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NSR database version of April 11, 2024.

Search: Author = H.Feldmeier

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2020FL01      Phys.Rev. C 101, 015502 (2020)

V.V.Flambaum, H.Feldmeier

Enhanced nuclear Schiff moment in stable and metastable nuclei

NUCLEAR STRUCTURE 153Eu, 227Ac, 235U, 237Np; analyzed octupole deformations in stable and nuclei with long half-lives; deduced estimates of the enhanced Schiff moments, atomic electric dipole moments (EDMs), and T, P-odd interaction constants in molecules containing these nuclei. Discussed possible experiments to test CP-violation theories predicting T, P-violating nuclear forces, and search for axions. 152Sm, 153Eu, 226Ra, 227Ac, 234,235,236U, 237Np; plotted experimental energy levels of positive and negative parities as function of J(J+1) rotational bands.

doi: 10.1103/PhysRevC.101.015502
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2015NE13      Phys.Rev. C 92, 024003 (2015)

T.Neff, H.Feldmeier, W.Horiuchi

Short-range correlations in nuclei with similarity renormalization group transformations

NUCLEAR STRUCTURE 4He; calculated relative density and momentum distributions, ground state wave functions, tensor and many body correlations using the no core shell model (NCSM) with the similarity renormalization group (SRG) transformed AV8' and N3LO interactions in two-body approximation. Short-range correlations.

doi: 10.1103/PhysRevC.92.024003
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2014FE09      Phys.Rev. C 90, 064005 (2014)

H.Feldmeier, T.Neff, D.Weber

Nucleon-nucleon potentials in phase-space representation

doi: 10.1103/PhysRevC.90.064005
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2014WE01      Phys.Rev. C 89, 034002 (2014)

D.Weber, H.Feldmeier, H.Hergert, T.Neff

From nucleon-nucleon interaction matrix elements in momentum space to an operator representation

doi: 10.1103/PhysRevC.89.034002
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2012NE08      J.Phys.:Conf.Ser. 337, 012055 (2012)

T.Neff, H.Feldmeier, K.Langanke

Microscopic calculation of the 3He(α, γ)7Be reaction rate using realistic interactions

NUCLEAR REACTIONS 3H, 3He(α, γ), E(cm)≈0.2-2.5 MeV; calculated S-factor, γ dipole strength using FMD (fermionic molecular dynamics). Compared with data.

doi: 10.1088/1742-6596/337/1/012055
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2011FE08      Phys.Rev. C 84, 054003 (2011)

H.Feldmeier, W.Horiuchi, T.Neff, Y.Suzuki

Universality of short-range nucleon-nucleon correlations

NUCLEAR STRUCTURE 2,3H, 3,4He; calculated Argonne v8' potential contours, one-body point densities, two-body density contours in coordinate and momentum space, three-body correlations in the unitary correlation operator method (UCOM) approach. Correlated Gaussian basis approach for the Argonne v8' interaction.

doi: 10.1103/PhysRevC.84.054003
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2011KA29      Phys.Rev. C 84, 054301 (2011)

Y.Kanada-Enyo, H.Feldmeier, T.Suhara

Two-neutron correlations in microscopic wave functions of 6He, 8He, and 12C

NUCLEAR STRUCTURE 6,8He, 12C; calculated one-body neutron density, two-neutron density contours, two-neutron correlations. Many body microscopic wave functions from antisymmetrized molecular dynamics (AMD).

doi: 10.1103/PhysRevC.84.054301
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2011NE02      Prog.Part.Nucl.Phys. 66, 341 (2011)

T.Neff, H.Feldmeier, K.Langanke

Towards microscopic ab initio calculations of astrophysical S-factors

NUCLEAR REACTIONS 3H, 3He(α, γ), E<2.5 MeV; calculated S-factors, p-wave scattering phase shifts, dipole strengths. Fermionic Molecular Dynamics, Argonne V18 potential.

doi: 10.1016/j.ppnp.2011.01.031
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2011VO16      J.Phys.:Conf.Ser. 312, 042026 (2011)

P.von Neumann-Cosel, M.Chernykh, H.Feldmeier, T.Neff, A.Richter

Pair decay width of the Hoyle state and carbon production in stars

NUCLEAR REACTIONS 12C(e, e'), E=73 MeV; measured Ee, Ie; deduced transition charge density for transition in from ground to the Hoyle state, formfactor at low q, pair decay widths.

doi: 10.1088/1742-6596/312/4/042026
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2010CH17      Phys.Rev.Lett. 105, 022501 (2010)

M.Chernykh, H.Feldmeier, T.Neff, P.von Neumann-Cosel, A.Richter

Pair Decay Width of the Hoyle State and its Role for Stellar Carbon Production

NUCLEAR REACTIONS 12C(e, e'), E=29-78 MeV; measured reaction products; deduced transition form factors, charge density, pair decay width of the Hoyle state.

doi: 10.1103/PhysRevLett.105.022501
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2009LI21      Phys.Rev. C 79, 064303 (2009)

E.Litvinova, H.Feldmeier, J.Dobaczewski, V.Flambaum

Nuclear structure of lowest 229Th states and time-dependent fundamental constants

NUCLEAR STRUCTURE 229Th; calculated Coulomb, neutron and proton kinetic energies, proton and neutron rms radii, and neutron and proton intrinsic quadrupole moments of almost degenerate ground state and the first excited state using Hartree-Fock and Hartree-Fock-Bogoliubov calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.064303
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2008BA39      Phys.Rev. C 78, 044306 (2008)

S.Bacca, H.Feldmeier, T.Neff

Long range tensor correlations in charge and parity projected fermionic molecular dynamics

NUCLEAR STRUCTURE 4He; calculated energies of 0+ states. Fermionic molecular dynamics. Long-range tensor correlations.

doi: 10.1103/PhysRevC.78.044306
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2008GE07      Phys.Rev.Lett. 101, 252502 (2008)

W.Geithner, T.Neff, G.Audi, K.Blaum, P.Delahaye, H.Feldmeier, S.George, C.Guenaut, F.Herfurth, A.Herlert, S.Kappertz, M.Keim, A.Kellerbauer, H.-J.Kluge, M.Kowalska, P.Lievens, D.Lunney, K.Marinova, R.Neugart, L.Schweikhard, S.Wilbert, C.Yazidjian

Masses and Charge Radii of 17-22Ne and the Two-Proton-Halo Candidate 17Ne

ATOMIC MASSES 17,18,19,20,21,22Ne; measured masses and charge radii using penning trap mass spectrometry.

doi: 10.1103/PhysRevLett.101.252502
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2008NE06      Eur.Phys.J. Special Topics 156, 69 (2008)

T.Neff, H.Feldmeier

Clustering and other exotic phenomena in nuclei

doi: 10.1140\epjst/e2008-00609-y
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2008NE13      Int.J.Mod.Phys. E17, 2005 (2008)

T.Neff, H.Feldmeier

Cluster and shell structures in the Fermionic Molecular Dynamics approach

NUCLEAR STRUCTURE 12C, 17,18,19,20,21,22Ne; calculated level energies, radii, matrix elements, B(E2). Fermionic Molecular Dynamics (FMD) model.

doi: 10.1142/S0218301308010994
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2007CH04      Phys.Rev.Lett. 98, 032501 (2007)

M.Chernykh, H.Feldmeier, T.Neff, P.von Neumann-Cosel, A.Richter

Structure of the Hoyle State in 12C

NUCLEAR REACTIONS 12C(e, e), (e, e'), E not given; analyzed σ(θ). 12C deduced excited state density, related features.

NUCLEAR STRUCTURE 12C; calculated energies, radii, transition strengths. Fermionic molecular dynamics model, α-cluster models.

doi: 10.1103/PhysRevLett.98.032501
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2007LA15      Prog.Part.Nucl.Phys. 59, 66 (2007)

K.Langanke, H.Feldmeier, G.Martinez-Pinedo, T.Neff

Astrophysically important nuclear reactions

doi: 10.1016/j.ppnp.2006.12.010
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2006BA27      Phys.Rev. C 73, 054608 (2006)

S.Bacca, H.Feldmeier

Resonant tunneling in a schematic model

doi: 10.1103/PhysRevC.73.054608
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2006RO15      Phys.Rev. C 73, 044312 (2006)

R.Roth, P.Papakonstantinou, N.Paar, H.Hergert, T.Neff, H.Feldmeier

Hartree-Fock and many body perturbation theory with correlated realistic NN interactions

NUCLEAR STRUCTURE 4He, 16,24O, 34Si, 40,48Ca, 48,56,78Ni, 88Sr, 90Zr, 100,114,132Sn, 146Gd, 208Pb; calculated ground-state energies, radii. 16O, 40Ca, 100,132Sn, 208Pb; calculated single-particle energies. O, Ca, Ni, Sn; calculated ground-state energies for even-A isotopes. Correlated realistic nucleon-nucleon interactions.

doi: 10.1103/PhysRevC.73.044312
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2005NE03      Nucl.Phys. A752, 321c (2005)

T.Neff, H.Feldmeier, R.Roth

Structure of light nuclei in Fermionic Molecular Dynamics

NUCLEAR STRUCTURE 4,5,6,7,8He, 7,8,9,10,11,12,13,14Be; calculated binding energies, radii, deformation. Fermionic molecular dynamics model.

doi: 10.1016/j.nuclphysa.2005.02.092
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2005RO32      Phys.Rev. C 72, 034002 (2005)

R.Roth, H.Hergert, P.Papakonstantinou, T.Neff, H.Feldmeier

Matrix elements and few-body calculations within the unitary correlation operator method

NUCLEAR STRUCTURE 3H, 4He; calculated ground-state energies vs oscillator parameter. Unitary correlation operator method.

doi: 10.1103/PhysRevC.72.034002
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2004NE08      Nucl.Phys. A738, 357 (2004)

T.Neff, H.Feldmeier

Cluster structures within Fermionic Molecular Dynamics

NUCLEAR STRUCTURE 12C; calculated cluster states energies, J, π, radii, B(E2). 4,5,6,7,8He; calculated binding energies, radii. Fermionic molecular dynamics approach.

doi: 10.1016/j.nuclphysa.2004.04.061
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2004RO37      Nucl.Phys. A745, 3 (2004)

R.Roth, T.Neff, H.Hergert, H.Feldmeier

Nuclear structure based on correlated realistic nucleon-nucleon potentials

NUCLEAR STRUCTURE 3,4He, 7Li, 9Be, 10B, 12C, 14N, 16O, 20Ne, 23Na, 24Mg, 27Al, 28Si, 32S, 36Ar, 36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,54Ca, 50Ti, 56Fe, 60Ni; calculated binding energies, radii. 7Li, 9Be, 12C, 16O, 20,22,24,26Ne, 26Mg, 40,48Ca; calculated particle density distributions. 7Li, 9Be, 12C, 20Ne; calculated levels, J, π. Unitary correlation operator method, fermionic molecular dynamics model.

doi: 10.1016/j.nuclphysa.2004.08.024
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2003NE03      Nucl.Phys. A713, 311 (2003)

T.Neff, H.Feldmeier

Tensor correlations in the unitary correlation operator method

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding energies, radii, correlated single-particle momentum distributions. Unitary correlation operator method.

doi: 10.1016/S0375-9474(02)01307-6
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2002BO02      Phys.Rev. C65, 017601 (2002)

J.P.Bondorf, H.Feldmeier, I.N.Mishustin, G.Neergaard

Equilibration and Freeze-Out in an Exploding System

doi: 10.1103/PhysRevC.65.017601
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2001FE04      Nucl.Phys. A681, 398c (2001)

H.Feldmeier

Liquid-Gas Phase Transition in Fermionic Molecular Dynamics

doi: 10.1016/S0375-9474(00)00545-5
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2001PO01      Nucl.Phys. A679, 793 (2001)

A.Pop, A.Andronic, I.Berceanu, M.Duma, D.Moisa, M.Petrovici, V.Simion, A.Bonasera, G.Imme, G.Lanzano, A.Pagano, G.Raciti, N.Colonna, G.d'Erasmo, A.Pantaleo, H.Feldmeier, J.Schnack

Global Features of Dissipative Processes in Light Heavy-Ion Collisions

NUCLEAR REACTIONS 27Al(19F, X), E=111.4, 125, 136.9 MeV; 12C(19F, X), E=111.4, 136.9 MeV; measured Z=5-16 fragments mass, charge, energy, and angular distributios. Comparisons with heavier systems and model predictions.

doi: 10.1016/S0375-9474(00)00348-1
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1999NE02      Nucl.Phys. A647, 107 (1999)

J.Nemeth, G.Papp, H.Feldmeier

Au + Au Central Collisions at 150, 250 and 400 A MeV Energies in QMD with Relativistic Forces

NUCLEAR REACTIONS 197Au(197Au, X), E=150, 250, 400 MeV/nucleon; calculated light, intermediate fragments charge, multiplicity distributions, angular distributions, transverse spectra. Relativistic scalar-vector force, quantum molecular dynamics. Comparison with data.

doi: 10.1016/S0375-9474(99)00009-3
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1998FE03      Nucl.Phys. A632, 61 (1998)

H.Feldmeier, T.Neff, R.Roth, J.Schnack

A Unitary Correlation Operator Method

doi: 10.1016/S0375-9474(97)00805-1
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1997BE31      Phys.Rev. C56, 839 (1997)

G.F.Bertsch, H.Feldmeier

Variational Approach to Anharmonic Collective Motion

doi: 10.1103/PhysRevC.56.839
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1997SC34      Phys.Lett. 409B, 6 (1997)

J.Schnack, H.Feldmeier

The Nuclear Liquid-Gas Phase Transition within Fermionic Molecular Dynamics

NUCLEAR STRUCTURE 16O, 24Mg, 27Al, 40Ca; analyzed excited system time evolution, temperature vs excitation energy; deduced phase transition features. 24Mg; calculated radial density vs excitation energy. Fermionic molecular dynamics model.

NUCLEAR REACTIONS 197Au(197Au, X), E=600 MeV/nucleon; 197Au, Ag(12C, X), (18O, X), E=30-84 MeV/nucleon; 181Ta(22Ne, X), E=8 MeV/nucleon; analyzed caloric curves data; deduced phase transition features.

doi: 10.1016/S0370-2693(97)00865-4
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1996FE18      Acta Phys.Hung.N.S. 3, 71 (1996)

H.Feldmeier, J.Nemeth, G.Papp

Multifragmentation Calculated with Relativistic Forces

NUCLEAR REACTIONS Ca(Ca, X), E=200, 400, 800 MeV/nucleon; calculated relative momenta distributions vs time. Br(O, X), E=50-200 MeV/nucleon; calculated fragments charge distribution vs time. Coordinate and momentum dependent relativistic forces.


1996SC16      Nucl.Phys. A601, 181 (1996)

J.Schnack, H.Feldmeier

Statistical Properties of Fermionic Molecular Dynamics

doi: 10.1016/0375-9474(95)00505-6
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1995FE01      Nucl.Phys. A583, 347c (1995)

H.Feldmeier, J.Schnack

Fermionic Molecular Dynamics: Ensembles and fluctuations therein

NUCLEAR REACTIONS 12C(12C, X), E=28.7 MeV/nucleon; calculated coordinate space densities integrated over z-direction; deduced different phenomena evidence related features. Fermionic molecular dynamics models.

doi: 10.1016/0375-9474(94)00684-F
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1995FE05      Nucl.Phys. A586, 493 (1995)

H.Feldmeier, K.Bieler, J.Schnack

Fermionic Molecular Dynamics for Ground States and Collisions of Nuclei

NUCLEAR STRUCTURE 4He, 6,7Li, 8Be, 12C, 16O; calculated ground state energies, charge radii, spatial density momentum distributions contour plots. Fermionic molecular dynamics equations.

doi: 10.1016/0375-9474(94)00792-L
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1994RH01      Phys.Rev. C49, 250 (1994)

M.Rhein, R.Barth, E.Ditzel, H.Feldmeier, E.Kankeleit, V.Lips, C.Muntz, W.Norenberg, H.Oeschler, A.Piechaczek, W.Polai, I.Schall

Elastoplasticity in Dissipative Heavy-Ion Collisions

NUCLEAR REACTIONS Pb(Pb, X), E=12 MeV/nucleon; measured δ-electron spectra in coincidence with elastic, dissipative collisions; deduced time evolution of nuclear reactions, deceleration and contact times. Elastoplastic properties of nuclear matter.

doi: 10.1103/PhysRevC.49.250
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1990GI08      Phys.Lett. 252B, 198 (1990)

P.Gippner, U.Brosa, H.Feldmeier, R.Schmidt

' Fast Fusion ' and ' Quasifission ': Two Possible mass-relaxation modes in asymmetric heavy-ion collisions leading to systems with Z(tot) = 108

NUCLEAR REACTIONS, ICPND 238U(32S, X), E=192 MeV; 232Th(40Ar, X), E=220 MeV; calculated fusion σ relative to capture. Simple diffusion model.

doi: 10.1016/0370-2693(90)90861-Y
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1985FE01      Nucl.Phys. A435, 229 (1985)

H.Feldmeier, H.Spangenberger

Dissipation and Fluctuation of the Relative Momentum in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 166Er(86Kr, X), E=703.5 MeV; 209Bi(136Xe, X), E=1.422 GeV; calculated di-nuclear potential vs separation, σ(fragment θ, E). Langevin equation, fluctuating force.

doi: 10.1016/0375-9474(85)90313-6
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1985GR14      Nucl.Phys. A444, 113 (1985)

M.K.Grossjean, H.Feldmeier

Level Density of a Fermi Gas with Pairing Interactions

NUCLEAR STRUCTURE 60Ni; calculated level density. Fermi gas model, pairing interactions.

doi: 10.1016/0375-9474(85)90294-5
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1985SP02      Nucl.Phys. A435, 267 (1985)

H.Spangenberger, F.Beck, H.Feldmeier

Quantum Interference and Statistical Fluctuations in Deep-Inelastic Heavy-Ion Reactions

NUCLEAR REACTIONS 166Er(86Kr, X), E=703.5 MeV; calculated σ(fragment θ, E). Scattering matrix approach, multi-channel formulation.

doi: 10.1016/0375-9474(85)90314-8
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1984FE13      Nucl.Phys. A428, 223c (1984)

H.Feldmeier, H.Spangenberger

Particle Exchange as the Dissipative Mechanism in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 166Er(86Kr, X), E=703 MeV; calculated σ(fragment θ, E), mean final energy, θ correlation. 100Mo(40Ar, X), E=270 MeV; calculated mean fragment mass, variance, total kinetic energy correlation. 92Mo, 238U(92Mo, X), E=1352 MeV; calculated σ(fragment θ, E). 238U(27Al, X)(48Ca, X), E=6 MeV/nucleon; calculated σ vs fragment mass. Particle exchange dissipation mechanism.

doi: 10.1016/0375-9474(84)90253-7
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1983CA18      Z.Phys. A313, 57 (1983)

J.Carter, C.Brendel, A.Richter, G.Schrieder, H.Feldmeier, W.Bohne, K.Grabisch, H.Lehr, H.Morgenstern

On the Fusion Dynamics of 40Ar + 40Ca - Fussion-Fission and Fusion-Evaporation

NUCLEAR REACTIONS 40Ca(40Ar, X), E=161, 190, 236, 273 MeV; measured σ(evaporation residue θ), total σ(evaporation residue) vs mass; deduced fusion L(maximum). Trajectory model, rotational, neck degrees of freedom.

doi: 10.1007/BF02115843
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1981BL02      Phys.Lett. 99B, 13 (1981)

J.Blocki, M.Dworzecka, F.Beck, H.Feldmeier

Collective Degrees of Freedom and One-Body Dissipation in Heavy Ion Collisions

NUCLEAR REACTIONS 139La(86Kr, X), E=505, 610, 710 MeV; calculated final kinetic energy vs θ. One-body dissipation, coupling of relative motion to collective degrees of freedom.

doi: 10.1016/0370-2693(81)90794-2
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1981CA11      Z.Phys. A302, 365 (1981)

J.Carter, H.Feldmeier, A.Richter, G.Schrieder, P.Wastyn

Comment on Fusion Cross Sections in the 40Ar + 40Ca and 40Ca + 40Ca Systems

NUCLEAR REACTIONS 40Ca(40Ar, X), (40Ca, X), E(cm)=50-200 MeV; calculated σ(fusion, E). One-body window friction model.

doi: 10.1007/BF01414272
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1980BA48      Z.Phys. A297, 333 (1980)

J.Bartel, H.Feldmeier

One- and Two-Body Dissipation in Peripheral Heavy Ion Collisions

NUCLEAR REACTIONS 16O(16O, X), E(cm)=2-20 MeV/nucleon; calculated excitation energies; deduced one-body dissipation dominance. Peripheral collisions, many-body Schrodinger equation, time-dependent perturbation theory.

doi: 10.1007/BF01422794
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1979WA21      Nucl.Phys. A332, 455 (1979)

P.Wastyn, H.Feldmeier, F.Beck, M.Dworzecka, H.Genz, M.Mutterer, A.Richter, G.Schrieder, J.P.Theobald

Strongly Damped Collisions in the 40Ar + 40Ca System

NUCLEAR REACTIONS 40Ca(40Ar, X), E=191, 236, 272 MeV; measured σ(E, fragment charge, θ).

doi: 10.1016/0375-9474(79)90013-7
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1978BE58      Ann.Phys.(New York) 115, 276 (1978)

H.Behrens, H.Genz, M.Conze, H.Feldmeier, W.Stock, A.Richter

Allowed β-Transitions, Weak Magnetism and Nuclear Structure in Light Nuclei

NUCLEAR STRUCTURE A=12-24; calculated shape factor, asymmetry, anisotropy of electrons from oriented nuclei, βγ(CP), βγ(θ) for allowed β transitions. Elementary particle, impulse approximation treatments.

doi: 10.1016/0003-4916(78)90158-6
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1978BE71      S.Afr.J.Phys. 1, 145 (1978)

F.Beck, M.Dworzecka, H.Feldmeier

Mass and Charge Distribution in Heavy-Ion Collisions

NUCLEAR REACTIONS 165Ho(84Kr, X), E=714 MeV; 209Bi(136Xe, X), E=1130 MeV; 40Ca(40Ca, X), E=236, 272 MeV; calculated fragment A, Z distribution; deduced correlated charge equilibration, relaxed density potentials. One body dissipation, liquid drop proximity potential.


1978DA18      Phys.Rev. C18, 2631 (1978)

K.T.R.Davies, H.T.Feldmeier, H.Flocard, M.S.Weiss

Comparison of Two- and Three-Dimensional Time-Dependent Hartree-Fock Calculations of the Reactions 16O + 16O and 40Ca + 40Ca

NUCLEAR REACTIONS 16O(16O, X), E=105 MeV; 40Ca(40Ca, X), E=192 MeV; calculated energy loss, deflection function in 2-, 3-dimensional time-dependent Hartree-Fock.

doi: 10.1103/PhysRevC.18.2631
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1978GR02      Nucl.Phys. A295, 319 (1978)

H.D.Graf, H.Feldmeier, P.Manakos, A.Richter, E.Spamer, D.Strottman

Study of Electic Monopole Transitions between the Ground State and the First Excited 0+ State in 40,42,44,48Ca with High Resolution Inelastic Electron Scattering

NUCLEAR REACTIONS 40,42,44,48Ca(e, e'), E=31-67 MeV; measured σ(E;Ee';θ). 40,42,44,48Ca 0+ level deduced E0 matrix elements. Shell model calculation.

doi: 10.1016/0375-9474(78)90120-3
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1977FE07      Z.Phys. A281, 379 (1977)

H.Feldmeier, P.Manakos

Perturbation Theory Instead of Large Scale Shell Model Calculations (Question)

NUCLEAR STRUCTURE 20,21,22Ne; analyzed wave functions. 24Mg, 28Si; calculated levels.

doi: 10.1007/BF01408186
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1977KO03      Phys.Rev. C15, 1359 (1977)

S.E.Koonin, K.T.R.Davies, V.Maruhn-Rezwani, H.Feldmeier, S.J.Krieger, J.W.Negele

Time-Dependent Hartree-Fock Calculations for 16O + 16O and 40Ca + 40Ca Reactions

NUCLEAR REACTIONS 16O(16O, X), 40Ca(40Ca, X); calculated interaction. Time-dependent Hartree-Fock.

doi: 10.1103/PhysRevC.15.1359
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1976BO41      Phys.Lett. 65B, 217 (1976)

J.P.Bondorf, H.T.Feldmeier, S.Garpman, E.C.Halbert

Classical Microscopic Description of U + U Collisions

NUCLEAR REACTIONS 235U(235U, X); calculated collision parameters.

doi: 10.1016/0370-2693(76)90166-0
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1973CO03      Phys.Lett. 43B, 101 (1973)

M.Conze, H.Feldmeier, P.Manakos

Special Non-Central Forces for sd-Shell Nuclei

doi: 10.1016/0370-2693(73)90419-X
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1973FE02      Z.Phys. 258, 81 (1973)

H.Feldmeier, P.Manakos, T.Wolff

Influence of Non-Central Interactions on Low Lying States of 24Mg

NUCLEAR STRUCTURE 24Mg; calculated levels, B(E2).

doi: 10.1007/BF01392710
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Note: The following list of authors and aliases matches the search parameter H.Feldmeier: , H.T.FELDMEIER