NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.S.Verma Found 9 matches. 2024RA11 J.Phys.(London) G51, 035104 (2024) A.K.Rana, S.Sihotra, H.P.Sharma, V.Singh, G.H.Bhat, S.Jehangir, J.A.Sheikh, N.Rather, Kuldeep, N.Singh, R.K.Bhowmik, R.Kumar, R.P.Singh, S.Muralithar, P.Chauhan, D.S.Verma, T.Trivedi, S.Kumar, R.Palit, D.Mehta Level structures of 96Tc and their microscopic description NUCLEAR REACTIONS 75As(28Si, 3n4p)96Tc, E=120 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, energy level, J, π, partial level scheme, high-spin states, DCO and IPDCO ratios, multipolarities. Comparison with the framework of triaxial projected shell model calculations. The 15UD Pelletron accelerator facility at inter university accelerator centre (IUAC), New Delhi.
doi: 10.1088/1361-6471/ad1f2e
2024VE01 At.Data Nucl.Data Tables 155, 101619 (2024) Bulk and neutron-proton asymmetry coefficients of the semi-empirical mass formula tuned to ground state mass excess of AME2020 and/or FRDM(2012) NUCLEAR STRUCTURE Z=1-133; analyzed available data; calculated mass excess using the semi-empirical mass formula of Davidson et al. with/without nuclear shape and shell effects does not reproduce the ground state mass excesses of the new atomic mass evaluation data AME2020 and/or FRDM(2012) with its coefficients at zero temperature.
doi: 10.1016/j.adt.2023.101619
2024VE03 J.Radioanal.Nucl.Chem. 333, 1443 (2024) Correlation of intrinsic fusion barriers and evaporation residue cross-sections of SHEs NUCLEAR REACTIONS 238U(48Ca, X)286Cn, 242Pu(48Ca, X)290Fl, 243Am(48Ca, X)291Mc, E not given; 248Cm(51V, X)299119, E=234, 237 MeV; 249Cf(50Ti, X)299120, E=225 MeV; analyzed available data; deduced a correlation between the variation of the intrinsic fusion barrier with incident energy and the measured excitation function of fusion-evaporation residue σ, the optimum energy estimates for undiscovered superheavy elements.
doi: 10.1007/s10967-023-09043-8
2022VE02 Int.J.Mod.Phys. E31, 2250042 (2022) D.S.Verma, Kushmakshi, P.Chauhan, Vivek Angular momentum effects on the decay modes of hot compound nuclei formed in 86Kr + 134, 138Ba reactions NUCLEAR REACTIONS 134,138Ba(86Kr, X)220U/224U, E=4.5 MeV/nucleon; calculated σ; deduced different responses of the preformation probability to the angular momentum variation is different for the fragments of various mass regions.
doi: 10.1142/S0218301322500422
2021VE02 Nucl.Phys. A1007, 122129 (2021) Investigation of the cold valley paths for the synthesis of isotopes of Ubh in optimum orientations NUCLEAR REACTIONS 176Yb(138Ba, X), 194Os(132Sn, X), 246Cf(68Ni, X), 256Cf(70Ni, X)314126/326126, E not given; analyzed available data; calculated shell closures, preformation probabilities, neutron evaporation σ.
doi: 10.1016/j.nuclphysa.2020.122129
2020VE02 Nucl.Phys. A995, 121690 (2020) Angular momentum as a probe for the reaction mechanism: The 88Mo* decay at three excitation energies
doi: 10.1016/j.nuclphysa.2019.121690
2020VE04 Phys.Atomic Nuclei 83, 407 (2020) Decay of Hot and Rotating 88Mo* at Incident Energies of 300, 450, and 600 MeV
doi: 10.1134/S1063778820030151
2020VE06 Nucl.Phys. A1003, 122031 (2020) Fission partition a reflection of shell closures: Decay of 220, 224U* at eight excitation energies NUCLEAR REACTIONS 134,138Ba(86Kr, X)220U/224U, E not given; calculated fission barrier, Mass distribution of the decay/fission σ for the compound systems, fragment σ. Comparison with available data.
doi: 10.1016/j.nuclphysa.2020.122031
2019VE04 Nucl.Phys. A989, 117 (2019) Isospin influence on the decay of compound nuclei formed in 78, 82Kr + 40Ca and 78, 86Kr + 40, 48Ca reactions NUCLEAR REACTIONS 40Ca(78Kr, x)118Ba, E=5.5 MeV/nucleon;40Ca(82Kr, x)122Ba, E=5.5 MeV/nucleon; 40,48Ca(78Kr, x), 118Ba;(86Kr, x)134Ba, E=10 MeV/nucleon; calculated scattering potential of the decay channel, fragmentation potential for compound systems 118,122,134Ba for different angular momenta, fragment preformation probability, preformation probability for light projectiles, IMFs and FFs; σ for possible reactions, fragment mass distributions; deduced separately σ values for neutron-rich and neutron-poor systems. Cross sections compared with published data.
doi: 10.1016/j.nuclphysa.2019.06.002
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