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NSR database version of April 29, 2024.

Search: Author = C.P.Panos

Found 25 matches.

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2009MO11      Phys.Rev. C 79, 045806 (2009)

Ch.C.Moustakidis, C.P.Panos

Equation of state for β-stable hot nuclear matter

doi: 10.1103/PhysRevC.79.045806
Citations: PlumX Metrics


2005CH47      Int.J.Mod.Phys. E14, 653 (2005)

K.Ch.Chatzisavvas, C.P.Panos

Quantum-information content of fractional occupation probabilities in nuclei

NUCLEAR STRUCTURE 4He, 12C, 16O, 24Mg, 28Si, 32S, 40Ca; analyzed fractional occupation probabilities, information entropy.

doi: 10.1142/S0218301305003478
Citations: PlumX Metrics


2005MO40      Int.J.Mod.Phys. E14, 1087 (2005)

Ch.C.Moustakidis, K.Ch.Chatzisavvas, C.P.Panos

Theoretical quantum-information properties of nuclei and trapped Bose gases

NUCLEAR STRUCTURE 4He, 12C, 16O, 40Ca; calculated information entropy.

doi: 10.1142/S0218301305003739
Citations: PlumX Metrics


2001MO17      Phys.Rev. C64, 014314 (2001)

Ch.C.Moustakidis, S.E.Massen, C.P.Panos, M.E.Grypeos, A.N.Antonov

Evaluation of Cluster Expansions and Correlated One-Body Properties of Nuclei

NUCLEAR STRUCTURE 4He, 12C, 16O, 24Mg, 28Si, 32S, 40Ca; calculated momentum and density distributions, radii, entropy, related parameters. Three cluster expansions compared.

doi: 10.1103/PhysRevC.64.014314
Citations: PlumX Metrics


2001PA22      Phys.Rev. C63, 064307 (2001)

C.P.Panos, S.E.Massen, C.G.Koutroulos

Universal Trend of the Information Entropy of a Fermion in a Mean Field

NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated single-particle states information entropy.

doi: 10.1103/PhysRevC.63.064307
Citations: PlumX Metrics


2000GA47      Phys.Rev. C62, 054610 (2000)

Y.K.Gambhir, J.P.Maharana, G.A.Lalazissis, C.P.Panos, P.Ring

Temperature Dependent Relativistic Mean Field for Highly Excited Hot Nuclei

NUCLEAR STRUCTURE 168Er, 168Yb, 150Sm, 208Pb, 298Fl; calculated binding energies, radii, deformations vs temperature. Temperature-dependent relativistic mean field approach.

doi: 10.1103/PhysRevC.62.054610
Citations: PlumX Metrics


1998LA21      Int.J.Mod.Phys. E7, 485 (1998)

G.A.Lalazissis, S.E.Massen, C.P.Panos, S.S.Dimitrova

Information Entropy as a Measure of the Quality of a Nuclear Density Distribution

NUCLEAR STRUCTURE 16O, 32S, 40Ca, 90Zr, 116Sn, 208Pb; calculated information entropy based on various density distribution models.

doi: 10.1142/S0218301398000257
Citations: PlumX Metrics


1997LA16      Z.Phys. A357, 429 (1997)

G.A.Lalazissis, C.P.Panos, M.E.Grypeos, Y.K.Gambhir

Semi-Phenomenological Neutron Density Distributions

NUCLEAR STRUCTURE 58,64Ni, 116Sn, 208Pb; calculated neutron density distribution, rms radii. 24Mg, 27Al, 28Si, 32S, 40Ar, 40,48Ca, 56Fe, 63Cu, 75As, 90Zr, 124Sn, 195Pt, 197Au, 208Pb; calculated rms radii. Semi-phenomenological approach, comparison to other models.

doi: 10.1007/s002180050263
Citations: PlumX Metrics


1997PA29      Int.J.Mod.Phys. E6, 497 (1997)

C.P.Panos, S.E.Massen

Quantum Entropy for Nuclei

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated total position-, momentum-space entropy related features. Harmonic oscillator shell model, correlated model.

doi: 10.1142/S0218301397000275
Citations: PlumX Metrics


1996LA31      Int.J.Mod.Phys. E5, 669 (1996)

G.A.Lalazissis, C.P.Panos

Isospin Dependent Oscillator Spacing for Neutrons and Protons in Nuclei using HF-BCS Radii

NUCLEAR STRUCTURE 14,15,16,17,18,19,20O, 21,22,23,24,25,26,27,28Mg, 25,26,27,28,29,30,31Si, 38,40,42,44,46,48Ca, 56,58,60,62,64,66,68Ni, 108,110,112,114,116,118,120,122,124,126,128,130,132Sn, 82,84,86,88,90,92,94,96,98Zr, 57,59,61,63,65,67Ni, 109,111,113,115,117,119,121,123,125,127,129,131Sn, 83,85,87,89,91,93,95,97Zr, 194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214Pb; calculated nucleon oscillator spacings; deduced isospin dependence related features. Hartree-Fock-BCS calculations.

doi: 10.1142/S0218301396000372
Citations: PlumX Metrics


1995LA03      Phys.Rev. C51, 1247 (1995)

G.A.Lalazissis, C.P.Panos

Isospin Dependence of the Oscillator Spacing

NUCLEAR STRUCTURE 16,17,18,19,20,21,22,23,24,25,26O, 34,36,38,40,42,44,46,48,50,52Ca; calculated oscillator spacing for these and Sn, Pb isotopes. 18O, 44Ca, 68Ni, 106Zr, 132Sn, 208Pb; calculated (h-bar x omega). Data on mean square radii analyzed.

doi: 10.1103/PhysRevC.51.1247
Citations: PlumX Metrics


1994LA18      Z.Phys. A348, 257 (1994)

G.A.Lalazissis, S.E.Massen, C.P.Panos

The Influence of State Dependent Short Range Correlations on the Depletion of the Nuclear Fermi Sea

NUCLEAR STRUCTURE 16O, 40Ca; calculated charge form factor, occupation numbers, probabilities; deduced state dependent short range correlations role in Fermi sea depletion.

doi: 10.1007/BF01305882
Citations: PlumX Metrics


1993LA03      J.Phys.(London) G19, 283 (1993)

G.A.Lalazissis, C.P.Panos

Oscillator Spacing and Its A Dependence

NUCLEAR STRUCTURE A=10-130; calculated nucleon oscillator spacing; deduced mass dependence. Semi-phenomenological density distribution derived from last nucleon separation energy.

doi: 10.1088/0954-3899/19/2/010
Citations: PlumX Metrics


1993LA15      Phys.Rev. C48, 944 (1993)

G.A.Lalazissis, S.E.Massen, C.P.Panos

Short-Range Correlations and Fractional Occupation Probabilities

NUCLEAR STRUCTURE 12C, 16O, 28Si, 32S, 40Ca; calculated occupation probabilities. Natural orbital representation.

doi: 10.1103/PhysRevC.48.944
Citations: PlumX Metrics


1992LA11      Phys.Rev. C46, 201 (1992)

G.A.Lalazissis, S.E.Massen, C.P.Panos

Systematic Study of the Effect of Short Range Correlations on the Occupation Numbers of the Shell Model Orbits in Light Nuclei

NUCLEAR STRUCTURE 4He, 12C, 16O, 24Mg, 28Si, 31P, 32S, 39K, 40Ca; calculated single particle orbitals occupational probabilities; deduced short range correlations role in Fermi sea depletion.

doi: 10.1103/PhysRevC.46.201
Citations: PlumX Metrics


1992LA23      Z.Phys. A344, 17 (1992)

G.A.Lalazissis, C.P.Panos

The Harmonic Oscillator Energy Level Spacing for Neutrons and Protons in Nuclei

NUCLEAR STRUCTURE Z=10-90; N ≤ 130; calculated harmonic oscillator energy level spacing; deduced behavior at closed shells.

doi: 10.1007/BF01291013
Citations: PlumX Metrics


1991GR08      J.Phys.(London) G17, 1093 (1991)

M.E.Grypeos, G.A.Lalazissis, S.E.Massen, C.P.Panos

The ' Cosh ' or Symmetrized Woods-Saxon Nuclear Potential

NUCLEAR STRUCTURE A=12-58; calculated symmetrized Woods-Saxon potential parameters. Alternative formulation to ' cosh ' potential.

doi: 10.1088/0954-3899/17/7/008
Citations: PlumX Metrics


1990GR13      J.Phys.(London) G16, 1627 (1990)

M.E.Grypeos, G.A.Lalazissis, S.E.Massen, C.P.Panos

Relative Probability of Recoilless (Lambda)-Production in Nuclei in the Plane-Wave Impulse Approximation

NUCLEAR STRUCTURE A=12-208; calculated Lambda production probability in (K-, π-).

doi: 10.1088/0954-3899/16/11/013
Citations: PlumX Metrics


1989GR19      Nuovo Cim. 102A, 445 (1989)

M.E.Grypeos, G.A.Lalazissis, S.E.Massen, C.P.Panos

A New Approach for the Determination of the Variation with the Mass Number of the (Lambda)-Oscillator Spacing

NUCLEAR STRUCTURE A=11-208; calculated lambda-hyperon oscillator spacing. Square well, Woods-Saxon potentials.

doi: 10.1007/BF02734863
Citations: PlumX Metrics


1989MA06      J.Phys.(London) G15, 311 (1989)

S.E.Massen, C.P.Panos

An Approximate Treatment of the Correlated Charge Form Factor of Light Nuclei

NUCLEAR STRUCTURE 4He, 12C, 16O; calculated charge form factor.

doi: 10.1088/0954-3899/15/3/009
Citations: PlumX Metrics


1988MA29      J.Phys.(London) G14, 753 (1988)

S.E.Massen, H.P.Nassena, C.P.Panos

A Formula for the Charge Form Factor of Closed-Shell Nuclei and Its Application to 16O

NUCLEAR STRUCTURE 16O; calculated charge form factor. Non-unitary model operator approach.

doi: 10.1088/0305-4616/14/6/015
Citations: PlumX Metrics


1987GR17      Int.J.Theor.Phys. 26, 583 (1987)

M.E.Grypeos, C.P.Panos

Dependence of (h-bar x Omega) on the Mass Number of Nuclei under the Assumption of a Trapezoidal Average Nuclear Density

NUCLEAR STRUCTURE A=4-60; calculated rms nuclear radii; deduced (h-barxomega) mass dependence. Trapezoidal nuclear density distribution.

doi: 10.1007/BF00670096
Citations: PlumX Metrics


1987PA13      J.Phys.(London) G13, 621 (1987)

C.P.Panos

The Isobar Degrees of Freedom in the Non-Unitary Model Operator Approach

NUCLEAR STRUCTURE 4He; calculated binding energy. Non-unitary model operator approach, isobar degrees of freedom.

doi: 10.1088/0305-4616/13/5/011
Citations: PlumX Metrics


1986PA08      J.Phys.(London) G12, 495 (1986)

C.P.Panos

The Non-Unitary Model Operator Approach with Realistic Potentials and Its Application to 4He

NUCLEAR STRUCTURE 4He; calculated binding energy. Nonunitary model operator method.

doi: 10.1088/0305-4616/12/6/008
Citations: PlumX Metrics


1986PA15      J.Phys.(London) G12, 1197 (1986)

C.P.Panos

Application of a Separation Condition to the Non-Unitary Model Operator Approach with Realistic Potentials

NUCLEAR STRUCTURE 4He; calculated binding energy. Nonunitary model operator.

doi: 10.1088/0305-4616/12/11/009
Citations: PlumX Metrics


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