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NSR database version of April 27, 2024.

Search: Author = B.C.Samanta

Found 9 matches.

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1991MA29      J.Phys.(London) G17, 1387 (1991)

M.M.Majumdar, B.C.Samanta, S.K.Samaddar

Energy-Dependent Nucleus-Nucleus Potential with the Paris Interaction

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca, ¹⁰⁹Ag, ²⁰⁸Pb(¹⁶O, ¹⁶O), ⁴⁰Ca, ²⁰⁸Pb(⁴⁰Ca, ⁴⁰Ca), ²⁰⁸Pb, ¹⁰⁹Ag(¹⁰⁹Ag, ¹⁰⁹Ag), ²⁰⁸Pb(²⁰⁸Pb, ²⁰⁸Pb), E not given; calculated nucleus-nucleus potential parameters; deduced energy dependence. Energy density formalism, frozen density approximation.

doi: 10.1088/0954-3899/17/9/012
Citations: PlumX Metrics

1990MA18      J.Phys.(London) G16, 713 (1990)

M.M.Majumdar, B.C.Samanta, S.K.Samaddar

Effect of Isobar on Nucleus-Nucleus Potential

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca), ¹⁰⁹Ag(¹⁰⁹Ag, ¹⁰⁹Ag), ²⁰⁸Pb(²⁰⁸Pb, ²⁰⁸Pb), E not given; calculated Woods-Saxon potential parameters. Lowest order Brueckner theory, effective interaction with, without isobar.

doi: 10.1088/0954-3899/16/5/008
Citations: PlumX Metrics

1988BA65      Nucl.Phys. A487, 175 (1988)

A.K.Banerjee, B.C.Samanta, S.K.Samaddar

Large-Scale Collective Motion in Heavy-Ion Collisions

NUCLEAR REACTIONS, ICPND ²⁸Si(²⁸Si, X), E(cm) ≈ 30-100 MeV; ⁴⁰Ca(⁴⁰Ca, X), E(cm) ≈ 60-200 MeV; calculated fusion σ(E). Classical dynamical model.

doi: 10.1016/0375-9474(88)90135-2
Citations: PlumX Metrics

1987SA42      J.Phys.(London) G13, L223 (1987)

S.K.Samaddar, A.K.Banerjee, B.C.Samanta

Shape Evolution in Collision between very Heavy Ions and Potential Pockets

NUCLEAR REACTIONS ²³⁸U(²³⁸U, X), E=700, 800 MeV; ²⁰⁸Pb(²⁰⁸Pb, X), E=650 MeV; calculated composite system shape features. Classical dynamical model.

doi: 10.1088/0305-4616/13/10/001
Citations: PlumX Metrics

1986SA01      Nucl.Phys. A451, 160 (1986)

S.K.Samaddar, M.M.Majumdar, B.C.Samanta, J.N.De

Vacuum Polarization and the Nuclear Mass Formula

NUCLEAR REACTIONS ¹⁰⁹Ag(¹⁰⁹Ag, X), E(cm) ≈ 227-237 MeV; calculated fusion σ(E); deduced vacuum polarization role.

doi: 10.1016/0375-9474(86)90249-6
Citations: PlumX Metrics

1985BA13      Phys.Lett. 153B, 213 (1985)

A.K.Banerjee, B.C.Samanta, S.K.Samaddar

Charge Polarization in Heavy-Ion Collisions

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁸Ni, X), ¹²⁰Sn(¹²⁰Sn, X), ²³⁸U(²³⁸U, X), E not given; calculated charge polarization potential vs separation distance. Droplet model, adiabatic approximation.

doi: 10.1016/0370-2693(85)90533-7
Citations: PlumX Metrics

1982SA14      Z.Phys. A306, 307 (1982)

S.K.Samaddar, B.C.Samanta, D.Sperber, M.Zielinska-Pfabe

Dynamical Model for Neck Formation in the Entrance Channel of a Heavy Ion Collision

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=186, 266, 506 MeV; ¹⁶O(¹⁶O, X), E=52, 84, 180 MeV; ⁸⁴Kr(⁸⁴Kr, X), E=460, 628, 1132 MeV; ²⁰⁸Pb(²⁰⁸Pb, X), E=1676, 2092, 3340 MeV; calculated neck radius vs L, E, mass, charge. Classical dynamical model.

doi: 10.1007/BF01432371
Citations: PlumX Metrics

1976GH01      Can.J.Phys. 54, 663 (1976)

M.K.Ghosh, S.R.Majumdar, B.C.Samanta

Ratio of Δ ² in Zirconium Isotopes

NUCLEAR STRUCTURE ^{84,86,88,92,94,96}Zr; calculated gap parameter, ground state energy.

doi: 10.1139/p76-073
Citations: PlumX Metrics

1975SA19      Indian J.Phys. 49, 198 (1975)

B.C.Samanta, P.K.Banerjee

Asymmetric Rotor Model with Angular-Momentum Dependent Moments of Inertia

NUCLEAR STRUCTURE ²⁴Mg, ⁵⁶Fe, ¹⁰²Ru, ¹⁰⁶Pd, ¹⁶⁰Dy, ^164,166,168Er, ¹⁶⁸Yb, ^184,186W, ¹⁹²Os, ^192,196Pt, ²²⁸Th, ²³⁴U, ²³⁸Pu, ²⁵⁴Fm; calculated rotational energies of positive parity levels.