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NSR database version of April 26, 2024.

Search: Author = K.C.Panda

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2014PA22      Pramana 82, 841 (2014)

K.C.Panda, B.C.Sahu, J.Bhoi

Accuracy of simple folding model in the calculation of the direct part of real α-α interaction potential

doi: 10.1007/s12043-014-0737-2
Citations: PlumX Metrics

2013PA26      Phys.Rev. C 88, 034602 (2013)

K.C.Panda, B.C.Sahu, R.K.Gupta

Spin-density contribution in the optical potential of open j-shell nuclei

NUCLEAR REACTIONS ²⁰Ne(¹⁶O, X), E(cm)=30.88 MeV; ⁴²Ca(¹⁶O, X), E(cm)=43.45 MeV; ⁴⁴Ca(¹⁶O, X), E(cm)=44 MeV; ⁵²Cr(¹⁶O, X), E(cm)=45.88 MeV; ⁵⁴Fe(¹⁶O, X), E(cm)=46.29 MeV; ⁵⁸Ni(¹⁶O, X), E(cm)=47.03 MeV; ⁶²Ni(¹⁶O, X), E(cm)=47.69 MeV; ⁶⁴Ni(¹⁶O, X), E(cm)=48 MeV; ⁷⁴Ge(¹⁶O, X), E(cm)=46.04 MeV; ⁷⁶Ge(¹⁶O, X), E(cm)=46.26 MeV; ⁹²Zr(¹⁶O, X), E(cm)=47.70 MeV; ⁶⁰Ni(¹⁸O, X), E(cm)=48.46 MeV; ⁶²Ni(¹⁸O, X), E(cm)=48.82 MeV; ⁶⁴Ni(¹⁸O, X), E(cm)=49.17 MeV; ⁷⁶Ge(¹⁸O, X), E(cm)=45.28 MeV; ³²S(²⁴Mg, X), E(cm)=68.57 MeV; ³⁶S(²⁴Mg, X), E(cm)=72 MeV; ³⁴S(³²S, X), E(cm)=49.97 MeV; ⁶²Ni(¹²C, X), E(cm)=40.22 MeV; ⁶⁴Ni(⁵⁸Ni, X), E(cm)=114.9 MeV; calculated energy-dependent real and imaginary parts of the optical potential of open j-shell nuclei, contribution of spin-density terms, effect of such contributions on elastic and sub-barrier fusion cross sections. Energy density model using the complex Skyrme III energy density.

doi: 10.1103/PhysRevC.88.034602
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2004SA08      Nucl.Phys. A733, 169 (2004)

P.K.Sahu, T.K.Jha, K.C.Panda, S.K.Patra

Hot nuclear matter in asymmetry chiral sigma model

doi: 10.1016/j.nuclphysa.2003.11.061
Citations: PlumX Metrics

1993SO16      J.Phys.(London) G19, 1929 (1993)

S.A.Sofianos, K.C.Panda, P.E.Hodgson

The Microscopic Alpha-Alpha Potential

NUCLEAR REACTIONS ⁴He(α, α), E(cm)=1, 10, 17 MeV; calculated microscopic potential. Skyrme effective interaction, folding, energy-density models.

doi: 10.1088/0954-3899/19/11/019
Citations: PlumX Metrics

1990PA11      J.Phys.(London) G16, 593 (1990)

K.C.Panda, T.Patra

Spin-Density Terms and Heavy-Ion Optical Potential

NUCLEAR REACTIONS ⁴⁸Ca(¹⁶O, ¹⁶O), E(cm)=42 MeV; ²⁰⁸Pb(¹⁶O, ¹⁶O), E(cm)=178.29 MeV; ²⁰⁸Pb(⁹⁰Zr, ⁹⁰Zr), E(cm)=90 MeV; ²⁰⁸Pb(²⁰⁸Pb, ²⁰⁸Pb), E(cm)=208 MeV; calculated model parameters. Optical potential, energy density model, complex Skyrme interaction.

doi: 10.1088/0954-3899/16/4/010
Citations: PlumX Metrics

1990PA19      Phys.Rev. C42, 1155 (1990)

K.C.Panda

Comment on ' Spin Density and the Real Part of the Heavy-Ion Potential '

NUCLEAR REACTIONS ⁴⁸Ca(¹⁶O, ¹⁶O), ⁹⁰Zr(¹⁶O, ¹⁶O), (⁴⁰Ca, ⁴⁰Ca), (⁴⁸Ca, ⁴⁸Ca), E not given; calculated potential real part spin-density contribution.

doi: 10.1103/PhysRevC.42.1155
Citations: PlumX Metrics

1988PA24      J.Phys.(London) G14, 1489 (1988)

K.C.Panda, T.Patra

Comparison of Folding Model and Energy Density Model for the Heavy-Ion Optical Potential

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca), E(cm)=120 MeV; calculated potential parameters vs internuclear distance. Folding, energy density models.

doi: 10.1088/0305-4616/14/12/011
Citations: PlumX Metrics

1985PA27      J.Phys.(London) G11, 1323 (1985)

K.C.Panda

A Simple Microscopic Approach to the Energy Dependence of the Real and Imaginary Parts of the Heavy-Ion Interaction Potential

NUCLEAR REACTIONS, ICPND ⁴⁰Ca(⁴⁰Ca, X), E(cm)=55-100 MeV; calculated fusion σ(E). ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca), E(cm)=71.8, 88, 93, 112.5, 120 MeV; ⁴⁰Ca(¹⁶O, ¹⁶O), E(cm)=28.57 MeV; calculated σ(θ); deduced potential parameters. Microscopic model.

doi: 10.1088/0305-4616/11/12/010
Citations: PlumX Metrics

1981PA09      J.Phys.(London) G7, 937 (1981)

K.C.Panda, B.Behera, R.K.Satpathy

Effects of Saturation, Antisymmetrisation and Energy Dependence on the Nucleus-Nucleus Interaction Potential

NUCLEAR REACTIONS ¹⁶O(¹⁶O, ¹⁶O), E=0, 100, 250, 500, 1000 MeV; calculated nucleus-nucleus potential. Finite-range effective interaction, saturation, antisymmetrization, energy dependence effects.

doi: 10.1088/0305-4616/7/7/016
Citations: PlumX Metrics

1980BE19      Phys.Rev. C21, 1883 (1980)

B.Behera, K.C.Panda, R.K.Satpathy

Imaginary Part of the Ion-Ion Interaction Potential

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca, ⁵⁶Ni(¹⁶O, ¹⁶O), ⁴⁰Ca, ⁵⁶Ni(⁴⁰Ca, ⁴⁰Ca), E(cm)=60 MeV; calculated ion-ion potential imaginary term.

doi: 10.1103/PhysRevC.21.1883
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1980BE25      Phys.Rev. C22, 148 (1980)

B.Behera, K.C.Panda, R.K.Satpathy

Energy Dependence of the Real Part of Ion-Ion Interaction Potential

NUCLEAR REACTIONS ¹⁶O(¹⁶O, ¹⁶O), E(cm)=0-1000 MeV; calculated ion-ion potential. Brueckner energy dependent formalism.

doi: 10.1103/PhysRevC.22.148
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1979BE32      Phys.Rev. C20, 683 (1979)

B.Behera, K.C.Panda, R.K.Satpathy

Simple Parametrization of the Energy Density and Calculations of the Real Part of the Ion-Ion Interaction Potential

NUCLEAR REACTIONS ¹⁶O, ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ²⁰⁸Pb(¹⁶O, X), ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ²⁰⁸Pb(⁴⁰Ca, X); calculated real part of ion-ion interaction potential, interaction barrier heights. Energy density functionals parametrized, Taylor expansion of two-body effective interactions.

doi: 10.1103/PhysRevC.20.683
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