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NSR database version of May 3, 2024.

Search: Author = G.Holzwarth

Found 25 matches.

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2000HO09      Nucl.Phys. A666-667, 24c (2000)

G.Holzwarth

Skyrme Model and Electromagnetic Form Factors of the Nucleon

doi: 10.1016/S0375-9474(00)00005-1
Citations: PlumX Metrics

2000HO12      Nucl.Phys. A672, 167 (2000)

G.Holzwarth

Skyrmions and Bags in the 2D-O(3) Model

doi: 10.1016/S0375-9474(99)00810-6
Citations: PlumX Metrics

1997HO02      Phys.Rev. C55, 1088 (1997)

G.Holzwarth, R.Machleidt

Skyrme-Model πNN Form Factor and Nucleon-Nucleon Interaction

NUCLEAR REACTIONS 1H(n, n), E ≤ 300 MeV; analyzed phase shifts data. Skyrme model πNN form factor, one-boson exchange NN-interaction.

NUCLEAR STRUCTURE 2H; calculated binding energy, D-state probability, quadrupole moment, asymptotic D/S state ratio.

doi: 10.1103/PhysRevC.55.1088
Citations: PlumX Metrics

1997WA13      Z.Phys. A357, 317 (1997)

H.Walliser, G.Holzwarth

Electro-Excitation Amplitudes of the Δ-isobar in the Skyrme Model

NUCLEAR STRUCTURE 1H; calculated magnetic form factor/μ(P)G(D). Skyrme model, Δ-isobar, NΔ transition also studied.

doi: 10.1007/s002180050248
Citations: PlumX Metrics

1996HO27      Z.Phys. A356, 339 (1996)

G.Holzwarth

Electro-Magnetic Nucleon Form Factors and Their Spectral Functions in Soliton Models

NUCLEAR STRUCTURE 1H, 1n; calculated magnetic, electric form factors, spectral functions. Soliton models.

doi: 10.1007/s002180050187
Citations: PlumX Metrics

1995HO09      Nucl.Phys. A587, 721 (1995)

G.Holzwarth, H.Walliser

Quantum Corrections to the Skyrmion Mass

doi: 10.1016/0375-9474(95)00012-P
Citations: PlumX Metrics

1994HO06      Nucl.Phys. A572, 69 (1994)

G.Holzwarth

The Nucleon Mass in the Skyrme Model

NUCLEAR STRUCTURE 1H, 1n; calculated μ. Skyrme model for nucleon mass.

doi: 10.1016/0375-9474(94)90422-7
Citations: PlumX Metrics

1985DA07      Nucl.Phys. A439, 477 (1985)

J.P.Da Providencia, G.Holzwarth

Low-Lying Nuclear Collective States and Giant Resonances in Nuclear Fluid Dynamics

NUCLEAR STRUCTURE A=184; calculated energy weighted sum fraction for several giant resonances. Nuclear fluid dynamics, general scaling approximation, comparison with RPA.

doi: 10.1016/0375-9474(85)90422-1
Citations: PlumX Metrics

1985KA23      Nucl.Phys. A445, 419 (1985)

U.Kaup, G.Holzwarth

Effect of the Pauli Principle on Collective States in Transitional Xe, Ba and Ce Nuclei

NUCLEAR STRUCTURE 124Xe, 126Ba, 128,130,132,134Ce; calculated levels, B(E2) values.

doi: 10.1016/0375-9474(85)90450-6
Citations: PlumX Metrics

1984HA46      Phys.Lett. 147B, 5 (1984)

A.Hayashi, G.Eckart, G.Holzwarth, H.Walliser

Pion-Nucleon Scattering Phase Shifts in the Skyrme Model

NUCLEAR REACTIONS 1n(π, π), E ≤ 500 MeV; calculated phase shifts. Skyrme model.

doi: 10.1016/0370-2693(84)90581-1
Citations: PlumX Metrics

1983DA05      Nucl.Phys. A398, 59 (1983)

J.P.Da Providencia, G.Holzwarth

Variational Approach to Nuclear Fluid Dynamics

NUCLEAR STRUCTURE A=208; calculated B(λ), radial wave functions. Nuclear fluid dynamics, variational approach.

doi: 10.1016/0375-9474(83)90647-4
Citations: PlumX Metrics

1983HO07      Nucl.Phys. A396, 171c (1983)

G.Holzwarth, G.Eckart

Nuclear Fluid Dynamics for Giant Resonances

NUCLEAR STRUCTURE 208Pb, 40Ca; calculated surface flow patterns; 90Zr calculated form factors. Giant resonances, fluid dynamical model.

doi: 10.1016/0375-9474(83)90017-9
Citations: PlumX Metrics

1983HO20      Prog.Theor.Phys.(Kyoto), Suppl. 74/75, 357 (1983)

G.Holzwarth

Fluiddynamical Models for Giant Resonances

NUCLEAR STRUCTURE A=208; calculated isoscalar dipole, quadrupole excitation density flow patterns. Generalized scaling approach, fluid dynamic models.

doi: 10.1143/PTPS.74.357
Citations: PlumX Metrics

1983WI13      Nucl.Phys. A410, 237 (1983)

J.Winchenbach, K.Pingel, G.Holzwarth, G.Kuhner, A.Richter

Doorway-State Analysis of the Fine Structure in the Giant Quadrupole Resonance in 208Pb Observed in Inelastic Electron Scattering

NUCLEAR REACTIONS 208Pb(e, e'), E=45-65 meV; analyzed σ(E(e')), E2 transition strength fragmentation. 208Pb deduced doorway escape energies, escape, spreading widths. Doorway to complicated state coupling.

doi: 10.1016/0375-9474(83)90200-2
Citations: PlumX Metrics

1982EC02      Phys.Lett. 118B, 9 (1982)

G.Eckart, G.Holzwarth

Sum Rules and Strength Functions in Nuclear Fluid Dynamics

NUCLEAR STRUCTURE 40Ca, 80Zr; calculated monopole excitation strength function. Sum rules, nuclear fluid dynamics.

doi: 10.1016/0370-2693(82)90590-1
Citations: PlumX Metrics

1982KO04      Nucl.Phys. A373, 173 (1982)

H.Koch, G.Eckart, B.Schwesinger, G.Holzwarth

Flow Patterns of Giant Resonances in the First- and Zero-Sound Approximation

NUCLEAR STRUCTURE A=40, 208; calculated T=0, T=1 dipole, quadrupole mode flow patterns. Zero-, first-sound approximations, comparison with RPA.

doi: 10.1016/0375-9474(82)90146-4
Citations: PlumX Metrics

1980EC05      Phys.Lett. B94, 453 (1980)

G.Eckart, G.Holzwarth, B.Schwesinger

Electric Multipole Modes in the Fluid-Dynamical Approximation

NUCLEAR STRUCTURE A=90, 208; calculated binding, kinetic energies per nucleon, surface energy, diffuseness. Electric multipole modes, fluid dynamical approach.

doi: 10.1016/0370-2693(80)90917-X
Citations: PlumX Metrics

1980SC14      Nucl.Phys. A341, 1 (1980)

B.Schwesinger, K.Pingel, G.Holzwarth

Excitation of the 2- Twist Mode by Inelastic Electron Scattering

NUCLEAR REACTIONS 90Zr, 208Pb(e, e'), E not given; calculated form factors. 90Zr, 208Pb deduced condition for twist-mode excitation of 2- giant resonance. Collective modes, Fermi fluid, PWBA, DWBA.

NUCLEAR STRUCTURE 90Zr, 208Pb; calculated B(M2), splitting of 2-, T=0, 1 giant resonance.

doi: 10.1016/0375-9474(80)90357-7
Citations: PlumX Metrics

1977EC01      Z.Phys. A281, 385 (1977)

G.Eckart, G.Holzwarth

Selfconsistent Thomas Fermi Method for Spherical Nuclei

NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116Sn, 208Pb; calculated p, n densities.

doi: 10.1007/BF01408187
Citations: PlumX Metrics

1977HO26      Z.Phys. A283, 219 (1977)

G.Holzwarth, G.Eckart

The Nuclear 'Twist'

NUCLEAR STRUCTURE 208Pb; calculated T=0, J=2- level parameters.

doi: 10.1007/BF01418715
Citations: PlumX Metrics

1976HO07      Nucl.Phys. A261, 1 (1976)

G.Holzwarth, D.Janssen, R.V.Jolos

On the Validity of the Boson Method for Transitional Nuclei

NUCLEAR STRUCTURE 72,74,76,78,80Se, 98,100,102,104Ru; calculated matrix elements.

doi: 10.1016/0375-9474(76)90037-3
Citations: PlumX Metrics

1975LI18      Phys.Rev. C12, 1035 (1975)

S.G.Lie, G.Holzwarth

Application of the Boson-Expansion Method to Even Se and Ru Isotopes

NUCLEAR STRUCTURE 76,78Se, 100,102Ru; calculated B(E2) ratios, quadrupole moment, levels. Boson expansion.

doi: 10.1103/PhysRevC.12.1035
Citations: PlumX Metrics

1972HO07      Z.Phys. 249, 332 (1972)

G.Holzwarth, S.G.Lie

The Collective Structure of the Intermediate Nuclei 78Se and 102Ru

NUCLEAR STRUCTURE 78Se, 102Ru; calculated levels, B(E2), quadrupole moment, E2 matrix elements. Bose expansion transcription into collective Hamiltonian.

doi: 10.1007/BF01379727
Citations: PlumX Metrics

1972HO10      Nucl.Phys. A185, 268 (1972)

G.Holzwarth

The Connection between the Generator Coordinate Method and Bose Expansions

doi: 10.1016/0375-9474(72)90568-4
Citations: PlumX Metrics

1972MA41      Nucl.Phys. A191, 438 (1972)

E.R.Marshalek, G.Holzwarth

Boson Expansions and Hartree-Bogoliubov Theory

doi: 10.1016/0375-9474(72)90526-X
Citations: PlumX Metrics

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