NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = D.Halderson Found 56 matches. 2016GR09 Phys.Rev. C 94, 014617 (2016) 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
2013GR11 Phys.Rev. C 88, 027602 (2013) 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
2013HA17 Phys.Rev. C 88, 014610 (2013) 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
2012GR09 Phys.Rev. C 85, 054617 (2012) 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
2009GR12 Phys.Rev. C 80, 044607 (2009) 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
2008GR07 J.Phys.(London) G35, 055102 (2008) 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
2008HA07 Phys.Rev. C 77, 034304 (2008) 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
2007HA46 Phys.Rev. C 76, 047301 (2007) Λ-hypernuclei single-particle energies with the Nijmegen ESC04 baryon-baryon interaction
doi: 10.1103/PhysRevC.76.047301
2006HA09 Phys.Rev. C 73, 024612 (2006) 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
2005HA26 Int.J.Mod.Phys. E14, 171 (2005) 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
2004HA04 Phys.Rev. C 69, 014609 (2004) 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
2004HA45 Phys.Rev. C 70, 034607 (2004) 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
2004HA49 Phys.Rev. C 70, 041603 (2004) 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
2002HA36 Nucl.Phys. A707, 65 (2002) 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
2000HA12 Phys.Rev. C61, 034001 (2000) 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
1999HA60 Phys.Rev. C60, 064001 (1999) Nijmegen Soft Core YN Potential with Bound State Restrictions
doi: 10.1103/PhysRevC.60.064001
1997HA48 Phys.Rev. C56, 2688 (1997) 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
1996HA15 Phys.Rev. C53, 2978 (1996) 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
1994HA48 J.Phys.(London) G20, 1461 (1994) 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
1993HA15 Phys.Rev. C48, 581 (1993) 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
1992HA01 Phys.Rev. C45, 42 (1992) 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
1992ZH03 Phys.Rev. C45, 563 (1992) 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
1990HA36 Phys.Rev. C42, 2584 (1990) 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
1989HA02 Phys.Rev. C39, 336 (1989) 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
1989HA32 Phys.Rev. C40, 2173 (1989) 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
1988HA07 Phys.Rev. C37, 1104 (1988) 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
1988HA35 Nucl.Phys. A487, 647 (1988) 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
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
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
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
1986HA34 Phys.Rev.Lett. 57, 1117 (1986) 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
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
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
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
1985NI03 J.Phys.(London) G11, 827 (1985) 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
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
1983HA21 Phys.Rev. C28, 1000 (1983) 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
1982PH01 Nucl.Phys. A375, 169 (1982) 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
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
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
1981HA01 Phys.Rev.Lett. 46, 100 (1981) 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
1981HA10 Nucl.Phys. A359, 365 (1981) 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
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
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
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
1980HA35 Nucl.Phys. A345, 141 (1980) 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
1979HA22 Nucl.Phys. A321, 295 (1979) 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
1979PH06 Phys.Rev.Lett. 43, 1785 (1979) 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
1979ST22 Phys.Rev. C20, 2114 (1979) 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
1978HA26 Nucl.Phys. A303, 359 (1978) 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
1978HA32 Phys.Rev. C18, 1542 (1978) 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
1977HA02 Phys.Rev. C15, 394 (1977) 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
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
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
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
1975HA01 Phys.Rev. C11, 237 (1975) Matrix Solution of the Bethe-Faddeev Equations NUCLEAR STRUCTURE 3H; calculated binding energy.
doi: 10.1103/PhysRevC.11.237
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