NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = D.Halderson

Found 56 matches.

Back to query form

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 p_1/2 and p_3/2 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1999HA60      Phys.Rev. C60, 064001 (1999)

D.Halderson

Nijmegen Soft Core YN Potential with Bound State Restrictions

doi: 10.1103/PhysRevC.60.064001
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
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
Citations: PlumX Metrics
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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Note: The following list of authors and aliases matches the search parameter D.Halderson: , D.W.HALDERSON