, X), E(cm)=80-100 MeV; Pb(8B, X), E(cm)=40-60 MeV; calculated fusion σ. Coupled-channels calculation, comparison with data.
doi: 10.1142/S0218301302001034
2002BH05 Phys.Rev. C66, 047601 (2002) C.Bhattacharya, K.Mullick, S.Bhattacharya, K.Krishan, T.Bhattacharjee, P.Das, S.R.Banerjee, D.N.Basu, A.Ray, S.K.Basu, M.B.Chatterjee Dissipative collisions in 16O +27Al at Elab = 116 MeV NUCLEAR REACTIONS 27Al(16O, X), E=116 MeV; measured fragments isotopic yields, energy and angular distributions; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.66.047601
2001BB02 Phys.Rev. C64, 064613 (2001) D.Bandyopadhyay, C.Bhattacharya, K.Krishan, S.Bhattacharya, S.K.Basu, A.Chatterjee, S.Kailas, A.Shrivastava, K.Mahata Exclusive Light Particle Measurements for the System 19F + 12C at 96 MeV NUCLEAR REACTIONS 12C(19F, xnypzα), E=96 MeV; measured Ep, Eα, σ(E, θ). 31P deduced hot compound nucleus decay features. Comparison with statistical model predictions.
doi: 10.1103/PhysRevC.64.064613
2000DH01 Eur.Phys.J. A 7, 209 (2000) A.K.Dhara, S.Bhattacharya, K.Krishan Dissipative Dynamics of Fission in the Framework of Asymptotic Expansion of Fokker-Planck Equation NUCLEAR REACTIONS 154Sm, 197Au, 238U(18O, F), E=158.8 MeV; calculated prescission neutron multiplicity vs fission fragment mass asymmetry, meanenergy of evaporated neutrons, fission fragment kinetic energy. 124Sn(16O, F), E not given; calculated time evolution of stochastic variables. Comparison with data from compound nuclei produced by different nuclear reactions.
doi: 10.1007/s100500050383
1999BA11 Phys.Rev. C59, 1179 (1999) D.Bandyopadhyay, S.K.Basu, C.Bhattacharya, S.Bhattacharya, K.Krishan, A.Chatterjee, S.Kailas, A.Navin, A.Shrivastava Evaporation of α Particles from the 31P Nucleus NUCLEAR REACTIONS 12C(19F, α), E=96 MeV; measured α spectra, σ(Eα, θ); deduced statistical model parameters, compound nucleus deformation.
doi: 10.1103/PhysRevC.59.1179
1998DH01 Phys.Rev. C57, 2453 (1998) A.K.Dhara, K.Krishan, C.Bhattacharya, S.Bhattacharya Dynamical Study of Fission Process and Estimation of Prescission Neutron Multiplicity
doi: 10.1103/PhysRevC.57.2453
1997BH05 Phys.Rev. C56, 212 (1997) Structure of One Neutron Halo Light Nuclei 11Be and 19O NUCLEAR STRUCTURE 11Be, 19O; calculated levels, rms charge radii; deduced contribution of odd particle. Particle-vibration coupling model, comparison with experiment.
doi: 10.1103/PhysRevC.56.212
1996BH02 Phys.Rev. C53, 1012 (1996) C.Bhattacharya, S.Bhattacharya, K.Krishan Prescission Neutron Multiplicities and Nuclear Viscosity: A systematic study NUCLEAR REACTIONS 134Ba(24Mg, F), 126Te(32S, F), E=180 MeV; 108Pd(50Ti, F), E=216 MeV; 142Nd(16O, F), E=100-207 MeV; 150Sm(16O, F), E=108-166 MeV; 170Er(28Si, F), E=135-165 MeV; 181Ta(19F, F), E=95-135 MeV; calculated prescission neutron multiplicity, viscosity coefficient, fission fragment average kinetic energy. Simple dynamical fission model, Euler-Lagrange equations based trajectories.
doi: 10.1103/PhysRevC.53.1012
1996BH06 Phys.Rev. C54, 3099 (1996) C.Bhattacharya, D.Bandyopadhyay, S.K.Basu, S.Bhattacharya, K.Krishan, G.S.N.Murthy, A.Chatterjee, S.Kailas, P.Singh Intermediate Mass Fragments Emission in the Reaction 96 MeV 19F on 12C NUCLEAR REACTIONS 12C(19F, X), E=96 MeV; measured σ(fragment θ, E), fission-like yields charge distributions. 27Al(α, X), E=60 MeV; 24Mg(7Li, X), E=47 MeV; analyzed data; deduced no entrance channel asymmetry dependence.
doi: 10.1103/PhysRevC.54.3099
1995BH03 Phys.Rev. C52, 798 (1995) C.Bhattacharya, D.Bandyopadhyay, G.S.N.Murthy, Y.P.Viyogi, S.K.Basu, K.Krishan, S.Bhattacharya, S.Kailas, A.Chatterjee, P.Singh Intermediate Mass Fragments Emission in the Reaction 47 MeV 7Li + Mg NUCLEAR REACTIONS Mg(7Li, X), E=47 MeV; measured σ(E, θ) for fragment Z=4-9; deduced moving source parameters, fragment average kinetic energies, total elemental σ. Binary fragmentation model analysis.
doi: 10.1103/PhysRevC.52.798
1995DA28 Z.Phys. A353, 49 (1995) S.Datta, K.Krishan, S.Bhattacharya Entrance Channel Effects on Preequilibrium Emission and Incomplete Fusion in Promptly Emitted Particle Model NUCLEAR REACTIONS 46Ti, 60Ni, 120Sn, 197Au(16O, xp), E=403 MeV; 46Ti, 120Sn, 197Au(32S, X), E=680 MeV; analyzed σ(θ, Ep), proton multiplicity data; deduced entrance channel effects role. Incomplete fusion, preequilibrium emission, promptly emitted particle model.
doi: 10.1007/BF01297727
1994BH03 Phys.Rev. C49, 3147 (1994) C.Bhattacharya, S.Bhattacharya, K.Krishan Intermediate Mass Fragment Yields from Fusion and Non-Fusion Processes in Nucleus-Nucleus Collisions in Fermi Energy Domain: An integrated dynamical approach NUCLEAR REACTIONS 197Au(40Ar, X), E=1.2 GeV; 109Ag(20Ne, X), E=0.8 GeV; calculated fusion probability vs impact parameter. 109Ag(20Ne, X), E=0.8 GeV; 197Au(40Ar, X), E=1.2 GeV; calculated fragment average kinetic-energy loss vs impact parameter, intermediate mass fragment emission σ vs Z. Other reactions studied, intergrated dynamical approach.
doi: 10.1103/PhysRevC.49.3147
1993BH03 Phys.Rev. C48, 577 (1993) Isotopic Variation of the rms Charge Radii of Ca Isotopes NUCLEAR STRUCTURE 40,42,44,46,48Ca; calculated charge distribution, rms charge radii. Woods-Saxon type one-body potential, experimental occupation probabilities.
doi: 10.1103/PhysRevC.48.577
1993BH07 Z.Phys. A346, 281 (1993) C.Bhattacharya, S.Bhattacharya, K.Krishan Phenomenological Analysis of Intermediate Mass Fragments Emission in Alpha Induced Reactions NUCLEAR REACTIONS 27Al(α, X), E=60 MeV; 46Ti(α, X), E=104 MeV; analyzed σ(fragment θ, E) for X=Li, Be, B, N. Phenomenological moving source model.
1993DH02 Phys.Rev. C48, 1910 (1993) A.K.Dhara, C.Bhattacharya, S.Bhattacharya, K.Krishan Mechanism of Intermediate Mass Fragment Emission at Low Energy NUCLEAR REACTIONS 40Ca(16O, F), E=806 MeV; 24Mg(23Na, F), E=89 MeV; 24Mg(32S, F), E=141 MeV; calculated symmetric fission total, saddle-to-scission time. 40Ca(16O, F), E ≈ 70-88 MeV; calculated symmetric fission fragment relative yields, average kinetic energy.
doi: 10.1103/PhysRevC.48.1910
1992KR04 Phys.Rev. C45, 2379 (1992) K.Krishan, P.Wagner, J.P.Coffin, F.Rami, S.Bhattacharya Preequilibrium to Evaporation Residues: Dynamical approach to intermediate energy nucleus-nucleus collisions NUCLEAR REACTIONS 24Mg(40Ar, X), E=1100 MeV; calculated lost nucleon total number, projectile, target temperature vs time, proton yield vs fragment mass, proton velocity vs fragment mass; 40Ar(13C, X), E=1100 MeV; calculated σ(fragment θ) vs fragment charge. 40Ar(13C, pX), E=1100 MeV; calculated σ(fragment θ, Ep, θp); deduced reaction mechanism phase transition. Nucleus-nucleus collisions dynamical evolution, preequilibrium, evaporation processes.
doi: 10.1103/PhysRevC.45.2379
1992KR09 Nucl.Phys. A542, 159 (1992) K.Krishan, S.Bhattacharya, J.N.De, S.K.Samaddar Distribution of Angular Momentum in Incomplete Fusion Reaction NUCLEAR REACTIONS 27Al(84Kr, X), E=20, 30 MeV/nucleon; calculated prompt particle average number vs incident L, incompletely fused composites mass, excitation energy, angular momentum distribution. Dynamic trajectory model, particle exchange dissipation, Monte Carlo simulation technique.
doi: 10.1016/0375-9474(92)90404-8
1992RA12 Phys.Rev. C46, 366 (1992) B.Rastegar, P.Wagner, M.Bozin, J.P.Coffin, P.Fintz, G.Guillaume, F.Jundt, K.Krishan, F.Rami, A.Malki, M.Zahar In-Plane Particle-Residue Correlations in the 40Ar(1100 MeV) + 24Mg Reaction NUCLEAR REACTIONS 24Mg(40Ar, X), E=1100 MeV; measured (light particle)(residue) correlations, (complex particle)(residue) correlations; deduced information on preequilibrium, evaporation emissions, complex particle emission role. Fermi jet, statistical binary fission models.
doi: 10.1103/PhysRevC.46.366
1992SA20 Pramana 39, 117 (1992) H.K.Sahu, M.C.Valsakumar, B.Panigrahi, K.G.M.Nair, K.Krishan Solid State Effects During Deuterium Implantation into Copper and Titanium NUCLEAR REACTIONS 2H(d, n), E=low; measured asymptotic neutron yield, fusion reaction; deduced solid state effects role during d implantation into Cu, Ti.
doi: 10.1007/BF02857501
1991BH05 Phys.Rev. C44, 1049 (1991) C.Bhattacharya, S.K.Basu, S.Bhattacharya, A.Chakrabarti, S.Chattopadhyaya, M.R.Duttamajumdar, K.Krishan, G.S.N.Murthy, B.Sinha, M.D.Trivedi, Y.P.Viyogi, S.K.Datta, R.K.Bhowmik Heavy Fragment Emission in Alpha-Induced Reactions on Aluminum at 60 MeV NUCLEAR REACTIONS 27Al(α, X), E=60 MeV; measured σ(fragment E, θ) for X=Li, Be, B, C, N, O; deduced phenomenological moving source model parameters, exit channel deformation. Statistical binary fragmentation model calculations.
doi: 10.1103/PhysRevC.44.1049
1991KR11 Z.Phys. A339, 531 (1991) Residual Velocity Distributions in Complete and Incomplete Fusion Reactions NUCLEAR REACTIONS 24Mg(40Ar, X), E=0.6-1.1 GeV; calculated residual velocity distribution. Sequential binary decay model.
doi: 10.1007/BF01288437
1991MA30 Z.Phys. A339, 283 (1991) A.Malki, J.P.Coffin, G.Guillaume, F.Jundt, K.Krishan, F.Rami, P.Wagner, P.Fintz, M.Zahar, M.Gonin, B.Heusch, M.Ohta, B.Rastegar, F.Merchez, J.Mistretta, S.Kox Preequilibrium Versus Thermalized Light-Charged Particle Emissions in the 40Ar(1100 MeV) + 24Mg Reaction. Dynamical Calculations NUCLEAR REACTIONS 24Mg(40Ar, X), E=1100 MeV; measured fragment yield, (fragment)(fragment)(θ); deduced light particle emission processes separation. Light-heavy fragment coincidence, p, d, t, α particle detected.
doi: 10.1007/BF01284066
1989BH03 Phys.Rev.Lett. 62, 2589 (1989) S.Bhattacharya, J.N.De, K.Krishan, S.K.Samaddar Role of Two-Body Collisions in Limiting Momentum Transfer and Energy Deposition in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 40Ca(14N, X), 56Fe(20Ne, X), 90Zr(32S, X), E=10-50 MeV/nucleon; calculated linear momentum transfer, temperature vs E. Promptly emitted particle model.
doi: 10.1103/PhysRevLett.62.2589
1989BH05 Phys.Rev. C40, 1814 (1989) Energetic Proton Spectra in the Promptly-Emitted-Particle Model NUCLEAR REACTIONS 90Zr, 27Al, 197Au(16O, pX), E=215, 310 MeV; calculated σ(θp, Ep). Promptly emitted particle model.
doi: 10.1103/PhysRevC.40.1814
1989KR04 Nucl.Phys. A495, 65c (1989) K.Krishan, S.Bhattacharya, J.N.De, S.K.Samaddar Saturation of Energy Deposition and Linear Momentum Transfer in Heavy Ion Collisions NUCLEAR REACTIONS 56Fe(20Ne, X), 90Zr(32S, X), 40Ca(14N, X), E ≤ 10 MeV/nucleon; calculated fractional linear momentum transfer vs E. Prompt emission model.
doi: 10.1016/0375-9474(89)90308-4
1988BH06 Phys.Rev. C37, 2916 (1988) S.Bhattacharya, K.Krishan, S.K.Samaddar, J.N.De Realistic Estimates for Promptly Emitted Particles NUCLEAR REACTIONS 165Ho(20Ne, xn), E=220, 292, 402 MeV; 165Ho(12C, xn), E=300 MeV; calculated promptly emitted multiplicities.
doi: 10.1103/PhysRevC.37.2916
1988CH28 Nucl.Phys. A485, 181 (1988) A.K.Chaudhuri, S.Bhattacharya, K.Krishan Nucleon Transfer Contribution to the Absorptive Heavy Ion Potential by the Monte Carlo Simulation Method NUCLEAR REACTIONS 40Ca(16O, X), E=55.6-214.1 MeV; 58Ni(16O, X), E=45-81 MeV; 208Pb(16O, X), E=129-312.6 MeV; 28Si(16O, X), E=36-81 MeV; 88Sr(16O, X), E=59 MeV; 40Ca(40Ca, X), E=143.6-240 MeV; 40Ca(20Ne, X), E=151 MeV; 209Bi(136Xe, X), E=940, 1130 MeV; calculated potential parameters, nucleon transfer contribution to imaginary term. Monte-Carlo simulation.
doi: 10.1016/0375-9474(88)90529-5
1988KR13 J.Phys.(London) G14, 1423 (1988) K.Krishan, S.K.Samaddar, J.N.De Spin Dispersion and Alignment in Deep Inelastic Collisions NUCLEAR REACTIONS 209Bi(86Kr, X), E=610 MeV; 238U(86Kr, X), E=730 MeV; 154Sm(32S, X), E=214 MeV; calculated fragment angular momentum gain vs incident L, spin variances vs energy loss. Stochastic nucleon exchange model.
doi: 10.1088/0305-4616/14/11/013
1987BA01 Nucl.Phys. A462, 587 (1987) D.Bandyopadhyay, S.R.Samaddar, K.Krishan, J.N.De Energy Dependent Nucleus-Nucleus Potential in Heavy Ion Collisions NUCLEAR REACTIONS 208Pb, 16O(16O, 16O), 208Pb(208Pb, 208Pb), E=0-40 MeV/nucleon; calculated nucleus-nucleus potential parameters. 27Al(16O, X), E(cm) ≈ 50-100 MeV; 17O(13C, X), E(cm) ≈ 8-50 MeV; 26Mg(20Ne, X), E(cm) ≈ 8-50 MeV; 27Al(32S, X), E ≈ 33-500 MeV; 109Ag(40Ar, X), E(cm) ≈ 100-500 MeV; calculated fusion σ(E). Proximity model.
doi: 10.1016/0375-9474(87)90407-6
1987BA57 Phys.Lett. 196B, 424 (1987) D.Bandopadhyay, S.K.Samaddar, K.Krishan, J.N.De Spectator Recoil and Nucleon Emission Spectra in Intermediate-Energy Nuclear Collisions NUCLEAR REACTIONS 124Sn(40Ar, X), E=44 MeV/nucleon; 197Au(12C, X), E=85 MeV/nucleon; calculated σ(E(p), θ(p)), σ(fragment θ, E), X(A)=70-130. Hot-zone model.
doi: 10.1016/0370-2693(87)90794-5
1987SA43 J.Phys.(London) G13, L231 (1987) S.K.Samaddar, K.Krishan, J.N.De Role of Barrier on Spin Orientation in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 209Bi(86Kr, X), E=610 MeV; calculated fragment spin orientation. Stochastic nucleon exchange model.
doi: 10.1088/0305-4616/13/10/002
1986BH08 Z.Phys. A325, 79 (1986) S.Bhattacharyya, J.N.De, S.K.Samaddar, K.Krishan Mass and Charge Distributions with Correlated Exchange NUCLEAR REACTIONS 56Fe(56Fe, X), 166Er, 139La(86Kr, X), E not given; calculated energy loss-mass variance correlation, inclusive variances isospin correlation coefficient dependence. Correlated nucleon exchange model.
1985DE44 Nucl.Phys. A445, 173 (1985) J.N.De, K.Krishan, S.K.Samaddar The Effect of the Shell Gap in Strongly Damped Collisions NUCLEAR REACTIONS 209Bi(56Fe, X), E=465 MeV; 144Sm(144Sm, X), E=6.95 MeV/nucleon; 209Bi(136Xe, X), E=940 MeV; 208Pb(208Pb, X), E=7.6 MeV/nucleon; calculated fragment charge variance energy dependence. 238U, 165Ho(56Fe, X), E=465 MeV; calculated fragment energy loss, charge variance correlation.
doi: 10.1016/0375-9474(85)90367-7
1985SA08 Phys.Rev. C31, 1053 (1985) S.K.Samaddar, J.N.De, K.Krishan Thermal Equilibrium in Strongly Damped Collisions NUCLEAR REACTIONS 238U, 165Ho(56Fe, X), E=465 MeV; calculated fragment charge centroids, variances, energy division. Nucleon exchange model, Monte-Carlo simulation.
doi: 10.1103/PhysRevC.31.1053
1984DE41 J.Phys.(London) G10, L257 (1984) J.N.De, K.Krishan, S.K.Samaddar The Mass and Charge Variances in Sm + Sm Collisions NUCLEAR REACTIONS 154Sm(154Sm, X), E=970 MeV; 144Sm(144Sm, X), E=1000 MeV; calculated charge, mass variances.
doi: 10.1088/0305-4616/10/2/016
1982DE01 Phys.Rev.Lett. 48, 81 (1982) J.N.De, S.K.Samaddar, K.Krishan Role of Stochastic Transfer of Nucleons for Angular Momentum Misalignment in Nuclear Collisions NUCLEAR REACTIONS 238U(86Kr, X), E=730 MeV; calculated target angular momentum gain, alignment factor vs (L), energy loss. Stochastic nucleon transfer, Pauli effect.
doi: 10.1103/PhysRevLett.48.81
1980MU03 Phys.Rev.Lett. 44, 1391 (1980) P.Mukherjee, K.Krishan, G.Banerjee Revised Shell Structure of 208Pb and its Effect on the Magicity of the Superheavy Nuclei NUCLEAR STRUCTURE 208Pb, 298Fl, 382154, 412154, 462154; calculated neutron-proton binding energies; deduced shell closure in superheavy. Core polarization, Woods-Saxon potential.
doi: 10.1103/PhysRevLett.44.1391
1979BH04 Phys.Rev. C20, 400 (1979) 1h11/2 States in 93,95Zr NUCLEAR STRUCTURE 93,95Zr; calculated fragmentation of 1h11/2 neutron single particle strength. Semi-microscopic model coupling neutron quasiparticle to phonon states of even-even core.
doi: 10.1103/PhysRevC.20.400
1978KR10 Phys.Rev. C18, 1026 (1978) Quasiparticle-Phonon Coupling Model Calculations for Odd-A Nb Isotopes NUCLEAR STRUCTURE 93,95,97Nb; calculated levels, J, π, B(E2).
doi: 10.1103/PhysRevC.18.1026
1976KR06 Phys.Rev. C13, 2055 (1976) Level Structure of the Odd-A Rb Isotopes NUCLEAR STRUCTURE 83,85Rb; calculated levels, J, π, B(E2), B(M1), T1/2, γ-branching. Quasiparticle-phonon coupling.
doi: 10.1103/PhysRevC.13.2055
1976KR12 Phys.Rev. C14, 758 (1976) Level Structure of 85,87Y NUCLEAR STRUCTURE 85,87Y; calculated levels, J, π, S, B(E2), B(M1). Quasiparticle-phonon coupling.
doi: 10.1103/PhysRevC.14.758
1976PA19 Nucl.Phys. A272, 365 (1976) Analogue Resonance in 51V(p, n)51Cr NUCLEAR STRUCTURE 52V; calculated IAS parameters.
doi: 10.1016/0375-9474(76)90338-9
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