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NSR database version of May 22, 2024.

Search: Author = H.Reinhardt

Found 35 matches.

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2000AL15      Nucl.Phys. A663-664, 683c (2000)

R.Alkofer, S.Ahlig, C.Fischer, M.Oettel, H.Reinhardt

Octet and Decuplet Baryons in a Confining and Convariant Diquark-Quark Model

doi: 10.1016/S0375-9474(99)00721-6
Citations: PlumX Metrics


1999SC15      Nucl.Phys. A651, 174 (1999)

O.Schroder, H.Reinhardt, H.Weigel

Nucleon Structure Functions in the Three-Flavor NJL Soliton Model

NUCLEAR STRUCTURE 1n, 1H; calculated structure functions. Three-flavor chiral soliton model. Comparisons with data.

doi: 10.1016/S0375-9474(99)00131-1
Citations: PlumX Metrics


1999WE11      Nucl.Phys. B(Proc.Supp.) S74, 125 (1999)

H.Weigel, L.Gamberg, H.Reinhardt, O.Schroder

Nucleon Structure Functions from a Chiral Soliton

doi: 10.1016/S0920-5632(99)00147-4
Citations: PlumX Metrics


1998GA49      Int.J.Mod.Phys. A32, 5519 (1998)

L.Gamberg, H.Reinhardt, H.Weigel

Nucleon Structure Functions from a Chiral Soliton in the Infinite Momentum Frame

NUCLEAR STRUCTURE 1H, 1n; calculated structure functions for deep inelastic scattering.

doi: 10.1142/S0217751X98002511
Citations: PlumX Metrics


1998OE03      Phys.Rev. C58, 2459 (1998)

M.Oettel, G.Hellstern, R.Alkofer, H.Reinhardt

Octet and Decuplet Baryons in a Covariant and Confining Diquark-Quark Model

doi: 10.1103/PhysRevC.58.2459
Citations: PlumX Metrics


1998SC39      Phys.Lett. 439B, 398 (1998)

O.Schroder, H.Reinhardt, H.Weigel

Strangeness Contribution to the Polarized Nucleon Structure Function g1(x)

NUCLEAR STRUCTURE 1n, 1H; calculated polarized structure function g1(x); deduced strange quark contribution. Valence quark approximation to chiral soliton model.

doi: 10.1016/S0370-2693(98)01038-7
Citations: PlumX Metrics


1997HA10      Nucl.Phys. A615, 291 (1997)

T.Haberichter, H.Reinhardt, N.N.Scoccola, H.Weigel

Strangeness Dependence in Radiative Hyperon Decay Amplitudes

doi: 10.1016/S0375-9474(96)00485-X
Citations: PlumX Metrics


1997HE21      Nucl.Phys. A625, 697 (1997)

G.Hellstern, R.Alkofer, H.Reinhardt

Diquark Confinement in an Extended NJL Model

doi: 10.1016/S0375-9474(97)00412-0
Citations: PlumX Metrics


1997HE26      Nucl.Phys. A627, 679 (1997)

G.Hellstern, R.Alkofer, M.Oettel, H.Reinhardt

Nucleon Form Factors in a Covariant Diquark-Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated form factors. Covariant quark-diquark model, Bethe-Salpeter equation.

doi: 10.1016/S0375-9474(97)00514-9
Citations: PlumX Metrics


1997LA25      Nucl.Phys. A622, 620 (1997)

K.Langfeld, H.Reinhardt, M.Rho

A New State of Hadronic Matter at High Density

doi: 10.1016/S0375-9474(97)00364-3
Citations: PlumX Metrics


1997MI26      Nucl.Instrum.Methods Phys.Res. B129, 153 (1997)

R.Michel, R.Bodemann, H.Busemann, R.Daunke, M.Gloris, H.-J.Lange, B.Klug, A.Krins, I.Leya, M.Lupke, S.Neumann, H.Reinhardt, M.Schnatz-Buttgen, U.Herpers, Th.Schiekel, F.Sudbrock, B.Holmqvist, H.Conde, P.Malmborg, M.Suter, B.Dittrich-Hannen, P.-W.Kubik, H.-A.Synal, D.Filges

Cross Sections for the Production of Residual Nuclides by Low- and Medium-Energy Protons from the Target Elements C, N, O, Mg, Al, Si, Ca, Ti, V, Mn, Fe, Co, Ni, Cu, Sr, Y, Zr, Nb, Ba and Au

NUCLEAR REACTIONS, ICPND C, N, O, Mg, 27Al, Si, Ca, Ti, V, Mn, Fe, Co, Ni, Cu, Sr, Y, Zr, Nb, Ba, Au(p, X), E ≈ 10-2500 MeV; measured residuals production σ. Activation, accelerator mass spectrometry techniques.

doi: 10.1016/S0168-583X(97)00213-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0276.


1997WE02      Phys.Lett. 399B, 287 (1997)

H.Weigel, L.Gamberg, H.Reinhardt

Nucleon Structure Functions from a Chiral Soliton

NUCLEAR REACTIONS 1H(ν, ν), (ν-bar, ν-bar), (e, e), E not given; analyzed scattering associated unpolarized structure functions. Chiral soliton approach, bosonized Nambu-Jona-Lasinio model.

doi: 10.1016/S0370-2693(97)00296-7
Citations: PlumX Metrics


1997WE11      Phys.Rev. D55, 6910 (1997)

H.Weigel, L.Gamberg, H.Reinhardt

Polarized Nucleon Structure Functions within a Chiral Soliton Model

NUCLEAR STRUCTURE 1n, 1H; calculated polarized-spin structure functions. Bosonized Nambu-Jona-Lasinio model.

doi: 10.1103/PhysRevD.55.6910
Citations: PlumX Metrics


1997ZU01      Phys.Rev. C55, 2030 (1997)

U.Zuckert, R.Alkofer, H.Weigel, H.Reinhardt

Baryons as Hybrids of Solitons and Three Quark Bound States

doi: 10.1103/PhysRevC.55.2030
Citations: PlumX Metrics


1996AB06      Phys.Lett. 366B, 26 (1996)

A.Abada, H.Weigel, H.Reinhardt

Radiative Decays of Hyperons in the Skyrme Model: E2/M1 transitions ratios

doi: 10.1016/0370-2693(95)01353-9
Citations: PlumX Metrics


1996AL04      Z.Phys. A354, 181 (1996)

R.Alkofer, H.Reinhardt, J.Schlienz, H.Weigel

Topologically Non-Trivial Chiral Transformations. The Chiral Invariant Elimination of the Axial Vector Meson

doi: 10.1007/s002180050031
Citations: PlumX Metrics


1996LA25      Nucl.Phys. A608, 331 (1996)

K.Langfeld, C.Kettner, H.Reinhardt

A Renormalizable Extension of the NJL-Model

doi: 10.1016/S0375-9474(96)00245-X
Citations: PlumX Metrics


1995AB16      Nucl.Phys. A593, 488 (1995)

A.Abada, R.Alkofer, H.Reinhardt, H.Weigel

Monopole Excitations of Baryons in the Nambu-Jona-Lasinio Soliton Model

doi: 10.1016/0375-9474(95)00342-X
Citations: PlumX Metrics


1995BU31      Phys.Lett. 356B, 168 (1995)

A.Buck, H.Reinhardt

Octet and Decuplet Baryons in the Hadronized Nambu-Jona-Lasinio Model with Proper Spin Projection

NUCLEAR STRUCTURE 1H; calculated mass. Hadronized Nambu-Jona-Lasinio model, proper spin projection, other baryons included.

doi: 10.1016/0370-2693(95)00847-E
Citations: PlumX Metrics


1995FR18      Nucl.Phys. A594, 406 (1995)

R.Friedrich, H.Reinhardt

ρω Mixing and the Pion Electromagnetic Form Factor in the Nambu-Jona-Lasinio Model

doi: 10.1016/0375-9474(95)00373-9
Citations: PlumX Metrics


1995LA04      Nucl.Phys. A585, 554 (1995)

R.F.Langbein, H.Reinhardt

Saddle-Point Approximation of Compact Integrals

doi: 10.1016/0375-9474(94)00533-S
Citations: PlumX Metrics


1995WE01      Nucl.Phys. A582, 484 (1995)

H.Weigel, R.Alkofer, H.Reinhardt

Estimate of Quantum Corrections to the Mass of the Chiral Soliton in the Nambu-Jona-Lasinio Model

doi: 10.1016/0375-9474(94)00480-B
Citations: PlumX Metrics


1995WE04      Nucl.Phys. A585, 513 (1995)

H.Weigel, U.Zuckert, R.Alkofer, H.Reinhardt

On the Analytic Properties of Chiral Solitons in the Presence of the (Omega)-Meson

doi: 10.1016/0375-9474(94)00625-W
Citations: PlumX Metrics


1995WE07      Phys.Lett. 353B, 20 (1995)

H.Weigel, A.Abada, R.Alkofer, H.Reinhardt

On the Strange Vector Form Factors of the Nucleon in the NJL Soliton Model

NUCLEAR STRUCTURE 1H, 1n; calculated μ, strange electric, magnetic form factor. Nambu-Jona-Lasinio model.

doi: 10.1016/0370-2693(95)00534-R
Citations: PlumX Metrics


1995ZU03      Phys.Lett. 362B, 1 (1995)

U.Zuckert, R.Alkofer, H.Weigel, H.Reinhardt

Diquarks in a Chiral Soliton Field

doi: 10.1016/0370-2693(95)01206-6
Citations: PlumX Metrics


1994LA21      Nucl.Phys. A579, 472 (1994)

K.Langfeld, H.Reinhardt

SU(N) Instantons and Their Condensation in the Field-Strength Approach

doi: 10.1016/0375-9474(94)90919-9
Citations: PlumX Metrics


1994LA26      Nucl.Phys. A580, 349 (1994)

R.F.Langbein, H.Reinhardt

The Field-Strength Approach on a Lattice

doi: 10.1016/0375-9474(94)90902-4
Citations: PlumX Metrics


1994WE12      Nucl.Phys. A576, 477 (1994)

H.Weigel, R.Alkofer, H.Reinhardt

Hyperons in the Bound-State Approach to the Nambu-Jona-Lasinio Chiral Soliton

doi: 10.1016/0375-9474(94)90742-0
Citations: PlumX Metrics


1994ZU02      Nucl.Phys. A570, 445 (1994)

U.Zuckert, R.Alkofer, H.Reinhardt, H.Weigel

The Chiral Soliton of the Nambu-Jona-Lasinio Model with Vector and Axial-Vector Mesons

doi: 10.1016/0375-9474(94)90068-X
Citations: PlumX Metrics


1993MA50      Nucl.Phys. A565, 543 (1993)

G.Mairle, M.Seeger, H.Reinhardt, T.Kihm, K.T.Knopfle, C.L.Wen

The Distribution of Proton-Hole Strengths in the (2s, 1d)-Shell of 35Cl, 37Cl and 39Cl

NUCLEAR REACTIONS 36,38,40Ar(polarized d, 3He), E=52 MeV; measured σ(θ), iT11(θ). 35,37,39Cl deduced levels, J, π, spectroscopic factors, proton occupancies, single-particle energies, spreading widths. 39Cl deduced mass excess. Enriched 36,38Ar gas targets. DWBA analysis.

doi: 10.1016/0375-9474(93)90044-X
Citations: PlumX Metrics


1993WE07      Phys.Lett. 312B, 6 (1993)

C.Weiss, A.Buck, R.Alkofer, H.Reinhardt

Diquark Electromagnetic Form Factors in a Nambu-Jona-Lasinio Model

NUCLEAR STRUCTURE 1H, 1n; calculated μ. Nambu-Jona-Lasinio model.

doi: 10.1016/0370-2693(93)90477-Y
Citations: PlumX Metrics


1988KI07      Phys.Lett. 208B, 79 (1988)

M.Kirchbach, H.Reinhardt

On the Meson-Exchange Correction to the Axial-Charge Density for ns1/2 → n'p1/2 n'p1/2 → ns1/2 β-Transitions

NUCLEAR STRUCTURE A=16; A=18; A=96; 206Hg, 206Tl(β-); calculated meson-exchange current correction, log ft.

doi: 10.1016/0370-2693(88)91207-5
Citations: PlumX Metrics


1985DZ02      Yad.Fiz. 41, 906 (1985)

R.V.Dzholos, H.Reinhardt, R.Schmidt, R.Schwengner

Microscopic Model of Kinetic Energy Damping in Heavy-Ion Deep Inelastic Collisions

NUCLEAR REACTIONS 238U(238U, X), E=1766 MeV; calculated fragment trajectories, kinetic energy loss time dependence.


1980RE01      Nucl.Phys. A337, 176 (1980)

H.Reinhardt

Application of the Nuclear Field Theory to Superfluid Nuclei: The Quasiparticle-Phonon Multiplet

NUCLEAR STRUCTURE 93Nb; calculated quasiparticle-phonon multiplet energy, B(λ). Nuclear field theory, pairing plus quadrupole force.

doi: 10.1016/0375-9474(80)90085-8
Citations: PlumX Metrics


1976RE05      Nucl.Phys. A262, 231 (1976)

H.Reinhardt

Investigation of Anharmonic Effects in Nuclear Field Theory: The Influence of the Non-Collective Roots

NUCLEAR STRUCTURE 58,60,62Ni; calculated quadrupole moment, B(E2).

doi: 10.1016/0375-9474(76)90617-5
Citations: PlumX Metrics


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