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NSR database version of May 24, 2024.

Search: Author = D.Halderson

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2016GR09      Phys.Rev. C 94, 014617 (2016)

J.Grineviciute, D.Halderson

Relativity versus exchange currents in 16O(e, e'p)

NUCLEAR REACTIONS 16O(e, e'p)15N, E=100, 172 MeV; calculated cross sections for p1/2 and p3/2 states, and response functions in quasi-elastic region using recoil corrected continuum shell model; Calculated meson exchange currents and relativistic effects via direct Pauli reduction.

doi: 10.1103/PhysRevC.94.014617
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2013GR11      Phys.Rev. C 88, 027602 (2013)

J.Grineviciute, D.Halderson

Higher-order corrections to electron-scattering multipoles

NUCLEAR REACTIONS 16O(e, e'), E not given; calculated nucleon form factors for lowest 2- and 3- states in 16O. Role of relativity and higher order correction terms. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.027602
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2013HA17      Phys.Rev. C 88, 014610 (2013)

D.Halderson

Recoil-corrected continuum shell model calculations for 11B(p, n)11C, 11B(p, p')11B*, 12C(e, e'x)

NUCLEAR REACTIONS 11B(p, n), E=30, 50 MeV; 11B(p, p), E=30.3, 155 MeV; 11B(p, p'), E=30 MeV; calculated σ(θ). 12C(e, e'X), E=480, 620, 680, 1500 MeV; calculated cross sections, longitudinal and transverse responses. Recoil-corrected continuum shell model calculations (RCCSM). Comparison with experimental data.

doi: 10.1103/PhysRevC.88.014610
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2012GR09      Phys.Rev. C 85, 054617 (2012)

J.Grineviciute, D.Halderson

Relativistic R matrix and continuum shell model

NUCLEAR STRUCTURE 90Zr, 16O; calculated single particle energies. quantum hydrodynamics (QHD), Hartree-Fock parameters, R-matrix level energies for 2-.

NUCLEAR REACTIONS 15N(p, p), E=39.84 MeV; calculated σ(θ). Relativistic R matrix formalism in a relativistic continuum shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.054617
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2009GR12      Phys.Rev. C 80, 044607 (2009)

J.Grineviciute, D.Halderson

Dirac oscillators and the relativistic R matrix

NUCLEAR REACTIONS 16O(p, p), E=200 MeV; 40Ca(p, p), E=9.0, 181, 200 MeV; 90Zr(p, p), E=160 MeV; calculated σ(θ), analyzing powers using relativistic impulse approximation calculations. Dirac oscillators. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.044607
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2008GR07      J.Phys.(London) G35, 055102 (2008)

J.Grineviciute, D.Halderson

Proton capture by 14N at astrophysical energies

NUCLEAR REACTIONS 14N(p, γ), E(cm) < 0.5 MeV; calculated S-factor. Comparison to data.

doi: 10.1088/0954-3899/35/5/055201
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2008HA07      Phys.Rev. C 77, 034304 (2008)

D.Halderson

p-shell Λ hypernuclei with the Nijmegen ESC04 baryon-baryon potential

NUCLEAR STRUCTURE 5He, 7Li, 9Be, 10,11B, 12C, 15N, 16O; calculated excitation spectra for hypernuclei. 4He, 16O; calculated level splittings using Nijmegen ESCO4 baryon-baryon interaction.

doi: 10.1103/PhysRevC.77.034304
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2007HA46      Phys.Rev. C 76, 047301 (2007)

D.Halderson

Λ-hypernuclei single-particle energies with the Nijmegen ESC04 baryon-baryon interaction

doi: 10.1103/PhysRevC.76.047301
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2006HA09      Phys.Rev. C 73, 024612 (2006)

D.Halderson

Reactions in the 8B and 8Li compound systems

NUCLEAR REACTIONS 7Be(p, γ), E(cm)=0-3 MeV; calculated S-factor, angular distribution coefficients. 7Be(p, p), (p, p'), E(cm)=0.5-3.5 MeV; calculated excitation functions, σ(θ). 7Li(n, γ), E=0-1000 MeV; calculated capture σ, angular distribution coefficients. 7Li(n, n'), E=0.4-1.7 MeV; calculated σ. Recoil-corrected continuum shell model.

doi: 10.1103/PhysRevC.73.024612
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2005HA26      Int.J.Mod.Phys. E14, 171 (2005)

D.Halderson

The continuum shell model with full correction for target recoil

NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=162 MeV; 12C(π+, K+), E not given; 7Be(p, p'), E(cm)=1-3.5 MeV; 3He(p, p), E=85 MeV; calculated σ(E, θ). 4He(γ, p), E(cm)=0-30 MeV; calculated σ. 6,7Li(p, p), E=49.75 MeV; calculated σ(θ), Ay(θ). Recoil-corrected continuum shell model, comparisons with data.

doi: 10.1142/S0218301305002977
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2004HA04      Phys.Rev. C 69, 014609 (2004)

D.Halderson

Continuum shell model predictions for 7Be+p

NUCLEAR REACTIONS 7Li(p, p), E=49.75 MeV; 6Li(p, p), E=0.4, 0.9 MeV; calculated σ(θ), Ay(θ). 7Be(p, p), E(cm)=1-4 MeV; calculated elastic excitation function, σ(θ=148°), Ay(θ=148°). Recoil corrected continuum shell model.

doi: 10.1103/PhysRevC.69.014609
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2004HA45      Phys.Rev. C 70, 034607 (2004)

D.Halderson

σ(γ, p)/σ(γ, n) ratio, current conservation, and nucleon scattering in 4He

NUCLEAR REACTIONS 4He(γ, p), (γ, n), E not given; calculated σ(E). 3He(p, p), E=40.5, 85 MeV; calculated σ(θ). General recoil-corrected continuum shell model, comparison with data.

doi: 10.1103/PhysRevC.70.034607
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2004HA49      Phys.Rev. C 70, 041603 (2004)

D.Halderson

Evidence for the 1/2- state in 7He

NUCLEAR REACTIONS 6He(p, n), E(cm)=0.5-3.5 MeV; 6He(n, n), E(cm)=0.05-1.5 MeV; analyzed excitation functions, σ(θ). 7He deduced resonance energy, width. Recoil-corrected continuum shell model.

doi: 10.1103/PhysRevC.70.041603
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2002HA36      Nucl.Phys. A707, 65 (2002)

D.Halderson

The p-Shell with One Particle in the Continuum

NUCLEAR REACTIONS 6Li(p, p), (p, p'), E=24.4-136 MeV; 6Li(n, n'), E=24 MeV; 6Li(n, p), E=120 MeV; 6Li(p, n), E=30.2-120 MeV; calculated σ(θ). 6Li(polarized p, p), (polarized p, p'), E=49.75-80 MeV; calculated Ay(θ). Continuum shell model, target recoil correction, comparisons with data.

doi: 10.1016/S0375-9474(02)00881-3
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2000HA12      Phys.Rev. C61, 034001 (2000)

D.Halderson

Λ-Hypernuclear Binding Energy Test of the Refit Nijmegen Soft Core YN Potential

NUCLEAR STRUCTURE 5He, 13C, 17O, 41,49Ca, 91Zr, 209Pb; calculated hypernuclei binding energies, Λ single-particle energies. First order Brueckner-Hartree calculations, Nijmegen soft core potential.

doi: 10.1103/PhysRevC.61.034001
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1999HA60      Phys.Rev. C60, 064001 (1999)

D.Halderson

Nijmegen Soft Core YN Potential with Bound State Restrictions

doi: 10.1103/PhysRevC.60.064001
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1997HA48      Phys.Rev. C56, 2688 (1997)

D.Halderson, V.A.Sadovnikova

Origin of Anomalous Values of σ(π+, π+'p)/σ(π-, π-'p)

NUCLEAR REACTIONS 4He(π+, π+), E=180 MeV; analyzed σ(θ); 4He(π+, π+'), (π+, π+'p), (π-, π-'p), E not given; analyzed σ(E, θ); deduced neutron excitation role.

doi: 10.1103/PhysRevC.56.2688
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1996HA15      Phys.Rev. C53, 2978 (1996)

D.Halderson

Calculations for 4He(e, e'N)

NUCLEAR REACTIONS 4He(e, e'p), (e, e'n), E=183.4 MeV; calculated σ(θ, E(nucleon)). 4He(e, e'X), E=320-589 MeV; calculated inclusive σ(θ, E). Recoil corrrected continuum shell model.

doi: 10.1103/PhysRevC.53.2978
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1994HA48      J.Phys.(London) G20, 1461 (1994)

D.Halderson

Effective Interactions and Nucleon Scattering from Light Nuclei

NUCLEAR REACTIONS 3H(p, p), E=4.5-156 MeV; 3H(p, n), E=156 MeV; 3He(p, p), E=85, 156 MeV; 4He(p, p), E=85 MeV; calculated σ(θ). 3H(p, p), E=19-40.5 MeV; calculated proton polarization P(θ). 12C(p, p), (p, p'), E=62 MeV; calculated σ(θ). Nucleon-nucleon potentials based effective interaction.

doi: 10.1088/0954-3899/20/9/015
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1993HA15      Phys.Rev. C48, 581 (1993)

D.Halderson

g-Matrix Calculations in Finite Hypernuclei

NUCLEAR STRUCTURE A=5, 17, 41; calculated hypernuclei binding energies. Nijmegen model potentials, g-matrix calculations.

doi: 10.1103/PhysRevC.48.581
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1992HA01      Phys.Rev. C45, 42 (1992)

D.Halderson

Theoretical Study of 4He(e, e')4He(*)

NUCLEAR REACTIONS 4He(e, e'), E=60.6-200 MeV; analyzed data. Recoil-corrected continuum shell model.

doi: 10.1103/PhysRevC.45.42
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1992ZH03      Phys.Rev. C45, 563 (1992)

Y.Zhang, D.Halderson

Eta Photoproduction via 2H(γ, (Eta))2H

NUCLEAR REACTIONS 2H(γ, X), E=700-860 MeV; calculated eta production σ(θ) vs E, isospin dependence. Impulse approximation.

doi: 10.1103/PhysRevC.45.563
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1990HA36      Phys.Rev. C42, 2584 (1990)

D.Halderson, A.S.Rosenthal

Photoproduction of Eta Mesons from Nuclei

NUCLEAR REACTIONS 12C, 16O, 24Mg, 28Si(γ, X), E < 760 MeV; calculated eta production σ(θ). Impulse approximation, (e, e') transition densities.

doi: 10.1103/PhysRevC.42.2584
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1989HA02      Phys.Rev. C39, 336 (1989)

D.Halderson, M.Yu, J.Yu

Structure of the First Excited State of 4He

NUCLEAR REACTIONS 4He(e, e'), (e, e), E not given; calculated form factors. Recoil corrected shell model.

doi: 10.1103/PhysRevC.39.336
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1989HA32      Phys.Rev. C40, 2173 (1989)

D.Halderson

Σ-Hypernuclear Production in Flight

NUCLEAR REACTIONS 12C(K-, π-), E at 400 MeV/c; 12C, 16O(K-, π+), E at 450 MeV/c; 9Be(K-, π-), E at 720 MeV/c; calculated σ(θ, E(π)). Continuum shell model.

doi: 10.1103/PhysRevC.40.2173
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1988HA07      Phys.Rev. C37, 1104 (1988)

D.Halderson, R.J.Philpott

Realistic Calculations for Strangeness Exchange at Rest

NUCLEAR REACTIONS 12C(K-, π-), E at rest; calculated K-capture rates.

doi: 10.1103/PhysRevC.37.1104
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1988HA35      Nucl.Phys. A487, 647 (1988)

D.Halderson

R-Matrix Theory for the Dirac Equation

NUCLEAR REACTIONS 12C(n, n), E not given; calculated phase shifts. Dirac R-matrix theory.

doi: 10.1016/0375-9474(88)90031-0
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1988HO11      Phys.Rev. C38, 1547 (1988)

A.Hotta, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, P.J.Ryan, R.P.Singhal, D.Halderson

Electroexcitation of 4He in the Near Continuum

NUCLEAR REACTIONS 4He(e, e'), E=130, 200 MeV; measured σ(E(e'), θ(e')). Shell model in continuum interpretation.

doi: 10.1103/PhysRevC.38.1547
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1988RO11      Ann.Phys.(New York) 184, 33 (1988)

A.S.Rosenthal, D.Halderson, K.Hodgkinson, F.Tabakin

Hypernuclear Photoproduction

NUCLEAR REACTIONS 1H(γ, K+), E at 1.2 GeV/c; calculated σ(θ). 12C(γ, K+), E=1.8 GeV; calculated σ(θ, E). 208Pb(γ, K+), E at 1.84 GeV/c; calculated σ(θ).

doi: 10.1016/0003-4916(88)90269-2
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1986BL07      Phys.Rev.Lett. 57, 543 (1986)

C.L.Blilie, D.Dehnhard, D.B.Holtkamp, S.J.Seestrom-Morris, S.K.Nanda, W.B.Cottingame, D.Halderson, C.L.Morris, C.F.Moore, P.A.Seidl, H.Ohnuma, K.Maeda

Measurement of Isospin Mixing in 4He and Its Implications for Charge-Symmetry Breaking

NUCLEAR REACTIONS 4He(π+, π+'), (π-, π-'), E=180 MeV; measured σ(E(π), θ(π)); deduced σ(π+)/σ(π-). 4He deduced very weak 1- state isospin mixing. DWIA analysis.

doi: 10.1103/PhysRevLett.57.543
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1986HA34      Phys.Rev.Lett. 57, 1117 (1986)

D.Halderson, Y.Mo, P.Ning

Comprehensive Calculations of the (π+, K+) Reaction on 12C

NUCLEAR REACTIONS 12C(π+, K+), E at 1054 MeV/c; calculated σ(θ, E(K+)); 12C(π+, π+), (K+, K+), E at 800 MeV/c; calculated σ(θ); deduced hypernuclear state configurations. DWIA, recoil corrected continuum shell model.

doi: 10.1103/PhysRevLett.57.1117
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1986HA39      Nucl.Phys. A458, 605 (1986)

D.Halderson, P.Ning, R.J.Philpott

Strangeness Exchange Reactions with the Recoil Corrected Continuum Shell Model

NUCLEAR REACTIONS 12C, 40Ca(K-, K-), (π-, π-), E at 800 MeV/c; 12C(K-, π-), E not given; calculated σ(θ). 16O(K-, π-), E at 790 MeV/c; 40Ca(K-, π-), E not given; calculated σ(θ(π), E(π)). Recoil corrected continuum shell model.

doi: 10.1016/0375-9474(86)90189-2
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1986RO25      Phys.Lett. 182B, 143 (1986)

A.S.Rosenthal, D.Halderson, F.Tabakin

Hypernuclear Photoproduction

NUCLEAR REACTIONS 12C, 208Pb(γ, K+), E=1.8 GeV/c; calculated hypernuclear excitation σ(θ); deduced spin-flip mode dominance, distortion effects. Full Coulomb, optical distortions, complete photoproduction vertex.

doi: 10.1016/0370-2693(86)91565-0
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1985JO02      Phys.Rev. C32, 103 (1985)

I.P.Johnstone, D.Halderson, J.A.Carr, F.Petrovich

Core Polarization in Inelastic Scattering to 52Cr(2+1)

NUCLEAR REACTIONS 52Cr(e, e'), E not given; calculated form factor. 52Cr(p, p'), E=40 MeV; calculated σ(θ). 52Cr(π+, π+'), (π-, π-'), E not given; calculated σ(θ), σ(θ(π), E(π)). 52Cr levels deduced σ(π+)-σ(π-) differences dependence on pion enhancement factors inclusion.

doi: 10.1103/PhysRevC.32.103
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1985NI03      J.Phys.(London) G11, 827 (1985)

P.Ning, D.Halderson

Microscopic Lane-Model Calculations

NUCLEAR REACTIONS 90,92,94Zr, 112,116,124Sn(p, n), E=25-80 MeV; calculated σ(θ) for IAS excitation. Microscopic Lane model.

doi: 10.1088/0305-4616/11/7/007
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1983CA05      Phys.Rev. C27, 1636 (1983)

J.A.Carr, F.Petrovich, D.Halderson, D.B.Holtkamp, W.B.Cottingame

Stretched Excitations and the Spin-dependent Part of the Pion-nucleon Interaction

NUCLEAR REACTIONS 28Si(π+, π+'), (π-, π-'), E=162 MeV; 16O(π+, π+'), (π-, π-'), E=164 MeV; calculated σ(θ). Impulse approximation, spin-orbit term, energy dependent t-matrix.

doi: 10.1103/PhysRevC.27.1636
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1983HA21      Phys.Rev. C28, 1000 (1983)

D.Halderson, R.J.Philpott

Charge Symmetry Breaking in 4He

NUCLEAR REACTIONS 4He(γ, p), (γ, n), E=20-36 MeV; calculated σ(ratio) vs E. 3H(p, n), (polarized p, n), E=1.5-4.5 MeV; calculated P(E), A(E). 3H(p, γ), E ≈ 2-16 MeV; calculated angular distribution, asymmetry coefficients a(k), (B(k)) vs E. 3He(n, γ), E=9 MeV; calculated σ(θ); deduced charge symmetry breaking interaction role inadequacy in interpreting data. Recoil-corrected continuum shell model.

doi: 10.1103/PhysRevC.28.1000
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1982PH01      Nucl.Phys. A375, 169 (1982)

R.J.Philpott, D.Halderson

Single-Particle Model of Capture to Continuum States

NUCLEAR REACTIONS 12C(p, p), E=26.2, 40, 61.4, 95 MeV; 11B(p, p), E=30.3 MeV; calculated σ(θ). 11B, 12C(p, γ), E=40 MeV; calculated σ(θ, Eγ). 11B(p, γ), (polarized p, γ), E=8-55 MeV; calculated σ(θ, Eγ), asymmetry vs E. Single particle model, continuum capture.

doi: 10.1016/0375-9474(82)90408-0
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1982TA05      Phys.Rev. C25, 1253 (1982)

S.L.Tabor, C.C.Chang, M.T.Collins, G.J.Wagner, J.R.Wu, D.W.Halderson, F.Petrovich

Survey of the (3He, t) Reaction: Excitation of the isobaric analog of the giant dipole resonance

NUCLEAR REACTIONS 12C, 16O, 27Al, 28Si, 40Ca, 46Ti, 90Zr(3He, t), (3He, 3He'), E=130, 170 MeV; measured σ(Et), σ(E(3He)), σ(θ). 16O, 27Al, 28Si, 40Ca, 46Ti, 90Zr deduced T=0, GQR. 12N, 16F, 27Si, 28P, 40Sc, 46V, 90Nb deduced IAS of T=1, GDR.

doi: 10.1103/PhysRevC.25.1253
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0078.


1982WR01      Phys.Rev. C25, 2823 (1982)

M.C.Wright, N.R.Roberson, H.R.Weller, D.R.Tilley, D.Halderson

Proton Capture in the 19 MeV Region of 12C

NUCLEAR REACTIONS 11B(p, γ), E=2.9-4.6 MeV; measured Eγ, Iγ, σ(θ) vs E. 12C transition deduced M1 quenching. Continuum shell model comparison.

doi: 10.1103/PhysRevC.25.2823
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1254.


1981HA01      Phys.Rev.Lett. 46, 100 (1981)

D.Halderson, R.J.Philpott

Radiative Capture to Unbound States via a Bremsstrahlung Mechanism

NUCLEAR REACTIONS 12C(p, γ), E=40 MeV; 11B(p, γ), E=40, 80 MeV; calculated σ(θγ, Eγ). 13N, 12C deduced resonances. Bremsstrahlung mechanism, capture to unbound states.

doi: 10.1103/PhysRevLett.46.100
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1981HA10      Nucl.Phys. A359, 365 (1981)

D.Halderson, R.J.Philpott

Radiative Capture to 4He

NUCLEAR REACTIONS 4He(γ, n), (γ, p), E not given; analyzed σ(θ); 3H(polarized p, γ), E=2-26 MeV; 3He(polarized n, γ), E=1-28 MeV; analyzed analyzing power vs θ. Continuum shell model, target recoil correction, noncentral forces.

doi: 10.1016/0375-9474(81)90242-6
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1981HA28      Phys.Rev. C24, 786 (1981)

D.Halderson, K.W.Kemper, J.D.Fox, R.O.Nelson, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell

Width of the 6-, T = 1, E(x) = 14.36 MeV State in 28Si and Its Relationship to Intermediate Energy Inelastic Scattering

NUCLEAR REACTIONS 27Al(p, p'), E=2.7-3.06 MeV; measured σ(Ep, θ). 28Si resonance deduced Γ. R-matrix analysis.

doi: 10.1103/PhysRevC.24.786
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1981HA29      Phys.Rev. C24, 1095 (1981)

D.Halderson, R.J.Philpott, J.A.Carr, F.Petrovich

Pion Inelastic Scattering to Particle Unbound Stretched States of 12C

NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=162 MeV; calculated σ(E(π), θ(π)). 12C levels deduced isospin mixing, Γ, Γn, Γp. Recoil corrected continuum shell model.

doi: 10.1103/PhysRevC.24.1095
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1980HA01      J.Phys.(London) G6, 59 (1980)

D.Halderson, B.Castel, G.Aizer

Non-Statistical Effects in Neutron Reactions on 32S

NUCLEAR REACTIONS 32S(n, γ), E ≈ 0-1.2 MeV; calculated cumulative Γn(E), Γγ, reduced n-width. Shell model in continuum.

doi: 10.1088/0305-4616/6/1/013
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1980HA35      Nucl.Phys. A345, 141 (1980)

D.Halderson, R.J.Philpott

Study of Nucleon Channel Reactions for A=12 and A=16 Systems with the Recoil Corrected Continuum Shell Model

NUCLEAR REACTIONS 11B(p, p), E=0.3-1 MeV; 11B(n, n), E=0.1-5 MeV; 11B(p, n), E=threshold-10 MeV; 15N(p, p), E=3-12 MeV; 15N(p, n), E=threshold-9 MeV; 15N(n, n), E=0.5-6 MeV; 15N(p, p'), E=8.5-11.5 MeV; calculated σ(θ, E). Continuum shell model, target recoil corrections, realistic interactions.

NUCLEAR STRUCTURE 12C, 12B, 16N, 16O; calculated levels. Continuum shell model, target recoil effects, realistic interactions.

doi: 10.1016/0375-9474(80)90415-7
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1979HA22      Nucl.Phys. A321, 295 (1979)

D.Halderson, R.J.Philpott

Recoil Corrected Continuum Shell Model Calculations for Four-Nucleon Systems

NUCLEAR REACTIONS 3H(p, p), (polarized p, p), E=4.15 MeV; 3He(n, n), (polarized n, n), E=8 MeV; calculated σ(θ), A(θ). Recoil-corrected continuum shell model in 1p-1h space.

doi: 10.1016/0375-9474(79)90127-1
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1979PH06      Phys.Rev.Lett. 43, 1785 (1979)

R.J.Philpott, D.Halderson

Prediction of Observable Polarization-Analyzing-Power Differences in 11B(p, n)11C

NUCLEAR REACTIONS 11B(p, n), E < 10 MeV; calculated polarization-analyzing power differences. Recoil corrected continuum 1p-1h shell model, realistic interactions.

doi: 10.1103/PhysRevLett.43.1785
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1979ST22      Phys.Rev. C20, 2114 (1979)

D.P.Stanley, D.Halderson

Coupled-Channels Calculation for Scattering and Capture of Alpha Particles Near the Giant Quadrupole Resonance

NUCLEAR REACTIONS 54Fe(α, α), (α, α'), E=8-17 MeV; calculated σ(E, θ). 58Ni(γ, α), E=7-15 MeV; calculated σ(E). Coupled channels method.

doi: 10.1103/PhysRevC.20.2114
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1978HA26      Nucl.Phys. A303, 359 (1978)

D.Halderson

The Giant Dipole Resonance in 55Co

NUCLEAR REACTIONS 54Fe(p, X), E=9-15 MeV; calculated σ(E, Eγ). 55Co GDR deduced T-splitting.

doi: 10.1016/0375-9474(78)90364-0
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1978HA32      Phys.Rev. C18, 1542 (1978)

D.Halderson, B.Castel

Neutron and Gamma Width Correlations in Neutron Capture Reactions: A Comparative Study

NUCLEAR REACTIONS 28Si(n, γ); calculated Γγ.

doi: 10.1103/PhysRevC.18.1542
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1977HA02      Phys.Rev. C15, 394 (1977)

D.W.Halderson, P.Goldhammer

Reaction Matrix Calculation of 4He with Three- and Four-Particle Correlations

NUCLEAR STRUCTURE 4He; calculated binding energy. Reid soft-core potential, Brueckner-bethe-Goldstone-Faddeev formalism.

doi: 10.1103/PhysRevC.15.394
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1977HA22      Ann.Phys.(New York) 103, 133 (1977)

D.Halderson, B.Castel, M.Divadeenam, H.W.Newson

s- and p-Wave Neutron Spectroscopy. Xf(ii). Intermediate Structure in the 28Si+n Reaction: Doorway State Calculation

NUCLEAR STRUCTURE 29Si; calculated low-lying structure. Doorway state calculation.

doi: 10.1016/0003-4916(77)90265-2
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1976HA05      Phys.Rev.Lett. 36, 760 (1976)

D.Halderson, B.Castel, I.P.Johnstone, M.Divadeenam

Neutron and Gamma Widths of a J = 3/2- Doorway State in 29Si

NUCLEAR STRUCTURE 29Si; calculated doorway resonances, widths.

doi: 10.1103/PhysRevLett.36.760
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1975CA25      Z.Phys. A274, 275 (1975)

B.Castel, D.Halderson, M.Micklinghoff, M.Divadeenam

Structure of Doorway States in the 40Ca + n Reaction

NUCLEAR STRUCTURE 41Ca; calculated S.

doi: 10.1007/BF01437740
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1975HA01      Phys.Rev. C11, 237 (1975)

D.W.Halderson, P.Goldhammer

Matrix Solution of the Bethe-Faddeev Equations

NUCLEAR STRUCTURE 3H; calculated binding energy.

doi: 10.1103/PhysRevC.11.237
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