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2017KA04      Phys.Rev. C 95, 014606 (2017)

C.Kalbach

Phenomenological model for light-projectile breakup

NUCLEAR REACTIONS ²⁷Al, Cu, Zr, Cd, Pt(d, p), E=14.8 MeV; ²⁷Al, Cu, Zr(d, xp), E=4-15 MeV; ²⁷Al, ¹¹⁸Sn, ²⁰⁹Bi(d, xp), E=10-60 MeV; ¹⁸¹Ta(d, xp), E=4-17 MeV; ⁶²Ni, ¹⁸¹Ta(d, p), E=15.0 MeV; ²⁷Al, ⁶²Ni, Nb, ¹¹⁹Sn, ¹⁸¹Ta(d, p), E=25.5 MeV; ⁵⁷Fe, ¹¹⁶Sn(d, p), E=27.5 MeV; ²⁷Al, ⁵⁸Ni, ⁹⁰Zr, ¹¹⁸Sn, ²⁰⁹Bi(d, p), E=56 MeV; ⁹⁰Zr, ²⁰⁸Pb, ²³²Th(d, p), E=70 MeV; ²⁷Al, ⁵⁸Ni(d, p), E=80 MeV; ⁹⁰Zr(³He, d), (³He, p), E=70, 90, 110 MeV; ²⁷Al, Co, Nb, ¹⁹⁷Au(³He, d), E=130 MeV; ⁹⁰Zr(³He, xd), E=20-110 MeV; ⁵⁹Co(³He, xd), E=20-120 MeV; ⁹⁰Zr(³He, xp), E=10-80 MeV; ¹⁹⁷Au(³He, xd), E=20-130 MeV; ²⁷Al, ⁵⁸Ni, ⁹⁰Zr(α, p), (α, d), E=80 MeV; ²⁷Al(α, t), (α, ³He), E=80 MeV; Bi(α, ³He), E=140 MeV; Al, ⁵⁸Ni, ⁹⁰Zr, Bi(α, p), (α, d), (α, t), (α, ³He), E=160 MeV; ⁹⁰Zr(α, xd), (α, xp), E=10-70 MeV; ⁵⁸Ni, ²⁰⁹Bi(α, xd), E=20-160 MeV; ²⁷Al, ⁵⁸Ni(α, xp), E=10-120 MeV; ²⁷Al(α, xt), E=20-160 MeV; ²⁷Al, ²⁰⁹Bi(α, x³He), E=50-160 MeV; analyzed systematics of experimental differential σ(θ, E) data from literature; deduced global systematics for differential σ(θ, E) for breakup mechanism of all charged-particle fragments, breakup can account for 50% to 60% of total reaction cross section; compared global model results with original data. Phenomenological model for breakup of d, ³He and α projectiles of 15-160 MeV energy, with one fragment emitted near projectile velocity in forward-angle cone.

doi: 10.1103/PhysRevC.95.014606
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2011OH05      J.Korean Phys.Soc. 59, 1817s (2011)

A.Ohrn, C.Gustavsson, M.Blann, V.Blideanu, J.Blomgren, S.Chiba, H.Duarte, F.Haddad, C.Kalbach, J.Klug, A.Koning, C.Le brun, C.Lebrun, F.R.Lecolley, X.Ledoux, N.Marie-noury, P.Mermod, L.Nilsson, M.Osterlund, S.Pomp, A.Prokofiev, U.Tippawan, Y.Watanabe

Measurements of Inelastic Neutron Scattering at 96 MeV from Carbon, Iron, Yttrium and Lead

NUCLEAR REACTIONS ¹²C, ⁵⁶Fe, ⁸⁹Y, ²⁰⁸Pb(n, n'x), E=96 MeV; measured En, In(θ) using SCANDAL (SCAttered Nucleon Detection AssembLy); deduced σ(E, θ), σ(θ); calculated σ(E, θ), σ(θ) using TALYS, QMD, PRECO. Compared with UCLA data at 65 MeV.

doi: 10.3938/jkps.59.1817
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2011VO06      Phys.Rev. C 83, 054605 (2011)

A.V.Voinov, S.M.Grimes, C.R.Brune, A.Burger, A.Gorgen, M.Guttormsen, A.C.Larsen, T.N.Massey, S.Siem, C.Kalbach

Equilibrium and pre-equilibrium processes in the ⁵⁵Mn(⁶Li, x p) and ⁵⁷Fe(α, x p) reactions

NUCLEAR REACTIONS ⁵⁵Mn(⁶Li, xp), (⁶Li, xn), E=15 MeV; ⁵⁷Fe(α, xp), E=30 MeV; measured neutron, proton and scattered α-particle spectra, cross sections, angular distributions. Comparison with calculations performed using the exciton pre-equilibrium model and Hauser-Feshbach evaporation model.

doi: 10.1103/PhysRevC.83.054605
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1841.

2006KA08      Phys.Rev. C 73, 024614 (2006)

C.Kalbach

Missing final states and the spectral endpoint in exciton model calculations

NUCLEAR REACTIONS ⁵³Cr, ⁵⁶Fe, ⁶⁰Ni, ⁶⁵Cu, ^94,95Mo(p, nX), E=25 MeV; ⁴⁸Ti, ⁵¹V, ⁵⁶Fe, ⁶³Cu, ⁸⁹Y, ⁹³Nb, ⁹⁶Mo, ¹¹⁵In(n, pX), E=14.8 MeV; ²⁷Al, ²⁸Si, ⁵⁹Co(n, nX), (n, pX), (n, dX), (n, tX), (n, αX), E ≈ 50 MeV; ²⁷Al, ^54,56Fe(n, nX), (n, pX), (n, dX), (n, tX), (n, ³HeX), (n, αX), E ≈ 62 MeV; ²⁷Al, ⁵⁸Ni(n, nX), (n, pX), (n, dX), (n, tX), (n, ³HeX), (n, αX), E=80 MeV; calculated σ(E). Exciton model, comparison with data.

doi: 10.1103/PhysRevC.73.024614
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2005KA11      Phys.Rev. C 71, 034606 (2005)

C.Kalbach

Preequilibrium reactions with complex particle channels

NUCLEAR REACTIONS ²⁷Al, ⁵⁴Fe, ⁵⁸Ni, ⁸⁹Y, ⁹⁰Zr, ¹²⁰Sn, ¹⁹⁷Au, ²⁰⁹Bi(p, pX), (p, dX), (p, tX), (p, ³HeX), (p, αX), E ≈ 29-90 MeV; ²⁷Al, ⁵⁸Ni, ⁶³Cu, ⁹⁰Zr, ²⁰⁸Pb(d, pX), (d, dX), (d, tX), (d, ³HeX), (d, αX), E ≈ 25-80 MeV; ⁶²Ni(³He, pX), (³He, dX), (³He, ³HeX), (³He, αX), E=24.3 MeV; ²⁷Al, ⁵⁴Fe, ⁵⁹Co, ⁶¹Ni, ⁶³Cu, ⁹⁰Zr, ¹⁰³Rh, ¹¹⁵In, ²⁰⁶Pb, ²³²Th(α, pX), (α, dX), (α, tX), (α, ³HeX), (α, αX), E ≈ 35-140 MeV; ²⁷Al, ²⁸Si, ⁵²Cr, ⁵⁹Co, ⁹³Nb, ²⁰⁹Bi, ²³⁸U(n, nX), (n, pX), (n, dX), (n, tX), (n, αX), E ≈ 14-63 MeV; calculated preequilibrium reactions particle spectra, σ(E); deduced reaction mechanism features. Comparison with data.

doi: 10.1103/PhysRevC.71.034606
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2005KA29      Phys.Rev. C 72, 024607 (2005)

C.Kalbach

Isospin conservation in preequilibrium reactions

NUCLEAR REACTIONS ⁵⁴Fe, ⁶⁰Ni, ⁹⁸Mo, ¹⁰⁶Pd, ¹⁵⁹Tb, ¹⁹⁷Au(p, pX), E=18-29 MeV; analyzed proton spectra, isospin conservation effects. ²⁷Al, ⁵⁸Ni(p, nX), (p, pX), (p, dX), (p, tX), (p, ³HeX), (p, tX), (p, αX), E=62, 90 MeV; ²⁸Si(n, nX), (n, pX), (n, dX), (n, tX), (n, ³HeX), (n, tX), (n, αX), E=50, 62.7 MeV; ²⁷Al, ⁵⁴Fe, ⁵⁸Ni(α, nX), (α, pX), (α, dX), (α, tX), (α, ³HeX), (α, tX), (α, αX), E=59, 140 MeV; analyzed En, Ep, light charged particle spectra, isospin conservation effects.

doi: 10.1103/PhysRevC.72.024607
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2004KA03      Phys.Rev. C 69, 014605 (2004)

C.Kalbach

Surface effects in preequilibrium reactions of incident neutrons

NUCLEAR REACTIONS ²⁸Si(n, pX), E=29, 39, 50 MeV; ²⁷Al, ²⁸Si, ⁵⁹Co, ²⁰⁹Bi, ²³⁸U(n, pX), E=28.5, 37.5, 49, 63 MeV; calculated angle-integrated σ(E); deduced surface localization effects. Exciton model, comparisons with data.

doi: 10.1103/PhysRevC.69.014605
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2000KA42      Phys.Rev. C62, 044608 (2000); Erratum Phys.Rev. C64, 039901 (2001)

C.Kalbach

Surface and Collective Effects in Preequilibrium Reactions

NUCLEAR REACTIONS ²⁴Mg, ²⁷Al, ²⁸Si, ⁴⁰Ca, ⁵⁵Mn, Ti, Fe, Cu, Zr, Mo, ¹¹⁵In, Sb, ¹⁸¹Ta, W, ¹⁸⁴W, Pb, ²⁰⁹Bi(n, xn), E ≈ 14-26 MeV; ⁵²Cr, ⁵⁶Fe, ⁶⁰Ni, ⁶⁵Cu, ^91,92,94Zr, ^92,94,95,96Mo, ¹⁰³Rh, ^{104,105,106,110}Pd, ^107,109Ag, ¹²⁰Sn, ¹⁶⁹Tm, ^{204,206,207,208}Pb(p, xn), E ≈ 18-26 MeV; ²⁷Al, ⁴⁶Ti, ⁵⁰Cr, ⁵⁴Fe, ⁶³Cu, ⁸⁹Y, ⁹³Nb, ⁹⁶Mo, ¹¹⁵In(n, xp), E ≈ 15 MeV; ⁹⁰Zr, ⁹³Nb, ^92,94Mo, ¹⁰³Rh, ^105,106Pd, Ag(p, xp), E ≈ 18 MeV; ⁵⁴Fe, ⁶⁰Ni, ⁹³Nb, ¹⁹⁷Au, ²⁰⁹Bi(p, p'), E ≈ 18-26 MeV; ⁵¹V, Fe, ⁵⁶Fe, Cu, ⁶⁵Cu, Ni, ²⁰⁹Bi(n, n'), E ≈ 18-26 MeV; ²⁷Al, ⁵⁸Ni, ⁹⁰Zr, ²⁰⁹Bi(p, p'), (p, n), E=90 MeV; calculated σ(E); deduced role of collective states, other reaction mechanism features. Exciton preequilibrium model, comparisons with data.

doi: 10.1103/PhysRevC.62.044608
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1999KA05      J.Phys.(London) G25, 75 (1999)

C.Kalbach

Toward a Global Exciton Model: The equilibrium component

NUCLEAR REACTIONS ²⁷Al, ^46,48Ti, ⁵⁰Cr, ⁵¹V, ^54,56Fe, ^63,65Cu, ⁸⁹Y, ⁹⁰Zr, ⁹³Nb, ^92,96Mo, ¹¹⁵In(n, xp), ⁹⁰Zr, ⁹³Nb, ^92,94,96Mo, ¹⁰³Rh, ^105,106Pd, Ag(p, xp), ²⁴Mg, ²⁷Al, ²⁸Si, ⁴⁰Ca, Ti, ⁵⁵Mn, Fe, Cu, Zr, Mo, ¹¹⁵In, Sb, ¹⁸¹Ta, W, Pb, ²⁰⁹Bi(n, xn), ⁵²Cr, ⁵⁶Fe, ⁶⁰Ni, ⁶⁵Cu, ^91,92,94Zr, ^92,94,95,96Mo, ¹⁰³Rh, ^{104,105,106,110}Pd, ^107,109Ag, ¹²⁰Sn, ^{204,206,207,208}Pb(p, xn), ⁵⁴Fe, ⁶⁰Ni, ²⁰⁹Bi, ¹⁹⁷Au(p, p'), ⁵¹V, ⁵⁶Fe, Fe, ⁶⁵Cu, Cu, Ni, ²⁰⁹Bi(n, n'), ⁹²Mo(n, p), ⁸⁹Y, ^116,118Sn(n, p), E ≈ 14-25 MeV; calculated proton spectra, neutron spectra; deduced state density shell correction effects. Comparison with data.

doi: 10.1088/0954-3899/25/1/008
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1998KA22      J.Phys.(London) G24, 847 (1998)

C.Kalbach

Toward a Global Exciton Model; Lessons at 14 MeV

NUCLEAR REACTIONS ²⁷Al, ⁴⁸Ti, ⁵⁰Cr, ⁵¹V, ^54,56Fe, ^63,65Cu, ⁸⁹Y, ⁹³Nb, ⁹⁶Mo, ¹¹⁵In(n, xp), ²⁴Mg, ²⁷Al, ²⁸Si, Ti, ⁵⁵Mn, Fe, ⁵⁹Co, Cu, Zr, ⁹³Nb, Mo, ¹¹⁵In, Sb, ¹⁸¹Ta, W, Pb, ²⁰⁹Bi(n, xn), ⁹²Mo(n, p), ⁸⁹Y, ^116,118Sn(p, n), Fe, ⁵⁹Co, ⁹³Nb(p, xp), E=14-15 MeV; analyzed σ(En), σ(Ep); deduced model parameters. Exciton model code PRECO-E.

doi: 10.1088/0954-3899/24/4/014
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1995KA50      J.Phys.(London) G21, 1499 (1995)

C.Kalbach

Shell-Corrected Particle-Hole State Densities for Pre-Equilibrium Reaction Calculations

NUCLEAR STRUCTURE ^208,210Pb, ¹¹⁷Sn; calculated shell-shifted equi-spacing model state densities. Comparison with realistic state densities.

doi: 10.1088/0954-3899/21/11/008
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1995KA51      J.Phys.(London) G21, 1519 (1995)

C.Kalbach

Consistent Exciton Model Calculations with Shell Structure, Pairing and Isospin Effects

NUCLEAR REACTIONS ⁹⁶Mo(p, n), E=25 MeV; ¹⁰⁰Mo(p, p'), E=18 MeV; ^90,91,92,94Zr(p, n), E=18, 25 MeV; ⁹⁰Zr(p, n), E=35, 45 MeV; ^{97,98,100,92,94,95,96}Mo(p, n), ⁸⁹Y(p, n), E=26 MeV; ⁹³Nb, ⁹⁰Zr(p, p'), E not given; ¹⁰³Rh, ^{104,105,106,108,110}Pd, ^107,109Ag(p, n), ¹⁰³Rh, ^105,106Pd, Ag(p, p'), E ≈ 18, 25 MeV; analyzed data. Consistent exciton model.

doi: 10.1088/0954-3899/21/11/009
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1993KA02      Phys.Rev. C47, 587 (1993)

C.Kalbach

Particle-Hole State Densities with Good Isospin

NUCLEAR STRUCTURE ⁵⁸Ni, ²⁰⁸Pb; calculated isospin-dependent state densities vs two exciton states excitation energy. A rederivation.

doi: 10.1103/PhysRevC.47.587
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1993KA20      Nucl.Sci.Eng. 115, 43 (1993)

C.Kalbach

Continuum Angular Distributions in the Transition Regions

NUCLEAR REACTIONS ⁹⁰Zr, ²⁰⁸Pb(p, n), E=120 MeV; ⁹⁰Zr(p, p'), E=120 MeV; ¹⁹⁷Au(p, p'), E=150 MeV; ⁵⁵Mn, ⁵⁶Fe, ⁵⁹Co, ⁶⁰Ni(n, α), E=14.1 MeV; ⁹⁰Zr, ^96,98,100Mo(p, α), E=18 MeV; ⁹³Nb(n, p), E=11.1, 14.1 MeV; ¹⁰³Rh(p, n), E=12.6, 18 MeV; ¹⁰⁷Ag(p, n), E=18.7, 25 MeV; ²⁰⁹Bi(n, n'), E=22.6, 25.7 MeV; ⁶³Cu(d, t), E=19.2, 24.7 MeV; ⁹³Nb(n, α), E=14.1, 14-18 MeV; calculated σ(θ) vs channel energy; deduced systematics.

doi: 10.13182/NSE93-A35521
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1990KA05      Phys.Rev. C41, 1656 (1990)

C.Kalbach

Phenomenology of Quasifree Scattering

NUCLEAR REACTIONS, MECPD, ICPND ²⁷Al, ^208,206Pb, ¹²C, ⁵⁸Ni, Be, Cu, U, Fe, Ge, ⁵¹V, ⁹⁰Zr, ⁴⁰Ca, W(p, p'), E=8-30 MeV; ⁹⁰Zr, ²⁰⁸Pb, Be, ²⁷Al, Ni, Ta, W, Pb, U, ⁵⁹Co, C(p, n), E=7.5-30 MeV; analyzed σ(E).

doi: 10.1103/PhysRevC.41.1656
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1988KA17      Phys.Rev. C37, 2350 (1988)

C.Kalbach

Systematics of Continuum Angular Distributions: Extensions to higher energies

NUCLEAR REACTIONS ⁵⁴Fe(p, p'), (p, t), ²⁷Al(p, α), (p, n), ⁵⁸Ni, ¹²⁰Sn(p, d), ⁹⁰Zr(p, p'), (p, α), ²⁰⁹Bi, ⁶⁴Ni(n, p), ²⁰⁹Bi(p, p'), E=60-90 MeV; ⁹³Nb(n, n'), E=257 MeV; ⁵⁴Fe(p, α), E=62 MeV; ¹⁰³Rh(α, p), E=42 MeV; ⁵⁸Ni(α, p), ²⁷Al(α, α'), E=100 MeV; ⁵⁸Ni(n, p), E=60 MeV; ⁵⁸Ni(p, n), ²⁰⁹Bi(p, α), E=90 MeV; ²³²Th(α, p), ⁹⁰Zr(α, α'), E=140 MeV; ⁵⁴Fe(α, d), (α, t), E=59 MeV; ⁶¹Ni(α, d), (α, t), E=35.5 MeV; ²⁰⁹Bi, ²⁷Al, ⁵⁹Co(p, p'), E=450 MeV; Fe, W(p, p'), E=558 MeV; ²⁷Al, Fe, W(p, d), E=558 MeV; ²⁷Al, ¹⁸¹Ta(p, p'), E=600 MeV; Fe, Pb(p, n), E=590 MeV; calculated double differential σ. Continuum reaction systematics.

doi: 10.1103/PhysRevC.37.2350
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1986KA04      Phys.Rev. C33, 818 (1986)

C.Kalbach

Two-Component Exciton Model: Basic formalism away from shell closures

NUCLEAR REACTIONS ⁵⁶Fe(n, n), (n, p), E=22 MeV; ⁵⁴Fe(p, p), (p, n), E=43.3, 66, 33.5 MeV; ⁵⁴Fe(p, p), (p, n), E=33.5 MeV; ¹⁰³Rh(p, p), (p, n), E=33.4 MeV; ¹⁶⁹Tm(p, p), (p, n), E=31.6 MeV; calculated preequilibrium energy spectra. ⁵⁴Fe(n, n'), E=22 MeV; ⁵⁴Fe(p, p'), (p, n), E=33.5 MeV; calculated σ(θ). One-, two-component exciton model.

doi: 10.1103/PhysRevC.33.818
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1985KA19      Phys.Rev. C32, 1157 (1985)

C.Kalbach

Surface Effects in the Exciton Model of Preequilibrium Nuclear Reactions

NUCLEAR REACTIONS ⁵⁶Fe, ⁸⁹Y, ¹⁹⁷Au(p, p'X), E=62 MeV; ²⁷Al, ⁵⁸Ni, ²⁰⁹Bi(p, nX), (p, p'X), E=90 MeV; ⁴⁸Ca, ⁹⁰Zr(p, nX), E=25, 35, 45 MeV; ²⁰⁸Pb(p, nX), E=35-45 MeV; ⁶⁴Zn(p, nX), E=26 MeV; ⁵⁴Fe(p, p'X), E=62 MeV; calculated continuum particle spectra. Exciton model, surface effects, preequilibrium processes.

doi: 10.1103/PhysRevC.32.1157
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1984KA34      Phys.Rev. C30, 1310 (1984)

C.Kalbach

Isospin Dependence of Two-Component Particle-Hole State Densities for Nuclei

NUCLEAR STRUCTURE ⁵⁸Ni, ²⁰⁸Pb; calculated isospin-dependent particle-hole states.

doi: 10.1103/PhysRevC.30.1310
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1981KA04      Phys.Rev. C23, 112 (1981)

C.Kalbach, F.M.Mann

Phenomenology of Continuum Angular Distributions. I. Systematics and parametrization

NUCLEAR REACTIONS ²⁷Al(d, p), ²⁷Al, ⁵⁸Ni(d, d'), (d, t), (d, α), E=80 MeV; ²⁰⁸Pb, ²³²Th(d, d'), ⁹⁰Zr, ²³²Th(d, t), ⁹⁰Zr, ²⁰⁸Pb(d, α), E=70 MeV; ¹²C(α, p), (α, α'), E=59 MeV; ⁵⁴Fe, ¹⁹⁷Au(p, p'), ⁵⁴Fe(p, d), (p, α), ¹⁹⁷Au(p, α), E=29 MeV; ¹²C, ²⁷Al, ¹⁹⁷Au, ²⁰⁹Bi(p, p'), ¹²C, ²⁷Al, ¹⁹⁷Au, ²⁰⁹Bi(p, α), E=62 MeV; analyzed σ(θ); deduced continuum particle emission systematics. Legendre polynomial analysis.

doi: 10.1103/PhysRevC.23.112
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1981KA25      Phys.Rev. C24, 819 (1981)

C.Kalbach

Bound and Unbound Particles in Griffin Model State Densities

NUCLEAR REACTIONS ⁵⁴Fe(p, p), E=4-36 MeV; calculated σ(Ep, θ). ⁵⁵Co deduced unbound particle-hole state densities. Griffin preequilibruim statistical model.

doi: 10.1103/PhysRevC.24.819
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1977KA23      Z.Phys. A283, 401 (1977)

C.Kalbach

The Griffin Model, Complex Particles and Direct Nuclear Reactions

NUCLEAR REACTIONS ⁵⁴Fe(p, p), E=29, 39, 62 MeV; ⁵⁴Fe(α, α), E=59 MeV; ¹²⁰Sn(p, p), E=62 MeV; ¹⁹⁷Au(p, p), E=29, 62 MeV; calculated σ.

doi: 10.1007/BF01409522
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1975KA30      Nuovo Cim. 29A, 283 (1975)

C.Kalbach

The Shell-Shifted Equi-Spacing Model for Particle-Hole State Densities

NUCLEAR STRUCTURE ¹¹⁵Pd, ¹¹⁵Cd, ¹¹⁵Sn, ¹¹⁵Te, ^206,208,210Pb; calculated multi-exciton state densities.

doi: 10.1007/BF02729757
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1975KA33      Z.Phys. A275, 175 (1975)

C.Kalbach, S.M.Grimes, C.Wong

Comparison of Proton and Neutron Spectra: The Extended Griffin Model, Pairing and Isospin

NUCLEAR REACTIONS ¹⁰³Rh, ¹⁵⁹Tb, ¹⁶⁹Tm(p, n), (p, p'), E=18 MeV; measured σ. Extended Griffin model, pairing, isospin.

doi: 10.1007/BF01409594
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1974BA76      Nucl.Phys. A234, 33 (1974)

R.Ballini, N.Cindro, J.P.Fouan, C.Kalbach, M.Lepareux, N.Saunier

Spectroscopy of the Continuum States of ²⁴Mg Using the ²⁰Ne(α, α') and ²³Na(p, α) Reactions

NUCLEAR REACTIONS ²⁰Ne(α, α'), E=10.25-14.82 MeV; ²³Na(p, α), E=8.2-9.5 MeV; measured σ(E, Eα, θ). ²⁴Mg deduced resonance energies. Enriched ²⁰Ne target. Natural Na target.

doi: 10.1016/0375-9474(74)90377-7
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1974BE41      Phys.Rev. C10, 1028 (1974)

F.E.Bertrand, R.W.Peelle, C.Kalbach-Cline

Differential Cross Sections for Charged-Particle Emission in Reactions Of 58-MeV α Particles with ¹²C, ¹⁶O, and ⁵⁴Fe: Comparison with the Exciton Model of Pre-Equilibrium Particle Emission

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁵⁴Fe(α, α'X), (α, tX), (α, dX), (α, pX), E=58 MeV; measured σ(Eα', Et, Ed, Ep, θ); deduced σ(E). Comparison with extended exciton model of preequilibrium particle emission.

doi: 10.1103/PhysRevC.10.1028
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0814.

1974KA10      Nucl.Phys. A222, 405 (1974)

C.Kalbach-Cline, J.R.Huizenga, H.K.Vonach

Isospin Conservation and Pre-Equilibrium Decay in (p, p') Reactions on Neutron Rich Tin Isotopes

NUCLEAR REACTIONS ^{112,118,120,124}Sn(p, p'), E=14.0, 17.8 MeV; measured σ(Ep', θ); enriched targets.

doi: 10.1016/0375-9474(74)90400-X
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1974LE13      Nucl.Phys. A223, 563 (1974)

P.M.S.Lesser, D.Cline, C.Kalbach-Cline, A.Bahnsen

Reorientation Measurements in the Even Nickel Isotopes

NUCLEAR REACTIONS ^58,60Ni(³²S, ³²S'γ), E=70 MeV; measured ³²S'γ(θ). ^58,60Ni levels deduced quadrupole moment.

doi: 10.1016/0375-9474(74)90706-4
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1973KA27      Nucl.Phys. A210, 590 (1973)

C.Kalbach-Cline

Residual Two-Body Matrix Elements for Pre-Equilibrium Calculations

NUCLEAR REACTIONS ⁵⁴Fe, ⁸⁹Y, ¹²⁰Sn, ¹⁹⁷Au, ²⁰⁹Bi(p, p), ⁵⁶Fe, ¹⁸¹Ta, ²⁰⁸Pb(p, n), ⁵⁴Fe, ⁵⁹Co, ⁵⁸Ni, ⁹³Nb, ¹²⁴Sn(α, p); calculated average effective two-body matrix element. ⁵⁵Co, ¹²¹Sb, ²¹⁰Po levels calculated T_1/2. ⁵⁴Fe(p, p), (α, p), ¹²⁰Sn(p, p); calculated σ.

doi: 10.1016/0375-9474(73)90296-0
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