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NSR database version of May 30, 2024.

Search: Author = G.S.Anagnostatos

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2008AN10      Int.J.Mod.Phys. E17, 1557 (2008)


On the possible stability of tetraneutrons and hexaneutrons

NUCLEAR STRUCTURE 3,5H, 4,5,6,7,8He, 5,6Li, 6,11Be; calculated binding energies.

doi: 10.1142/S0218301308010568
Citations: PlumX Metrics

2003LU17      Bull.Rus.Acad.Sci.Phys. 67, 790 (2003)

V.K.Luk'yanov, E.V.Zemlyanaya, D.N.Kadrev, A.N.Antonov, K.Spasova, G.S.Anagnostatos, J.Giapitzakis

Role of Coulomb distortion in calculation of 12C nucleus form factor with allowance for α-clusterization and nucleon-nucleon correlations

NUCLEAR STRUCTURE 12C; calculated form factors, matter density distributions.

2002AN12      Yad.Fiz. 65, 615 (2002); Phys.Atomic Nuclei 65, 583 (2002)

G.S.Anagnostatos, C.Politis, C.Syros, P.K.Kakanis, J.Giapitzakis

Alpha Clustering in 4n Nuclei from 4He to 40Ca

NUCLEAR STRUCTURE 12C, 16O, 20Ne, 36Ar, 40Ca; calculated α-cluster states features. Isomorphic shell model.

doi: 10.1134/1.1471255
Citations: PlumX Metrics

2002AN28      Bull.Rus.Acad.Sci.Phys. 65, 1668 (2002)

G.S.Anagnostatos, J.S.Vaagen, K.A.Gridnev, M.P.Kartamyshev, V.K.Lukyanov

Role of Linear α-Cluster Configuration in Formation of Charge Form Factors of 12C Nucleus

NUCLEAR STRUCTURE 12C; calculated electron scattering form factors; deduced role of linear α-cluster configuration.

2002AV02      Int.J.Mod.Phys. E11, 249 (2002)

M.Avrigeanu, G.S.Anagnostatos, A.N.Antonov, V.Avrigeanu

Elastic Scattering as a Test of Density Distributions in 6He and 8He

NUCLEAR REACTIONS 1H(6He, 6He), (8He, 8He), E = 25-72 MeV/nucleon; calculated σ(θ), optical potential features. 6,8He deduced matter density distribution features. Comparison with data.

doi: 10.1142/S021830130200082X
Citations: PlumX Metrics

2002DA10      Eur.Phys.J. A 14, 125 (2002)

J.Dabrowski, J.Rozynek, G.S.Anagnostatos

Σ- Atoms and the ΣN Interaction

ATOMIC PHYSICS 12C, 16O, 24Mg, 27Al, 28Si, 32S, 40Ca, 48Ti, 138Ba, 184W, 208Pb; calculated Σ- atoms level energy shifts. Comparison with data.

doi: 10.1007/s10050-002-8797-y
Citations: PlumX Metrics

2002GR26      Int.J.Mod.Phys. E11, 359 (2002)

K.A.Gridnev, M.P.Kartamyshev, J.S.Vaagen, V.K.Lukyanov, G.S.Anagnostatos

The Role of Linear Alpha-Cluster Configuration for 12C

NUCLEAR STRUCTURE 12C; calculated electron scattering form factors; deduced role of linear α-cluster configuration.

doi: 10.1142/S0218301302000934
Citations: PlumX Metrics

2002LU14      Part. and Nucl., Lett. 111, 5 (2002)

V.K.Lukyanov, E.V.Zemlyanaya, D.N.Kadrev, A.N.Antonov, K.Spasova, G.S.Anagnostatos, J.Giapitzakis

Role of the Coulomb Distortion in Form-Factor Calculations for 12C with Alpha-Clusterization and Nucleon-Nucleon Correlations

NUCLEAR STRUCTURE 12C; calculated density distributions, elastic form factors; deduced effect of α-clustering.

2001AN24      Yad.Fiz. 64, No 7, 1304 (2001); Phys.Atomic Nuclei 64, 1229 (2001)

G.S.Anagnostatos, C.Politis, A.Vahlas, J.Giapitzakis, A.N.Antonov, M.Avrigeanu

Light Exotic Nuclei: A new explanation of halo

NUCLEAR STRUCTURE 6,8He; calculated neutron and proton density distributions. 7,8,9,10Be; calculated binding energies, radii, internal vibrational and rotational energies.

doi: 10.1134/1.1389547
Citations: PlumX Metrics

2001DA13      Acta Phys.Pol. B32, 2179 (2001)

J.Dabrowski, J.Rozynek, G.S.Anagnostatos

Nuclear and Atomic States of Σ Hyperons and the ΣN Interaction

NUCLEAR STRUCTURE 12C, 16O, 24Mg, 27Al, 28Si, 32S, 40Ca, 48Ti, 138Ba, 184W, 208Pb; calculated Σ hypernucleus energy shifts, widths. Several models compared with data.

2000AV02      Phys.Rev. C62, 017001 (2000)

M.Avrigeanu, G.S.Anagnostatos, A.N.Antonov, J.Giapitzakis

Dynamics of Two-Neutron Transfer Reactions on the Borromean Nucleus 6He Reexamined

NUCLEAR REACTIONS 1H, 4He(6He, 6He), E=151 MeV; calculated σ(θ). 4,6He deduced density distribution features. Comparisons with data.

doi: 10.1103/PhysRevC.62.017001
Citations: PlumX Metrics

2000LU18      Bull.Rus.Acad.Sci.Phys. 64, 681 (2000)

V.L.Lukyanov, E.V.Zemlyanaya, D.N.Kadrev, A.N.Antonov, K.Spasova, G.S.Anagnostatos, P.Ginis, J.Giapitzakis

Structure of α-Clusters and Charge Formfactors of the 12C Nucleus

NUCLEAR STRUCTURE 12C; calculated levels form-factors, wave functions, radial transition densities. α-cluster model calculations, comparison with data.

1999AN08      J.Phys.(London) G25, 69 (1999)

G.S.Anagnostatos, A.N.Antonov, P.Ginis, J.Giapitzakis, M.K.Gaidarov

On the Central Depression in Density of 4He

NUCLEAR STRUCTURE 4He; calculated charge, point-proton density distributions. Natural orbital representation.

doi: 10.1088/0954-3899/25/1/007
Citations: PlumX Metrics

1998AN24      Phys.Rev. C58, 2115 (1998)

G.S.Anagnostatos, A.N.Antonov, P.Ginis, J.Giapitzakis, M.K.Gaidarov, A.Vassiliou

Nucleon Momentum and Density Distributions in 4He Considering Internal Rotation

NUCLEAR STRUCTURE 4He; calculated charge density, nucleon momentum distributions, rms charge radius; deduced role of internal rotation. Natural orbital representation.

doi: 10.1103/PhysRevC.58.2115
Citations: PlumX Metrics

1998AN31      Phys.Rev. C58, 3305 (1998)

G.S.Anagnostatos, P.Ginis, J.Giapitzakis

α-Planar States in 28Si

NUCLEAR STRUCTURE 28Si; calculated α-planar states deofrmations, related features, cluster-associated resonances. Isomorphic shell model. Comparison with data.

doi: 10.1103/PhysRevC.58.3305
Citations: PlumX Metrics

1998GI21      Int.J.Mod.Phys. E7, 585 (1998)

J.Giapitzakis, P.Ginis, A.N.Antonov, S.E.Massen, G.S.Anagnostatos

Multiharmonic Nuclear Hamiltonian in the Region 120 < A ≤ 140

NUCLEAR STRUCTURE 123Sb, 123,124,125,126,128,130Te, 127I, 126,128,129,130,131,132,134,136Xe, 133Cs, 130,132,134,135,136,137,138Ba, 138,139La, 136,138,140Ce; calculated radii, ground state binding energies. Isomorphic shell model. Comparison with data.

doi: 10.1142/S0218301398000324
Citations: PlumX Metrics

1996AN19      Int.J.Mod.Phys. E5, 557 (1996)


Nuclear Charge Radii from H to Pb

NUCLEAR STRUCTURE A=1-208; calculated charge radii. Independent particle shell-model extended to incorporate ground state properties.

doi: 10.1142/S0218301396000293
Citations: PlumX Metrics

1996KA41      Phys.Rev. C54, 2996 (1996)

P.K.Kakanis, G.S.Anagnostatos

Persisting α-Planar Structure in 20Ne

NUCLEAR STRUCTURE 20Ne; calculated binding energy, rms charge radius, electric quadrupole, octupole, hexadecapole moments, B(λ), T1/2, average moment of inertia factor, levels, Γ. Isomorphic shell model, hybrid between conventional shell, liquid drop models.

doi: 10.1103/PhysRevC.54.2996
Citations: PlumX Metrics

1995AN01      Phys.Rev. C51, 152 (1995)


Alpha-Chain States in 12C

NUCLEAR STRUCTURE 12C; calculated levels, charge rms radius, intrinsic quadrupole moment. Isomorphic shell model, α-chain states.

doi: 10.1103/PhysRevC.51.152
Citations: PlumX Metrics

1995GA33      Phys.Rev. C52, 3026 (1995)

M.K.Gaidarov, A.N.Antonov, G.S.Anagnostatos, S.E.Massen, M.V.Stoitsov, P.E.Hodgson

Proton Momentum Distribution in Nuclei Beyond 4He

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Fe, 208Pb; calculated proton momentum distribution. Natural orbital representation model, empirical 4He nucleon momentum distribution input.

doi: 10.1103/PhysRevC.52.3026
Citations: PlumX Metrics

1992AN08      Can.J.Phys. 70, 361 (1992)


Multiharmonic Nuclear Hamiltonian

NUCLEAR STRUCTURE 16O, 28Si, 36,40Ar, 40Ca, 56Fe, 58,60Ni, 90Zr, 104,110Pd, 120Sn, 126Te, 136,138Ba, 142Nd, 202Hg, 208Pb; calculated binding energies, rms charge radii. Multi-harmonic oscillator potential, shell model.

doi: 10.1139/p92-059
Citations: PlumX Metrics

1991AN05      Can.J.Phys. 69, 114 (1991)

G.S.Anagnostatos, T.S.Kosmas, E.F.Hefter, C.N.Panos

Semiclassical Approximation for the Isotopic Shift of Charge Radii in Ca Isotopes

NUCLEAR STRUCTURE 40,41,42,43,44,45,46,47,48Ca; analyzed isotope shift, rms charge, mass radii. Isomorphic shell model.

doi: 10.1139/p91-017
Citations: PlumX Metrics

1990AN16      Phys.Rev. C42, 961 (1990)

G.S.Anagnostatos, C.N.Panos

Semiclassical Simulation of Finite Nuclei

NUCLEAR STRUCTURE 16O; calculated potential, kinetic, binding energies, mass rms radius time evolution. Semi-classical simulation.

doi: 10.1103/PhysRevC.42.961
Citations: PlumX Metrics

1989AN03      Phys.Rev. C39, 877 (1989)


Classical Equations-of-Motion Model for High-Energy Heavy-Ion Collisions

NUCLEAR REACTIONS 20Ne(20Ne, pX), E=800 MeV/nucleon; calculated inclusive σ(θ, Ep). Equations-of-motion model.

doi: 10.1103/PhysRevC.39.877
Citations: PlumX Metrics

1985AN11      Int.J.Theor.Phys. 24, 579 (1985)


Isomorphic Shell Model for Closed-Shell Nuclei

NUCLEAR STRUCTURE 4He, 16O, 40,48Ca, 58Ni, 90Zr, 120Sn, 142Nd, 208Pb; calculated rms charge, n, p, n-p radii, average nuclear densities, radial parameter. Isomorphic shell model.

doi: 10.1007/BF00670466
Citations: PlumX Metrics

1984AN20      Lett.Nuovo Cim. 41, 409 (1984)

G.S.Anagnostatos, C.N.Panos

Simple Static Central Potentials as Effective Nucleon-Nucleon Interactions

NUCLEAR STRUCTURE 16O, 40Ca; calculated rms charge radii, Coulomb, kinetic, potential, binding energies. Isomorphic model.

doi: 10.1007/BF02739593
Citations: PlumX Metrics

1982PA22      J.Phys.(London) G8, 1651 (1982)

C.N.Panos, G.S.Anagnostatos

Comments on ' A Relation between Average Kinetic Energy and Mean-Square Radius in Nuclei '

NUCLEAR STRUCTURE 16O, 40Ca; calculated average kinetic energy, rms radii. Isomorphic model.

doi: 10.1088/0305-4616/8/12/007
Citations: PlumX Metrics

1980AN13      Phys.Rev. C22, 305 (1980)


Comments on 'Extension of the Variable-Moment-of-Inertia Model to High Spins'

NUCLEAR STRUCTURE 158,160Dy, 162,164Er, 168Yb, 172,174,176Hf; calculated levels, moment of inertia, square of angular velocity. Modified variable moment of inertia model.

doi: 10.1103/PhysRevC.22.305
Citations: PlumX Metrics

1977AN12      Atomkernenergie 29, 207 (1977)


Static Properties of Nuclei in the s-d Shell

NUCLEAR STRUCTURE 16O, 17,19F, 19,20,21,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,35,36S, 35,36,37Cl, 36,38Ar, 40Ca, 39K; calculated rms radii, quadrupole moment, Coulomb energies.

1975AN10      Nucl.Phys. A246, 445 (1975)


Interpretation of the Non-Zero Energy for Iπ = 0+ and the Break in Mallmann's Curves

NUCLEAR STRUCTURE 8Be, 12C, 40Ar, 42,44Ca, 48,50Ti, 52Cr, 54Fe, 60,62Ni, 64,66Zn, 68,70,74Ge, 72,74,76,78,82Se, 82,84Kr, 86Sr, 88,90,92Zr, 90,92,94,96,98,100Mo, 94,96,98,100,102Ru, 106,108,110Pd, 110,114Cd, 108,110,112,116,118Sn, 114,116,118,120,122,124,126,128,130,132,134Te, 126,128,130,132,134,136Xe, 134,136,138Ba, 140Ce, 142,144Nd, 142,144,146,148Sm, 146,150,152Gd, 154Dy, 192Os, 190,192,194,196Pt, 206,208,210Pb, 200,202,204,206,208,210Po; calculated levels, analyzed break in Mallmann'S curve, predicted new levels.

doi: 10.1016/0375-9474(75)90658-2
Citations: PlumX Metrics

1973AN04      Can.J.Phys. 51, 998 (1973)


The Geometry of the Isomorphic Model of the Closed-Shell Nuclei

NUCLEAR STRUCTURE 16O, 40Ca, 58Ni, 90Zr, 112Sn, 142Nd, 208Pb calculated nuclear radii.

doi: 10.1139/p73-130
Citations: PlumX Metrics

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