NSR Query Results
Output year order : Descending NSR database version of May 21, 2024. Search: Author = C.Kalbach-Cline Found 29 matches. 2017KA04 Phys.Rev. C 95, 014606 (2017) 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
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
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
2006KA08 Phys.Rev. C 73, 024614 (2006) 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
2005KA11 Phys.Rev. C 71, 034606 (2005) 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
2005KA29 Phys.Rev. C 72, 024607 (2005) 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
2004KA03 Phys.Rev. C 69, 014605 (2004) 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
2000KA42 Phys.Rev. C62, 044608 (2000); Erratum Phys.Rev. C64, 039901 (2001) 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, 104,105,106,110Pd, 107,109Ag, 120Sn, 169Tm, 204,206,207,208Pb(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
1999KA05 J.Phys.(London) G25, 75 (1999) 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, 104,105,106,110Pd, 107,109Ag, 120Sn, 204,206,207,208Pb(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
1998KA22 J.Phys.(London) G24, 847 (1998) 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
1995KA50 J.Phys.(London) G21, 1499 (1995) 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
1995KA51 J.Phys.(London) G21, 1519 (1995) 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; 97,98,100,92,94,95,96Mo(p, n), 89Y(p, n), E=26 MeV; 93Nb, 90Zr(p, p'), E not given; 103Rh, 104,105,106,108,110Pd, 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
1993KA02 Phys.Rev. C47, 587 (1993) 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
1993KA20 Nucl.Sci.Eng. 115, 43 (1993) 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
1990KA05 Phys.Rev. C41, 1656 (1990) 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
1988KA17 Phys.Rev. C37, 2350 (1988) 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
1986KA04 Phys.Rev. C33, 818 (1986) 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
1985KA19 Phys.Rev. C32, 1157 (1985) 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
1984KA34 Phys.Rev. C30, 1310 (1984) 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
1981KA04 Phys.Rev. C23, 112 (1981) 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
1981KA25 Phys.Rev. C24, 819 (1981) 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
1977KA23 Z.Phys. A283, 401 (1977) 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
1975KA30 Nuovo Cim. 29A, 283 (1975) 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
1975KA33 Z.Phys. A275, 175 (1975) 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
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
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
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 112,118,120,124Sn(p, p'), E=14.0, 17.8 MeV; measured σ(Ep', θ); enriched targets.
doi: 10.1016/0375-9474(74)90400-X
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
1973KA27 Nucl.Phys. A210, 590 (1973) 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 T1/2. 54Fe(p, p), (α, p), 120Sn(p, p); calculated σ.
doi: 10.1016/0375-9474(73)90296-0
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