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NSR database version of April 11, 2024.

Search: Author = H.M.Hofmann

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2010KI10      Eur.Phys.J. A 44, 239 (2010)

J.Kirscher, H.W.Griesshammer, D.Shukla, H.M.Hofmann

Universal correlations in pion-less EFT with the resonating group method: Three and four nucleons

NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energy, radius using Refined Resonating Group Method and Effective Field Theory.

NUCLEAR REACTIONS 3He(n, n), E not given; calculated scattering length using Refined Resonating Group Method and Effective Field Theory.

doi: 10.1140/epja/i2010-10939-5
Citations: PlumX Metrics


2009CA28      Nucl.Data Sheets 110, 3215 (2009)

A.D.Carlson, V.G.Pronyaev, D.L.Smith, N.M.Larson, Z.Chen, G.M.Hale, F.-J.Hambsch, E.V.Gai, S.-Y.Oh, S.A.Badikov, T.Kawano, H.M.Hofmann, H.Vonach, S.Tagesen

International Evaluation of Neutron Cross Section Standards

doi: 10.1016/j.nds.2009.11.001
Citations: PlumX Metrics


2008CA28      Nucl.Data Sheets 109, 2834 (2008)

A.D.Carlson, S.A.Badikov, Z.Chen, E.Gai, G.M.Hale, F.-J.Hambsch, H.M.Hofmann, T.Kawano, N.M.Larson, S.Y.Oh, V.G.Pronyaev, D.L.Smith, S.Tagesen, H.Vonach

Covariances Obtained from an Evaluation of the Neutron Cross Section Standards

NUCLEAR REACTIONS 6Li(n, t), E < 1 MeV; 10B(n, α), E < 1 MeV; analyzed cross sections.

doi: 10.1016/j.nds.2008.11.019
Citations: PlumX Metrics


2008HO04      Phys.Rev. C 77, 044002 (2008)

H.M.Hofmann, G.M.Hale

4He experiments can serve as a database for determining the three-nucleon force

NUCLEAR REACTIONS 3H(p, p), (polarized p, p), (p, n), E<11 MeV; 3He(n, n), (polarized n, n), E<10 MeV; 2H(polarized d, p), (polarized d, n), (polarized d, d), (d, p), (d, n), (d, d), E<10 MeV; calculated phase shifts, angular momentum, σ(θ), analyzing powers. Microscopic calculations for 4He compound system using relativistic nucleon-nucleon and three-nucleon forces. R-matrix analysis. Comparisons with experimental data.

doi: 10.1103/PhysRevC.77.044002
Citations: PlumX Metrics


2008HO12      Nucl.Data Sheets 109, 2807 (2008)

H.M.Hofmann

Towards Covariances from Nuclear Theory for Light Nuclei

NUCLEAR REACTIONS 2H(n, n), E < 20 MeV; 3He(n, p), E(cm) < 45 MeV; 6Li(n, t), E < 10 MeV; calculated cross sections.

doi: 10.1016/j.nds.2008.11.014
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2004PR09      Phys.Rev. C 70, 055801 (2004)

R.M.Prior, M.C.Spraker, A.M.Amthor, K.J.Keeter, S.O.Nelson, A.Sabourov, K.Sabourov, A.Tonchev, M.Ahmed, J.H.Kelley, D.R.Tilley, H.R.Weller, H.M.Hofmann

Energy dependence of the astrophysical S factor for the 6Li(p, γ)7Be reaction

NUCLEAR REACTIONS 6Li(polarized p, γ), E=80, 95, 110, 120, 130 keV; measured Eγ, Iγ, analyzing power; deduced energy dependence of astrophysical S-factor.

doi: 10.1103/PhysRevC.70.055801
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1136.


2004SA61      Phys.Rev. C 70, 064601 (2004)

K.Sabourov, M.W.Ahmed, R.S.Canon, B.Crowley, K.Joshi, J.H.Kelley, S.O.Nelson, B.A.Perdue, E.C.Schreiber, A.Sabourov, A.Tonchev, H.R.Weller, E.A.Wulf, R.M.Prior, M.C.Spraker, H.M.Hofmann, M.Trini

Experimental and theoretical study of the 2H(d(pol), γ)4He reaction below Ec.m.=60keV

NUCLEAR REACTIONS 2H(polarized d, γ), E<115 keV; measured Eγ, Iγ, σ(θ), Ay(θ), T20(θ); deduced transition matrix elements. Comparison with resonating group model predictions.

doi: 10.1103/PhysRevC.70.064601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1493.


2003HO14      Phys.Rev. C 68, 021002 (2003)

H.M.Hofmann, G.M.Hale

Microscopic calculation of the spin-dependent neutron scattering lengths on 3He

NUCLEAR REACTIONS 3He(n, p), E(cm) ≈ 1-40 keV; calculated σ. 3He(n, X), E not given; calculated spin-dependent scattering lengths. R-matrix analysis, microscopic calculation using realistic two- and three-nucleon forces.

doi: 10.1103/PhysRevC.68.021002
Citations: PlumX Metrics


2003RE04      Nucl.Phys. A716, 107 (2003)

C.Reiss, H.M.Hofmann

The Ay problem in refined resonating group model calculations for p-3He scattering

NUCLEAR REACTIONS 3He(p, p), E(cm)=5.2, 22.5 MeV; calculated phase shifts, σ(θ), Ay(θ). Refined resonating group model, comparison with data.

doi: 10.1016/S0375-9474(02)01587-7
Citations: PlumX Metrics


2002TI10      Nucl.Phys. A708, 3 (2002)

D.R.Tilley, C.M.Cheves, J.L.Godwin, G.M.Hale, H.M.Hofmann, J.H.Kelley, C.G.Sheu, H.R.Weller

Energy Levels of Light Nuclei A = 5, 6, 7

COMPILATION 5,6n, 5,6,7H, 5,6,7He, 5,6,7Li, 5,6,7Be, 6,7B, 6C; compiled, evaluated structure data.

doi: 10.1016/S0375-9474(02)00597-3
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This article is in the ENSDF database. For more information, select a mass: 5 , 6 , 7 .


2001PF02      Phys.Rev. C64, 044003 (2001)

B.Pfitzinger, H.M.Hofmann, G.M.Hale

Elastic p-3He and n-3H Scattering with Two- and Three-Body Forces

NUCLEAR REACTIONS 3He(p, p), 3H(n, n), E(cm)=0-5 MeV; calculated phase shifts, σ(θ), σ. Two- and three-nucleon forces, R-matrix analysis.

doi: 10.1103/PhysRevC.64.044003
Citations: PlumX Metrics


1997HO01      Nucl.Phys. A613, 69 (1997)

H.M.Hofmann, G.M.Hale

Microscopic Calculation of the 4He System

NUCLEAR STRUCTURE 4He; calculated point Coulomb form factors, levels. Resonating group model.

NUCLEAR REACTIONS 3He(n, n), 3H(p, p), 2H(d, d), E(cm) ≤ 12.5 MeV; calculated phase shifts vs E. 3H(p, p), (polarized p, p), 3H(p, n), 3He(n, n), 3He(polarized n, n), E(cm)=3 MeV; analyzed σ(θ), analyzing power data. 2H(d, p), (d, n), E(cm)=2.11 MeV; analyzed σ(θ). 2H(polarized d, p), E(cm)=2-11 MeV; analyzed iT11(θ), T20(θ), T21(θ), T22(θ). 2H(polarized d, n), E(cm)=2.11 MeV; analyzed vector analyzing power vs θ. 2H(d, d), E(cm)=3.11 MeV; analyzed σ(θ). 2H(polarized d, d), E(cm)=3.11 MeV; analyzed iT11(θ), T20(θ), T21(θ), T22(θ). Resonating group model.

doi: 10.1016/S0375-9474(96)00418-6
Citations: PlumX Metrics


1997WI03      Phys.Rev. C55, 684 (1997)

C.Winkler, H.M.Hofmann

Determination of Bound-State Wave Functions by a Genetic Algorithm

NUCLEAR STRUCTURE 7Li; calculated binding energy, convergence related features. Genetic algorithm, resonating group method.

doi: 10.1103/PhysRevC.55.684
Citations: PlumX Metrics


1997WU01      Phys.Rev. C55, 688 (1997)

J.Wurzer, H.M.Hofmann

Structure of the Helium Isotopes 4He-8He

NUCLEAR STRUCTURE 6He; calculated binding energy, matter, charge rms point nucleon radii, levels. 8He; calculated matter, charge, rms point matter, charge density distributions, 4n-breakup threshold energies. 7He; calculated levels.

NUCLEAR REACTIONS 6He(n, n), (n, n'), E(cm) ≤ 20 MeV; calculated phase shifts vs E. 6He(p, p), E=high; calculated differential σ.

doi: 10.1103/PhysRevC.55.688
Citations: PlumX Metrics


1996WU01      Z.Phys. A354, 135 (1996)

J.Wurzer, H.M.Hofmann

Microscopic Multi-Channel Calculations for the 10Li System

NUCLEAR STRUCTURE 10Li; calculated levels. Microscopic multi-channel calculation, refined resonating group method.

NUCLEAR REACTIONS 9Li(n, n), E ≤ 10 MeV; calculated phase shift vs E. Microscopic multi-channel calculation, refined resonating group method.

doi: 10.1007/s002180050024
Citations: PlumX Metrics


1995KE14      Phys.Rev. D51, 3936 (1995)

J.Keppler, H.M.Hofmann

Spin Structure of the Proton in a Nonrelativistic Quark Model

NUCLEAR STRUCTURE 1H; calculated spin structure. Extended quark potential.

doi: 10.1103/PhysRevD.51.3936
Citations: PlumX Metrics


1995TO08      Phys.Rev. C52, 1963 (1995)

E.L.Tomusiak, W.Leidemann, H.M.Hofmann

Photon Polarization in the 4He(γ, d(pol))2H Reaction

NUCLEAR REACTIONS 4He(polarized γ, d), E=50 MeV; calculated σ(θ), photon asymmetry, polarization observables vs θ.

doi: 10.1103/PhysRevC.52.1963
Citations: PlumX Metrics


1994KE09      Phys.Rev. C50, 237 (1994)

C.D.Keith, C.R.Gould, D.G.Haase, N.R.Roberson, W.Tornow, G.M.Hale, H.M.Hofmann, H.Postma

Sensitivity of Polarized Neutron-Polarized 3He Scattering to the Excited Level Structure of 4He

NUCLEAR REACTIONS 3He(polarized n, n), (n, n), E=0.1-10 MeV; calculated σ(E), total longitudinal, transverse σ differences; deduced sensitivity to 4He level structure. Multi-channel resonating group model, polarized target.

doi: 10.1103/PhysRevC.50.237
Citations: PlumX Metrics


1994WE10      Phys.Rev. C50, 1492 (1994)

S.Weber, M.Kachelriess, M.Unkelbach, H.M.Hofmann

6Li Inelastic Form Factors in a Cluster Model

NUCLEAR REACTIONS 6Li(e, e'), E not given; calculated longitudinal, transverse form factors. Resonating group model.

doi: 10.1103/PhysRevC.50.1492
Citations: PlumX Metrics


1992UN02      Nucl.Phys. A549, 550 (1992)

M.Unkelbach, H.M.Hofmann

Meson-Exchange Currents in Electromagnetic Transitions of the 4He System

NUCLEAR REACTIONS 4He(γ, p), E=20-50 MeV; 4He(γ, n), E=20-50 MeV; calculated σ(E). 3He(polarized p, γ), E=2-9 MeV; calculated analyzing power vs θ. 4He(e, e'p), (e, e'n), E not given; calculated σ(θ(e'), θ(nucleon), energy transfer). Refined resonating group model, meson exchange currents.

doi: 10.1016/0375-9474(92)90665-7
Citations: PlumX Metrics


1991BR02      Phys.Rev. C43, 201 (1991)

M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann

Isospin Breaking Effects in the Reaction 4He(d, 3He)3H at Low Energies

NUCLEAR REACTIONS 4He(d, 3He), E=23-25 MeV; measured σ(θ); deduced σ asymmetry, S-matrix elements. Resonating group model predictions comparison.

doi: 10.1103/PhysRevC.43.201
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1566.


1991UN01      Phys.Lett. 261B, 211 (1991)

M.Unkelbach, H.M.Hofmann

7Li Form Factors in a Microscopic Cluster Calculation

NUCLEAR REACTIONS 7Li(e, e'), E not given; calculated longitudinal, transverse form factors. Microscopic cluster structure, resonating group model, meson effects.

doi: 10.1016/0370-2693(91)90316-I
Citations: PlumX Metrics


1991UN02      Few-Body Systems 11, 143 (1991)

M.Unkelbach, H.M.Hofmann

6Li Elastic Form Factors and Antisymmetrization

NUCLEAR REACTIONS 6Li(e, e), E not given; calculated longitudinal, transverse form factors. Resonating group method.

doi: 10.1007/BF01318559
Citations: PlumX Metrics


1990BR09      Phys.Rev. C41, 2435 (1990)

M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann

Isospin Breaking in the Analyzing Power of 3H(3He, 2H)4He and the Inverse Reaction

NUCLEAR REACTIONS 3H(polarized 3He, d), E=18 MeV; calculated analyzing power; deduced isospin symmetry violation matrix element. Resonating group model.

doi: 10.1103/PhysRevC.41.2435
Citations: PlumX Metrics


1989BR23      Nucl.Phys. A501, 462 (1989)

M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann, B.Vuaridel, W.Gruebler, V.Konig, P.A.Schmelzbach, K.Elsener

Barshay-Temmer Test for the 4He(d(pol), 3He)3H Reaction

NUCLEAR REACTIONS 4He(d, 3He), E(cm)=14-33 MeV; measured σ(θ, E), iT11(θ, E); deduced asymmetries with respect to θ(cm)=90°, isospin violation magnitude. Resonating group calculations.

doi: 10.1016/0375-9474(89)90141-3
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1989KE09      Few-Body Systems 7, 31 (1989)

H.Kellermann, H.M.Hofmann, Ch.Elster

Gaussian Parametrization of a Meson-Theoretical N-N Potential for Microscopic Nuclear-Structure Calculations

NUCLEAR STRUCTURE 2H; calculated binding energy, rms radius, quadrupole moment, μ, D-state probability. Bonn potential.

doi: 10.1007/BF01078436
Citations: PlumX Metrics


1989SP05      Phys.Rev.Lett. 63, 1574 (1989)

M.Spahn, Th.Kihm, K.T.Knopfle, J.Friedrich, N.Voegler, Ch.Schmitt, V.H.Walther, M.Unkelbach, H.M.Hofmann

Study of Charge Symmetry in 4He by Simultaneous 4He(e, e'p)3H and 4He(e, e'n)3He Measurements

NUCLEAR REACTIONS 4He(e, e'p), (e, e'n), E=183.4 MeV; measured σ(θ(e'), θ(p)), σ(θ(e'), θ(n)); deduced σ. 4He deduced no charge symmetry breaking in GDR region.

doi: 10.1103/PhysRevLett.63.1574
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1988LA14      Phys.Rev. C38, 565 (1988)

J.L.Langenbrunner, G.Feldman, H.R.Weller, D.R.Tilley, B.Wachter, T.Mertelmeier, H.M.Hofmann

2H(d(pol), γ)4He Reaction at E(d) = 1.2 MeV

NUCLEAR REACTIONS 2H(polarized d, γ), E=1.2 MeV; measured σ(θ), analyzing power vs θ; deduced γ-multipolarity, relative transition strengths. Microscopic multi-channel resonating group model.

doi: 10.1103/PhysRevC.38.565
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1284.


1988WA02      Phys.Lett. 200B, 246 (1988)

B.Wachter, T.Mertelmeier, H.M.Hofmann

The 2H(d, γ)4He Reaction and the D-State of the Alpha Particle: A microscopic study

NUCLEAR REACTIONS, ICPND, MECPD 2H(polarized d, γ), E=10 MeV; calculated σ(θ), analyzing powers, capture σ, astrophysical S(E). Microscopic multi-channel resonating group model.

doi: 10.1016/0370-2693(88)90764-2
Citations: PlumX Metrics


1988WA20      Phys.Rev. C38, 1139 (1988)

B.Wachter, T.Mertelmeier, H.M.Hofmann

Differences in the Mirror Reactions 3H(p, γ)4He and 3He(n, γ)4He from an Isospin Conserving Nuclear Force

NUCLEAR REACTIONS 3H(p, γ), 3He(n, γ), E=0.1-50 MeV; calculated σ(Eγ), σ(θ); deduced no evidence for charge symmetry breaking. Multi-channel resonating group model.

doi: 10.1103/PhysRevC.38.1139
Citations: PlumX Metrics


1986ME13      Nucl.Phys. A459, 387 (1986)

T.Mertelmeier, H.M.Hofmann

Consistent Cluster Model Description of the Electromagnetic Properties of Lithium and Beryllium Nuclei

NUCLEAR STRUCTURE 6Li; calculated charge radius, μ, quadrupole moment, B(λ). 7Li, 7Be; calculated rms, charge radii, μ, quadrupole moment, B(λ). Cluster model.

NUCLEAR REACTIONS, ICPND 3H, 3He(α, γ), E ≤ 3 MeV; calculated electric dipole capture σ(E), astrophysical S-factor vs E. Cluster model.

doi: 10.1016/0375-9474(86)90141-7
Citations: PlumX Metrics


1984HO10      Phys.Rev.Lett. 52, 2038 (1984)

H.M.Hofmann, D.Fick

Fusion of Polarized Deuterons

NUCLEAR REACTIONS, ICPND 2H(polarized d, n), E(cm) ≤ 150 keV; calculated total reaction σ(E), σ(θ) anisotropy, attenuation vs E; deduced nonsuppression of fusion, neutron production processes. Discussion of d-3He fusion reactor implications.

doi: 10.1103/PhysRevLett.52.2038
Citations: PlumX Metrics


1983HO11      Z.Phys. A311, 289 (1983)

H.M.Hofmann, T.Mertelmeier, H.A.Weidenmuller

Influence of Statistical Experimental Errors on Amplitude Correlations in Resonance Spectroscopy

NUCLEAR REACTIONS 44Ca(p, p'), E ≈ resonance; analyzed data. 45Sc resonances deduced reduced partial width distribution, deviations from multi-variate Gaussian. Statistical analysis.

doi: 10.1007/BF01415683
Citations: PlumX Metrics


1983HO22      Nucl.Phys. A410, 208 (1983)

H.M.Hofmann, T.Mertelmeier, W.Zahn

The Nuclear Systems 7Li and 7Be in a Resonating Group Model

NUCLEAR REACTIONS 4He(3He, 3He), 6Li(p, p), E=1-13 MeV; calculated phase shifts vs E. 4He(3He, 3He), E=4, 10 MeV; calculated σ(θ). 4He(polarized 3He, 3He), E=8, 10 MeV; calculated analyzing power vs θ. 6Li(p, p), (polarized p, p), E=1.94, 3.94, 5.94 MeV; calculated σ(θ), analyzing power vs θ. 6Li(p, p), E=3.94, 5.94 MeV; calculated analyzing power vs θ. Polarized target. 6Li(p, p'), (polarized p, p'), E=5.94 MeV; calculated σ(θ), proton polarization, analyzing power vs θ. 4He(3He, p), (polarized 3He, p), E=6, 8, 10 MeV; calculated proton polarization, analyzing power vs θ. 6Li(polarized p, d), E=3.94, 5.94 MeV; calculated proton analyzing power vs θ. Resonating group model.

NUCLEAR STRUCTURE 7Li, 7Be; calculated levels, reaction threshold energies. Resonating group model.

doi: 10.1016/0375-9474(83)90199-9
Citations: PlumX Metrics


1982HO05      Czech.J.Phys. B32, 288 (1982)

H.M.Hofmann, W.Zahn

On the Further Development of the Resonating Group Approach

NUCLEAR REACTIONS 1H(polarized t, t), 3H(polarized p, p), E(cm)=3.2, 3.7 MeV; calculated analyzing power vs θ. 6Li(γ, 3He), E=15-35 MeV; calculated σ(total) vs E. 12C(12C, α), E(cm)=4-8 MeV; calculated astrophysical strength function. Resonating group method, SU(3) cluster model.

NUCLEAR STRUCTURE 6Be; calculated levels. Resonating group method, SU(3) cluster model.

doi: 10.1007/BF01602070
Citations: PlumX Metrics


1981HE13      Phys.Lett. 103B, 92 (1981)

K.T.Hecht, H.M.Hofmann, W.Zahn

Toward a Microscopic Description of the Sub-Coulomb 12C + 12C Resonances

NUCLEAR REACTIONS 12C(12C, α), E not given; calculated resonance energy, strength factor. Microscopic coupled-cluster model, antisymmetrized SU(3) basis, quadrupole-quadrupole interaction, important exit channels.

doi: 10.1016/0370-2693(81)90677-8
Citations: PlumX Metrics


1981HO04      Nucl.Phys. A357, 139 (1981)

H.M.Hofmann, W.Zahn, H.Stowe

Microscopic Multi-Channel Calculations for the A = 4 Systems

NUCLEAR REACTIONS 3H(n, n), E(cm)=1-5 MeV; 3He, 3H(p, p), 3He(n, n), 2H(d, d), E(cm)=1-10 MeV; calculated phase shifts; 2H(d, n), (d, p), E=2, 3, 4 MeV; calculated polarization vs θ; 3H(polarized p, p), 1H(polarized t, t), E(cm)=3.2, 3.7 MeV; calculated A(θ). 4He deduced levels, J, π, T. Resonating group theory, multi-channel calculations.

doi: 10.1016/0375-9474(81)90630-8
Citations: PlumX Metrics


1981HO23      Nucl.Phys. A368, 29 (1981)

H.M.Hofmann, W.Zahn

Microscopic Multi-Channel Calculations for the 6Be System

NUCLEAR REACTIONS 3He(polarized 3He, 3He), (3He, 3He), (polarized 3He, p), (3He, p), E(cm)=6-16 MeV; calculated σ(θ), vector polarization vs θ, phase shifts. 6Be deduced resonances, J, π. Microscopic multi-channel calculations, resonating group model.

doi: 10.1016/0375-9474(81)90728-4
Citations: PlumX Metrics


1980HO34      Z.Phys. A297, 153 (1980)

H.M.Hofmann, T.Mertelmeier, M.Herman, J.W.Tepel

Hauser-Feshbach Calculations in the Presence of Weakly Absorbing Channels with Special Reference to the Elastic Enhancement Factor and the Factorization Assumption

doi: 10.1007/BF01421472
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1976HO14      Nucl.Phys. A266, 138 (1976)

H.M.Hofmann, Y.Starkand, M.W.Kirson

Perturbation Theory and Pade Approximants in Realistic Large-Matrix Models of the Nuclear Effective Interaction

NUCLEAR STRUCTURE 18O; calculated energy matrices for J, π, T=0, +, 1 states.

doi: 10.1016/0375-9474(76)90287-6
Citations: PlumX Metrics


1975HO23      Ann.Phys.(New York) 90, 403 (1975)

H.M.Hofmann, J.Richert, J.W.Tepel, H.A.Weidenmuller

Direct Reactions and Hauser-Feshbach Theory

doi: 10.1016/0003-4916(75)90005-6
Citations: PlumX Metrics


1973DI08      Phys.Lett. 44B, 484 (1973)

M.Dillig, H.M.Hofmann, M.G.Huber

Microscopic Description of Nuclear π+ Production in 12C

NUCLEAR REACTIONS 12C(p, π+), E=185 MeV; calculated σ(Eπ+, θ).

doi: 10.1016/0370-2693(73)90003-8
Citations: PlumX Metrics


1973HO23      Nucl.Phys. A209, 233 (1973)

H.M.Hofmann

Comparison of Short-Range Correlation and Distortion Effects in Quasielastic Electron Scattering

NUCLEAR REACTIONS 16O(e, e'p), E=2.5 GeV; measured nothing, calculated σ(θ(p)). Single particle model.

doi: 10.1016/0375-9474(73)90575-7
Citations: PlumX Metrics


1970HO32      Z.Phys. 240, 420 (1970)

H.M.Hofmann, D.Fick

Three-Body Calculations of Elastic Deuteron-Helium-4-Scattering with Faddeev Equations

NUCLEAR REACTIONS 4He(d, d), E < 10 MeV; calculated phase shifts.

doi: 10.1007/BF01395578
Citations: PlumX Metrics


1969KI04      Nucl.Phys. A126, 529 (1969)

K.Kilian, G.Clausnitzer, W.Durr, D.Fick, R.Fleischmann, H.M.Hofmann

Untersuchung der Reaktionen 7Li(p, p0)7Li, 7Li(p, p1)7Li* und 7Li(p, α)4He mit Polarisierten Protonen der Energie 2.7 bis 10.6 MeV

NUCLEAR REACTIONS 7Li(p, p0), (p, p1), (p, α), E=2.7-10.6 MeV; measured σ(E;θ), polarization analyzing power (E, θ). Enriched target.

doi: 10.1016/0375-9474(69)90845-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1443.


1968DU07      Nucl.Phys. A120, 678 (1968); Erratum Nucl.Phys. A141, 673 (1970)

W.Durr, G.Clausnitzer, D.Fick, R.Fleischmann, H.M.Hofmann, K.Kilian

Die Analysierstarke der Reaktion 6Li(d, α)4He mit Vektorpolarisierten Deuteronen der Energie 2.1-10.9 MeV

NUCLEAR REACTIONS 6Li(polarized d, α), E=2.1-10.9 MeV; measured polarization-analyzing power (E, θ). Enriched target.

doi: 10.1016/0375-9474(68)90472-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1375.


1968DU09      Nucl.Phys. A122, 153(1968)

W.Durr, G.Clausnitzer, D.Fick, R.Fleischmann, H.M.Hofmann, K.Kilian

Untersuchung der j-Abhangigkeit der Vektoranalysierstarke der Reaktionen 6Li(d, p0) und 6Li(d, p1) mit Rein Vektorpolarisierten Deuteronen der Energie 2.1-10.9 MeV

NUCLEAR REACTIONS 6Li(d, p), (polarized d, p), E=2.1-10.9 MeV; measured σ(E; Ep, θ), vector-polarization analyzing power A(E; Ep, θ). Enriched target.

doi: 10.1016/0375-9474(68)90709-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1376.


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