NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Blann Found 111 matches. Showing 1 to 100. [Next]2014KO20 Nucl.Data Sheets 118, 280 (2014) A.Yu.Konobeyev, U.Fischer, P.E.Pereslavtsev, M.Blann Improved Simulation of the Pre-equilibrium Triton Emission in Nuclear Reactions Induced by Nucleons NUCLEAR REACTIONS 27Al(p, t), E=61.7, 90 MeV;54Fe(p, t), E=61.5 MeV;58Ni(p, t), E=90 MeV;120Sn(p, t), E=28.8, 61.5 MeV;208Pb(p, t), E=62.9 MeV; calculated σ(Etriton) using Sato-Iwamoto-Harada model and direct pick-up. Compared with data.
doi: 10.1016/j.nds.2014.04.058
2011KO41 J.Korean Phys.Soc. 59, 935s (2011) A.Yu.Konobeyev, U.Fischer, P.E.Pereslavtsev, A.J.Koning, M.Blann Implementation of the Geometry Dependent Hybrid Model in TALYS NUCLEAR REACTIONS 56Fe(n, n'), E=14.1 MeV;90Zr(p, n), E=160 MeV; calculated σ(En); 56Fe(n, p), E=14.8 MeV; calculated σ(Ep); 58Ni(p, n), (p, p'), (p, d), E=90 MeV; calculated σ(En), σ(Ep), σ(E(deuteron)); 27Al(p, d), (p, α)E=61.7 MeV; calculated σ(Eα), σ(E(deuteron)); 209Bi(p, α), E=90 MeV; calculated σ(Eα). GDH (Geometry-Dependent Hybrid Model) implemented into TALYS code. Comparison with data, ALICE and ALICE/ASH codes.
doi: 10.3938/jkps.59.935
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
2000BL16 Phys.Rev. C62, 034604 (2000) Precompound Monte-Carlo Model for Cluster Induced Reactions NUCLEAR REACTIONS 93Nb(α, p), E < 50 MeV; 93Nb(α, 2n), (α, 3n), (α, 4n), E < 140 MeV; calculated σ. Precompound Monte-Carlo simulation model. Comparison with data.
doi: 10.1103/PhysRevC.62.034604
1998BL01 Phys.Rev. C57, 233 (1998) New Precompound Decay Model: Angular distributions NUCLEAR REACTIONS 90Zr(p, xn), E=45-256 MeV; 208Pb(p, xn), E=256 MeV; calculated σ(En, θ); 90Zr(p, xp), E=80, 160, 200 MeV; calculated σ(Ep, θ); deduced precompound decay features. Comparison with data.
doi: 10.1103/PhysRevC.57.233
1998TI12 Nucl.Instrum.Methods Phys.Res. A414, 73 (1998) Yu.E.Titarenko, O.V.Shvedov, M.M.Igumnov, S.G.Mashnik, E.I.Karpikhin, V.D.Kazaritsky, V.F.Batyaev, A.B.Koldobsky, V.M.Zhivun, A.N.Sosnin, R.E.Prael, M.B.Chadwick, T.A.Gabriel, M.Blann Experimental and Computer Simulation Study of the Radionuclides Produced in Thin 200Bi Targets by 130 MeV and 1.5 GeV Proton-Induced Reactions NUCLEAR REACTIONS 209Bi(p, X), E=130, 1500 MeV; measured Eγ, Iγ; deduced cumulative yields. Comparison with several simulation models.
doi: 10.1016/S0168-9002(98)00530-0
1997ME28 Nucl.Instrum.Methods Phys.Res. A398, 324 (1997) M.V.Mebel, A.S.Iljinov, C.Grandi, G.Reffo, M.Blann Analysis of Isotope Yields and Excitation Functions for Fissile and Non-Fissile Nuclei with CEF and HMS-ALICE Codes NUCLEAR REACTIONS 58,62Ni(p, X), E=80-1000 MeV; 209Bi, 232Th, 238U(p, X), E=150-1800 MeV; calculated fragments isotopic yields. Comparison of computer codes. Comparison with data.
doi: 10.1016/S0168-9002(97)00779-1
1997MU17 Phys.Scr. 56, 137 (1997) Yu.Murin, M.Blann, B.Jakobsson The Isotopic Effect as a Clock for Nuclear Fragmentation NUCLEAR REACTIONS 116,124Sn(α, X), E=50 MeV/nucleon; 112,124Sn(p, X), E=1 GeV; 112,124Sn(14N, X), E=32 MeV/nucleon; analyzed light fragment emission rates ratios data; deduced fragmentation time scale. Boltzmann master equation combined with statistical multi-fragmentation method.
doi: 10.1088/0031-8949/56/2/002
1996BL14 Acta Phys.Pol. B27, 587 (1996) XXIV Mazurian Lakes School of Nuclear Physics - Summary
1996BL16 Phys.Rev. C54, 1341 (1996) New Precompound Decay Model NUCLEAR REACTIONS, ICPND 90Zr(p, xn), E=25-250 MeV; calculated neutron spectra. 59Co(p, 3n), (p, 2np), (p, np), (p, 3np), (p, 5n3p), 51V(p, n), (p, 3np), E=threshold-200 MeV; calculated σ vs E. New precompound Monte Carlo simulation model.
doi: 10.1103/PhysRevC.54.1341
1996SC46 Nucl.Instrum.Methods Phys.Res. B114, 91 (1996) Th.Schiekel, F.Sudbrock, U.Herpers, M.Gloris, H.-J.Lange, I.Leya, R.Michel, B.Dittrich-Hannen, H.-A.Synal, M.Suter, P.W.Kubik, M.Blann, D.Filges Nuclide Production by Proton-Induced Reactions on Elements (6 ≤ Z ≤ 29) in the Energy Range from 200 MeV to 400 MeV NUCLEAR REACTIONS, ICPND C, N, O, Mg, 27Al, Si, Ca, Ti, Mn, Fe, Co, Ni, Cu(p, X), E=200-400 MeV; measured residuals production σ. Accelerator mass spectrometry, activation technique.
doi: 10.1016/0168-583X(96)00145-0
1995NA35 Nucl.Sci.Eng. 119, 97 (1995) P.Nagel, J.Rodens, M.Blann, H.Gruppelaar Intermediate Energy Nuclear Reaction Code Intercomparison: Applications to Transmutation of Long-Lived Reactor Wastes NUCLEAR REACTIONS 208Pb, 90Zr(p, xn), E=25-800 MeV; 90Zr(p, xp), E=80, 160 MeV; analyzed σ(θ, θ(nucleon)). Zr, Pb(p, xn), (p, xp), E < 1 GeV; analyzed nucleon multiplicities. Intercomparison of codes.
doi: 10.13182/NSE95-A24074
1994MU06 Phys.Rev. C49, 2602 (1994) M.G.Mustafa, M.Blann, G.Peilert, A.Botvina Comparison of Fast Cascade Plus Statistical Models for Heavy Ion Induced Multifragmentation Reactions NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; calculated neutron, proton kinetic energy, neutron multiplicity averaged up to time t. Fast cascade plus statistical models.
doi: 10.1103/PhysRevC.49.2602
1993BO15 Z.Phys. A345, 297 (1993) A.Botvina, I.N.Mishustin, M.Blann, M.G.Mustafa, G.Peilert, H.Stocker, W.Greiner Mechanisms of Fragment Production in Heavy-Ion Reactions at Intermediate Energies NUCLEAR STRUCTURE 100Ru; calculated total excitation energy, entropy per nucleon vs temperature, fragment charge yields. Three models of nuclear disintegration.
doi: 10.1007/BF01280837
1993KO53 Nucl.Instrum.Methods Phys.Res. B79, 297 (1993) J.E.Koster, R.O.Nelson, M.E.Schillaci, S.A.Wender, D.Mayo, F.P.Brady, J.Romero, D.Krofcheck, M.Blann, P.Anthony, V.R.Brown, L.Hansen, B.Pohl, T.C.Sangster, H.Nifenecker, J.A.Pinston Neutron-Proton Bremsstrahlung Experiments NUCLEAR REACTIONS 1H(n, γ), E=138-401 MeV; measured γ rays. Tof techniques.
doi: 10.1016/0168-583X(93)95348-9
1993MU10 Phys.Rev. C48, 588 (1993) M.G.Mustafa, M.Blann, A.V.Ignatyuk Realistic Level Densities in Fragment Emission at High Excitation Energies NUCLEAR STRUCTURE 100Ru; calculated fragment (Z ≤ 14) yields; deduced level density models dependence.
doi: 10.1103/PhysRevC.48.588
1993ST06 Phys.Rev. C47, 1647 (1993) S.Stamer, W.Scobel, W.B.Amian, R.C.Byrd, R.C.Haight, J.L.Ullmann, R.W.Bauer, M.Blann, B.A.Pohl, J.Bisplinghoff, R.Bonetti Double Differential Cross Sections for Neutron Emission Induced by 256 MeV and 800 MeV Protons NUCLEAR REACTIONS 7Li, 27Al, Zr, Pb(p, xn), E=256, 800 MeV; measured σ(θ, E); deduced reaction mechanism. Intranuclear cascade, statistical multi-step, hybrid models.
doi: 10.1103/PhysRevC.47.1647
1992MU01 Phys.Rev. C45, 1078 (1992) M.G.Mustafa, M.Blann, A.V.Ignatyuk, S.M.Grimes Nuclear Level Densities at High Excitations NUCLEAR STRUCTURE 20Ne, 40Ca, 100Ru; calculated level densities. Fermi gas formulas, thermodynamic methods, shell model single particle levels.
doi: 10.1103/PhysRevC.45.1078
1992PE08 Phys.Rev. C46, 1457 (1992) G.Peilert, J.Konopka, H.Stocker, W.Greiner, M.Blann, M.G.Mustafa Dynamical Treatment of Fermi Motion in a Microscopic Description of Heavy Ion Collisions NUCLEAR REACTIONS Zr, Pb, 27Al(p, xn), E=80-800 MeV; analyzed σ(θ, En). Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.46.1457
1991BL06 Phys.Rev. C44, 431 (1991) M.Blann, M.G.Mustafa, G.Peilert, H.Stocker, W.Greiner Expectations of Fragment Decay from Highly Excited Nuclei NUCLEAR STRUCTURE 100Ru; calculated primary, cluster yields for deexcitation cascade; deduced excitation energy dependence. Statistical model.
doi: 10.1103/PhysRevC.44.431
1991BL08 Phys.Rev. C44, R590 (1991) Multifragmentation for 36Ar + 238U Treated as Statistical Dynamic Interaction Processes NUCLEAR REACTIONS 238U(36Ar, X), E=35 MeV/nucleon; calculated exclusive multi-fragment multiplicities. Fast cascade, Boltzmann master equation.
doi: 10.1103/PhysRevC.44.R590
1990KA09 Nucl.Instrum.Methods Phys.Res. A288, 585 (1990) S.K.Kataria, V.S.Ramamurthy, M.Blann, T.T.Komoto Shell-Dependent Level Densities in Nuclear Reaction Codes NUCLEAR REACTIONS, ICPND 54Fe(α, p), (α, np), (α, n), (α, 2n), (α, xnyp), (α, 2np), (α, 3np), (α, 4np), (α, 3n), (α, 4n), E=threshold-70 MeV; calculated σ(E). Shell dependent level densities, exciton model.
doi: 10.1016/0168-9002(90)90155-Y
1990SC14 Phys.Rev. C41, 2010 (1990) W.Scobel, M.Trabandt, M.Blann, B.A.Pohl, B.R.Remington, R.C.Byrd, C.C.Foster, R.Bonetti, C.Chiesa, S.M.Grimes Preequilibrium (p, n) Reaction as a Probe for the Effective Nucleon-Nucleon Interaction in Multistep Direct Processes NUCLEAR REACTIONS 27Al, 90Zr, 208Pb(p, xn), E=120-160 MeV; measured σ(En, θ); deduced effective NN-interaction strength.
doi: 10.1103/PhysRevC.41.2010
1989BL08 Phys.Rev. C40, 2498 (1989) M.Blann, T.T.Komoto, I.Tserruya Equilibrium Cluster Emission from 3He + Ag Reactions NUCLEAR REACTIONS, ICPND Ag(3He, X), E=40-200 MeV; calculated isotopic yields vs mass number, σ(fragment θ, E), σ(E) for X=Li, Be, B, C, N, O, F, Ne. Hauser-Feshbach theory, hybrid preequilibrium decay model.
doi: 10.1103/PhysRevC.40.2498
1989GR04 Phys.Rev. C39, 1320 (1989) K.Grotowski, R.Planeta, M.Blann, T.Komoto Fission Barriers of Light Nuclei NUCLEAR REACTIONS, ICPND 40Ca(12C, F), E=74.3-186 MeV; 40Ca(9Be, F), E=141 MeV; 40Ca(6Li, F), E=153 MeV; 12C(32S, F), E=280 MeV; analyzed fission σ. 52Fe, 49Cr, 46V, 44Ti deduced fission barriers.
doi: 10.1103/PhysRevC.39.1320
1989TR01 Phys.Rev. C39, 452 (1989); Erratum Phys.Rev. C39, 2089 (1989) M.Trabandt, W.Scobel, M.Blann, B.A.Pohl, R.C.Byrd, C.C.Foster, R.Bonetti, S.M.Grimes Preequilibrium Neutron Emission in the Reactions 90Zr, 208Pb(p, xn) with 80 MeV Projectiles NUCLEAR REACTIONS 90Zr, 208Pb(p, xn), E=80 MeV; measured σ(E(n), θ(n)). Model calculations.
doi: 10.1103/PhysRevC.39.452
1988BL05 Nucl.Instrum.Methods Phys.Res. A265, 490 (1988) Calculation of γ-Ray Cascades in Code ALICE NUCLEAR REACTIONS 93Nb, 27Al, 197Au(n, xγ), E=9.5, 14, 18.5 MeV; 181Ta(n, xγ), E=14 MeV; calculated angle integrated σ(Eγ).
doi: 10.1016/S0168-9002(98)90018-3
1988RE05 Nucl.Instrum.Methods Phys.Res. A267, 408 (1988) G.Reffo, M.Blann, T.Komoto, R.J.Howerton Low Energy Neutron Capture of Neutron-Rich Target Nuclides NUCLEAR STRUCTURE A=80-160; calculated capture (n, γ) σ; deduced level density parameters.
doi: 10.1016/0168-9002(88)90483-4
1988RE11 Phys.Rev. C38, 1190 (1988); Erratum Phys.Rev. C39, 1188 (1989) G.Reffo, M.Blann, B.A.Remington Medium Energy γ Rays in Nuclear Reactions NUCLEAR REACTIONS 93Nb, 139La(n, γ), E=14.1 MeV; 154Sm(α, γ), 148Sm(3He, γ), E=27 MeV; calculated angle-integrated γ-spectra. Semi-direct reaction formalism.
doi: 10.1103/PhysRevC.38.1190
1988RE13 Phys.Rev. C38, 1746 (1988) B.A.Remington, M.Blann, A.Galonsky, L.Heilbronn, F.Deak, A.Kiss, Z.Seres Boltzmann Master Equation Analysis of Preequilibrium Neutron Emission from Heavy-Ion Collisions at 35 MeV/Nucleon NUCLEAR REACTIONS 165Ho(14N, xn), E=35 MeV/nucleon; analyzed data; deduced reaction mechanism. Boltzmann master equation model.
doi: 10.1103/PhysRevC.38.1746
1987BL08 Phys.Rev. C35, 1581 (1987) Precompound Decay in Heavy Ion Reactions via the Hybrid Model NUCLEAR REACTIONS 165Ho(20Ne, xn), E=220, 292 MeV; 165Ho(12C, xn), E=300 MeV; calculated neutron spectra. Hybrid model.
doi: 10.1103/PhysRevC.35.1581
1987BL09 Z.Phys. A326, 429 (1987) Numerical Test of Approximations in the Hybrid Precompound Decay Model NUCLEAR REACTIONS 93Nb(n, n'), (n, p), E=14.7, 45, 90 MeV; calculated angle integrated σ. Hybrid model.
1987RE03 Phys.Rev. C35, 1720 (1987) B.A.Remington, M.Blann, G.F.Bertsch n-p Bremsstrahlung Interpretation of High Energy Gamma Rays from Heavy-Ion Collisions NUCLEAR REACTIONS 1H(n, γ), E=130, 208 MeV; calculated σ(θn, θp). 1H(p, γ), E=140 MeV; 2H(p, γ), E=197 MeV; calculated σ. 2H, C, Pb(p, γ), E=140 MeV; 12C, Pb(14N, γX), 197Au(40Ar, γX), 12C, Ag(86Kr, γX), E=20-44 MeV/nucleon; 12C(12C, γX), E=48, 84 MeV/nucleon; calculated σ(Eγ, θγ), σ. 208Pb(14N, γX), E=30 MeV/nucleon; calculated γ-ray number vs time. Incoherent pnγ bremsstrahlung mechanism.
doi: 10.1103/PhysRevC.35.1720
1987RE11 Phys.Rev. C36, 1387 (1987) Angular Distributions of High Energy Gamma Rays from Heavy-Ion Collisions via an n-p Bremsstrahlung Interpretation NUCLEAR REACTIONS 12C, 2H(p, γ), E=140 MeV; calculated σ(θγ); deduced (n, p) bremsstrahlung mechanism dominance.
doi: 10.1103/PhysRevC.36.1387
1986BL14 Phys.Rev. C34, 2215 (1986) Observations on Rotating Finite-Range Fission Barriers Derived from Barriers for Nonrotating Nuclei NUCLEAR STRUCTURE 52Fe, 97Rh, 151Ho, 176Os; calculated fission barriers vs angular momentum. Rotating liquid drop model, finite range corrections.
doi: 10.1103/PhysRevC.34.2215
1986RE14 Phys.Rev.Lett. 57, 2909 (1986) B.A.Remington, M.Blann, G.F.Bertsch Intranuclear N - N Collision Model for the Production of High-Energy Gamma Rays in Heavy-Ion Collisions NUCLEAR REACTIONS C, Pb(14N, γX), E=20, 30, 40 MeV/nucleon; calculated σ(Eγ, θγ). Boltzmann master equation.
doi: 10.1103/PhysRevLett.57.2909
1985BL01 Phys.Rev. C31, 295 (1985) Precompound Limits of Linear Momentum Transfer in Heavy Ion Reactions NUCLEAR REACTIONS 60Ni(16O, X), E=8.8-100 MeV/nucleon; calculated projectile to residue linear momentum transfer. Boltzmann master equation.
doi: 10.1103/PhysRevC.31.295
1985BL07 Phys.Rev. C31, 1245 (1985) Precompound Decay Calculations for Reactions Induced by 10-100 MeV/Nucleon Heavy Ions NUCLEAR REACTIONS 165Ho(20Ne, nX), (20Ne, nF), E=220, 292, 402 MeV; calculated precompound neutron spectra, n(evaporation residue)-, fission fragment(n)-coin. 86Kr(27Al, X), E=10-100 MeV/nucleon; calculated precompound decay quantities. 60Ni(16O, X), E=0.141-2.027 GeV; calculated compound nuclear decay prior to equilibration. 90Zr(p, n), E=25, 45 MeV; calculated σ(θn, En). Boltzmann master equation model.
doi: 10.1103/PhysRevC.31.1245
1985BL09 Phys.Rev.Lett. 54, 2215 (1985) Subthreshold Pion Production: A intranuclear N-N collision interpretation NUCLEAR REACTIONS 27Al, 58Ni, 184W(14N, π0), E=35 MeV/nucleon; 12C(12C, π0), E=60, 74, 84 MeV/nucleon; calculated pion production σ.
doi: 10.1103/PhysRevLett.54.2215
1985BL12 Phys.Rev. C32, 411 (1985) M.Blann, S.M.Grimes, L.F.Hansen, T.T.Komoto, B.A.Pohl, W.Scobel, M.Trabandt, C.Wong Single-Particle Effects in Precompound Reactions: Influence of the f7/2 shell closure NUCLEAR REACTIONS 50,52,53Cr, 58Fe, 59Co, 60Ni, 63Cu(p, n), E=25 MeV; measured angle integrated neutron spectra; deduced precompound emission shell dependence.
doi: 10.1103/PhysRevC.32.411
1985BL17 Phys.Rev. C32, 1231 (1985) Subthreshold Pion Production NUCLEAR REACTIONS 27Al, 58Ni, 184W(14N, π0), E=MeV/nucleon; 12C, 58Ni, 238U(12C, π0), E=60, 74, 84 MeV/nucleon; 40Ca, 119Sn, 238U(40Ar, π0), E=44 MeV/nucleon; calculated σ(E(π)). Boltzmann master equation, heavy ion reaction equilibration.
doi: 10.1103/PhysRevC.32.1231
1985FA04 Phys.Rev.Lett. 55, 1376 (1985) M.Fatyga, K.Kwiatkowski, V.E.Viola, C.B.Chitwood, D.J.Fields, C.K.Gelbke, W.G.Lynch, J.Pochodzalla, M.B.Tsang, M.Blann Evolution of Nucleus-Nucleus Collision Mechanisms from the Barrier to beyond the Fermi Energy NUCLEAR REACTIONS 238U(14N, F), E=30-45 MeV/nucleon; 238U(12C, F), E=20-35 MeV/nucleon; 238U(6Li, F), E=30, 35 MeV/nucleon; measured fission (fragment)(fragment)-coin, σ(fragment θ) vs fragment-fragment θ(relative); deduced linear momentum transfer limitation, reaction mechanism.
doi: 10.1103/PhysRevLett.55.1376
1984BL06 Phys.Rev. C29, 1678 (1984) Precompound Evaporation Analyses of Excitation Functions for (α, xn) Reactions NUCLEAR REACTIONS, ICPND 181Ta(α, n), (α, 2n), (α, 3n), (α, 4n), E=threshold-65 MeV; 234,233U(α, n), (α, 2n), (α, 3n), E=threshold-45 MeV; 234U(α, 4n), E=40-45 MeV; 197Au(α, n), (α, 2n), (α, 3n), (α, 4n), E=threshold-80 MeV; 237Np, 235U(α, 4n), (α, 3n), (α, 2n), (α, n), E ≈ threshold-50 MeV; calculated σ(E). 237Np, 239Pu(3He, t), (3He, d), 240Pu(3He, t), E not given; calculated fission probability vs excitation energy. 239,238,237,235,234,233Pu, 241,240,239,238,237Am deduced fission barriers, neutron binding energy, barrier (a(F)/a(n)). Precompound evaporation model.
doi: 10.1103/PhysRevC.29.1678
1984BL15 Phys.Rev. C30, 1493 (1984) Precompound Nucleon Angular Distributions in the Continuum NUCLEAR REACTIONS 90Zr(p, n), E=25, 45, 90 MeV; 93Nb(n, xn), E=14.7, 25.7 MeV; 209Bi(n, xn), E=25.7 MeV; calculated σ(θn, En). 208Pb(p, n), E=45 MeV; calculated σ(θ). Fermi gas, nucleon-nucleon scattering kinematics, single kernel.
doi: 10.1103/PhysRevC.30.1493
1984SC33 Phys.Rev. C30, 1480 (1984) W.Scobel, M.Blann, T.T.Komoto, M.Trabandt, S.M.Grimes, L.F.Hansen, C.Wong, B.A.Pohl Single Particle Effects in Precompound Reactions NUCLEAR REACTIONS 50,52,53Cr, 54,56,58Fe, 59Co, 60Ni, 63Cu, 89Y, 90,91,92,94Zr, 92,94,96,97,98,100Mo, 110Pd, 159Tb(p, xn), E=25 MeV; 90,91,92,94Zr(p, xn), E=18 MeV; measured inclusive σ(En, θn); deduced precompound reaction single particle effects.
doi: 10.1103/PhysRevC.30.1480
1983BL09 Phys.Rev. C28, 1475 (1983) Global Test of Modified Precompound Decay Models NUCLEAR REACTIONS, ICPND 202Hg(p, 2p), (p, n2p), E=30-90 MeV; calculated σ(E). 27Al, 58Ni, 90Zr, 120Sn, 208Pb(p, X), E ≈ 10-100 MeV; 208Pb, 27Al(n, X), E ≈ 0.3-100 MeV; Ni(n, X), E ≈ 1-15 MeV; Sn(n, X), E ≈ 0.5-30 MeV; calculated reaction σ(E). 52Cr, 56Fe, 93Nb(n, xn), E=14.5 MeV; calculated σ vs En. 52Cr, 56Fe, 93Nb(n, p), E=14.7 MeV; calculated σ(Ep). 51V(p, n), E=18-26 MeV; 107,109Ag, 108,110Pd(p, n), E=18, 22, 25 MeV; 208Pb(p, n), E=35, 45 MeV; 120Sn, 48Ca(p, n), E=25, 35, 45 MeV; 27Al, 58Ni, 90Zr, 209Bi(p, n), E=90 MeV; calculated σ(En). 90Zr, 209Bi, 27Al, 58Ni(p, p'), E=90 MeV; 54Fe, 209Bi(p, p'), E=39, 62 MeV; calculated σ(Ep'); deduced best-fit model, parameter set. Hybrid, geometry dependent hybrid precompound decay models.
doi: 10.1103/PhysRevC.28.1475
1983BL10 Phys.Rev. C28, 1648 (1983) Precompound Analyses of Spectra and Yields following Nuclear Capture of Stopped π- NUCLEAR REACTIONS 58Ni, 27Al, 209Bi, 90Zr(p, p'), (p, n), E=90 MeV; calculated σ(Ep), σ(En). 62Ni(p, xnp), (p, xn2p), E=80, 100, 136, 164 MeV; 64Ni(p, xnp), (p, xn2p), E=100, 136 MeV; calculated product yields. 12C, Cu, 27Al, 16O, Pb, 181Ta, 197Au, 59Co(π-, xn), E at rest; calculated neutron spectra. 12C, 40Ca, 59Co(π-, xp), E at rest; calculated proton spectra.
doi: 10.1103/PhysRevC.28.1648
1983BL12 Phys.Rev. C28, 2286 (1983) M.Blann, B.L.Berman, T.T.Komoto Precompound-Model Analysis of Photonuclear Reactions NUCLEAR REACTIONS Sn, 140Ce, 181Ta, 208Pb(γ, xn), E ≈ 20-140 MeV; 16O(γ, xn), E ≈ 20-90 MeV; calculated σ(E); deduced photoneutron average multiplicities, widths. 181Ta, Pb, (π-, xn), E at rest; calculated average fast neutron, total neutron, fast proton multiplicities. Quasideuteron absorption mechanism, hybrid precompound-plus-evaporation model.
doi: 10.1103/PhysRevC.28.2286
1983CA19 Phys.Rev. C28, 1493 (1983) C.M.Castaneda, J.L.Ullmann, F.P.Brady, J.L.Romero, N.S.P.King, M.Blann Precompound Analyses of 58-64Ni(n, px) Reactions NUCLEAR REACTIONS 58,60,62,64Ni(n, pX), E=60 MeV; measured σ(θp), σ vs nucleon kinetic energy; deduced neutron number dependence, best fit model. Hybrid, geometry dependent hybrid models, neutron skin effect.
doi: 10.1103/PhysRevC.28.1493
1983SC19 Z.Phys. A311, 323 (1983) W.Scobel, L.F.Hansen, B.A.Pohl, C.Wong, M.Blann Double Differential Cross Sections for (p, xn) Reactions of 64Zn, 65Cu and 89Y with 26 MeV Protons NUCLEAR REACTIONS 64Zn, 65Cu, 89Y(p, xn), E=26 MeV; measured inclusive σ(θn, En). Tof. Preequilibrium, hybrid model analysis.
doi: 10.1007/BF01415688
1982BL12 Phys.Rev. C26, 465 (1982) Fusion-Excitation-Function Analyses with a Dynamic Model NUCLEAR REACTIONS, ICPND 62Ni(35Cl, X), E(cm)=60-180 MeV; 116Sn(35Cl, X), 141Pr(35Cl, X), E(cm)=120-240 MeV; 27Al(35Cl, X), (32S, X), 24Mg(32S, X), E(cm)=30-110 MeV; 109Ag(40Ar, X), E(cm)=100-260 MeV; 62Ni(58Ni, X), E(cm)=100-170 MeV; 27Al, 40Ca(16O, X), E(cm)=20-140 MeV; 65Cu(86Kr, X), E(cm)=130-310 MeV; 90Zr(86Kr, X), E(cm)=160-360 MeV; 165Ho, 209Bi(84Kr, X), E(cm)=250-500 MeV; calculated fusion σ vs E. Swiatecki dynamic model.
doi: 10.1103/PhysRevC.26.465
1982BL13 Phys.Rev. C26, 472 (1982) Statistical Fission Parameters for Nuclei at High Excitation and Angular Momenta NUCLEAR STRUCTURE 97Rh, 151Ho, 176Os; calculated fission barrier vs J. Rotating liquid drop model. NUCLEAR REACTIONS 62Ni, 116Sn, 141Pr(35Cl, X), (35Cl, F), E=150-290 MeV; 133Cs(20Ne, F), 141Pr(12C, F), E not given; calculated fission σ vs E. Rotating liquid drop model.
doi: 10.1103/PhysRevC.26.472
1982BL19 Phys.Rev. C26, 1471 (1982) M.Blann, D.Akers, T.A.Komoto, F.S.Dietrich, L.F.Hansen, J.G.Woodworth, W.Scobel, J.Bisplinghoff, B.Sikora, F.Plasil, R.L.Ferguson Saturation Analysis as a Test of Statistical Fission in Heavy Ion Reactions NUCLEAR REACTIONS 120,122Sn(56Fe, X), E=330-456 MeV; measured σ(evaporation residue θ), σ(fragment θ) vs mass; deduced statistical fission decay yield limit. 176Os deduced fission barrier vs J.
doi: 10.1103/PhysRevC.26.1471
1982SI01 Phys.Rev. C25, 686 (1982) B.Sikora, J.Bisplinghoff, M.Blann, W.Scobel, M.Beckerman, F.Plasil, R.L.Ferguson, J.Birkelund, W. Wilcke Parameter Scaling Test of a Dynamic Nucleus-Nucleus Collision Theory NUCLEAR REACTIONS, Fission 62Ni, 116Sn, 141Pr(35Cl, X), (35Cl, F), E=155-300 MeV; measured σ(evaporation residue), σ(fission) vs E. Dynamic model analysis.
doi: 10.1103/PhysRevC.25.686
1982SI04 Phys.Rev. C25, 885 (1982) B.Sikora, M.Blann, W.Scobel, J.Bisplinghoff, M.Beckerman Fusion Excitation Function of 58Ni + 62Ni at 215-275 MeV NUCLEAR REACTIONS 62Ni(58Ni, X), E=215-275 MeV; measured σ(evaporation residue) vs E; deduced fusion barrier, radius. Potential models.
doi: 10.1103/PhysRevC.25.885
1982SI05 Phys.Rev. C25, 1446 (1982) B.Sikora, W.Scobel, M.Beckerman, J.Bisplinghoff, M.Blann Measurement and Statistical Analyses of Fission and Fusion Excitation Functions for 35Cl on 62Ni, 116Sn, and 141Pr up to E(lab) = 215 MeV NUCLEAR REACTIONS, Fission 62Ni, 116Sn, 141Pr(35Cl, X), (35Cl, F), E=200, 215 MeV; measured σ(evaporation residue θ), σ(fragment θ); deduced statistical fission parameters. Statistical rotating liquid drop model.
doi: 10.1103/PhysRevC.25.1446
1981BL01 Phys.Rev. C23, 205 (1981) Precompound Decay in Heavy-Ion Reactions NUCLEAR REACTIONS 109Ag(40Ar, X), E=240, 320 MeV; 197Au(16O, X), E=214, 320 MeV; calculated σ(Ep), σ(En). Precompound model, coaelescence plus equilibration, Boltzmann equation.
doi: 10.1103/PhysRevC.23.205
1980BL04 Phys.Rev. C21, 1770 (1980) Decay of Deformed and Superdeformed Nuclei Formed in Heavy Ion Reactions NUCLEAR REACTIONS 109Ag(40Ar, X), E=236 MeV; 40Ca(16O, X), E=214 MeV; calculated transmission coefficients for spherical, deformed, superdeformed nuclei. 149Tb, 56Ni deduced fraction of α decay vs spin, α, n, p branching ratios, superdeformation effects. Rotating liquid drop model, Hauser-Feshbach calculation.
doi: 10.1103/PhysRevC.21.1770
1980SI04 Phys.Rev. C21, 614 (1980) B.Sikora, M.Blann, W.Scobel, J.Bisplinghoff, M.Beckerman Comparisons of Experimental and Theoretical Nucleus-Nucleus Potentials for Heavy-Ion Reactions NUCLEAR REACTIONS 24Mg, 27Al, 40Ca(32S, X), E=67-132 MeV; 27Al, 58,62,64Ni, 90Zr, 116Sn(35Cl, X), E=70-170 MeV; 116Sn, 141Pr(35Cl, X), E=135-170 MeV; analyzed fusion σ(E); deduced fusion barriers, radii. Proximity potential, Yukawa-plus-exponential model, modified Woods-Saxon potential.
doi: 10.1103/PhysRevC.21.614
1979BL01 Phys.Rev. C19, 1288 (1979) M.Blann, R.H.Stokes, B.Erkkila, H.C.Britt, P.D.Goldstone, R.L.Ferguson, F.Plasil, H.H.Gutbrod Final and Primary Yields and Dispersions for Strongly Damped Reaction Of 86Kr + 124Sn NUCLEAR REACTIONS 124Sn(86Kr, X), E=440, 720 MeV; measured distributions of fragment energy, mass vs atomic number; deduced primary distribution.
doi: 10.1103/PhysRevC.19.1288
1979BL09 Phys.Lett. 88B, 5 (1979) Alpha Decay Amplification in Superdeformed Nuclei: An Important New Mechanism of Nuclear de-Excitation at High Angular Momenta NUCLEAR REACTIONS 109Ag(40Ar, α), E=169-337 MeV; calculated transmission coefficients for n, p, α. 149Tb deduced decay probabilities for n, p, α, fission channels, evidence for superdeformation. Statistical model for deformed nuclei.
doi: 10.1016/0370-2693(79)90100-X
1979SI20 Phys.Rev. C20, 2219 (1979) B.Sikora, J.Bisplinghoff, W.Scobel, M.Beckerman, M.Blann Fusion of 58,60,62Ni with 113-170 MeV 40Ca Ions NUCLEAR REACTIONS 62,58Ni(40Ca, X), E=113-170 MeV; measured evaporation residue σ(E).
doi: 10.1103/PhysRevC.20.2219
1978BI01 Phys.Rev. C17, 177 (1978) J.Bisplinghoff, P.David, M.Blann, W.Scobel, T.Mayer-Kuckuk, J.Ernst, A.Mignerey 35Cl-Induced Fission and Fissionlike Reactions on 58,62Ni, 112,116,120,124Sn, and 141Pr NUCLEAR REACTIONS 58,62Ni, 112,116,120,124Sn, 141Pr(35Cl, F), E=155-170 MeV; measured σ(E, Z, θ); deduced total fission σ. Gas proportional/solid state counter telescopes.
doi: 10.1103/PhysRevC.17.177
1978PL02 Phys.Rev.Lett. 40, 1164 (1978) F.Plasil, R.L.Ferguson, H.C.Britt, R.H.Stokes, B.H.Erkkila, P.D.Goldstone, M.Blann, H.H.Gutbrod Measurement of the Energy Division Versus Mass in Highly Damped Reactions NUCLEAR REACTIONS 124Sn(86Kr, X), E=440, 720 MeV; measured σ(A, Z).
doi: 10.1103/PhysRevLett.40.1164
1978SC03 Z.Phys. A284, 343 (1978) W.Scobel, J.Bisplinghoff, M.Blann, A.Mignerey, P.David, J.Ernst, T.Mayer-Kuckuk Elastic Scattering of 35Cl from 27Al, 58,62Ni, 116,120,124Sn and 141Pr NUCLEAR REACTIONS 27Al, 58,62Ni, 116,120,124Sn, 141Pr(35Cl, 35Cl), E=100-170 MeV; measured σ(E, θ); deduced optical model parameters, interaction radii.
doi: 10.1007/BF01406807
1978ZO01 Nucl.Phys. A297, 163 (1978) Collective Potential-Energy Surfaces in Heavy-Ion Reactions NUCLEAR REACTIONS 109Ag(40Ar, 40Ar), 65Cu, 209Bi(84Kr, 84Kr), 209Bi(136Xe, 136Xe); calculated potential.
doi: 10.1016/0375-9474(78)90204-X
1977BE01 Phys.Rev.Lett. 38, 272 (1977) Fission Barriers at High Angular Momenta NUCLEAR REACTIONS 109Ag(40Ar, F), (40Ar, X), E=170-340 MeV; analyzed σ(E).
doi: 10.1103/PhysRevLett.38.272
1977BE21 Phys.Lett. 68B, 31 (1977) Mass Dependence of Statistical Fission Parameters NUCLEAR REACTIONS 62Ni, 116Sn, 141Pr(35Cl, F), E(cm)=155-170 MeV; 107Ag(20Ne, F), E(cm)=118-166 MeV; 109Ag(40Ar, F), E(cm)=169-337 MeV; calculated fission σ.
doi: 10.1016/0370-2693(77)90027-2
1977BI06 Phys.Rev. C16, 1058 (1977) J.Bisplinghoff, A.Mignerey, M.Blann, P.David, W.Scobel Statistical Analysis of Heavy-Ion-Induced Fission Excitation Functions NUCLEAR REACTIONS 62Ni, 116Sn, 141Pr(35Cl, F), E=155-170 MeV; calculated σ(E). Statistical model.
doi: 10.1103/PhysRevC.16.1058
1977BR30 Phys.Rev.Lett. 39, 1458 (1977) H.C.Britt, B.H.Erkkila, P.D.Goldstone, R.H.Stokes, B.B.Back, F.Folkmann, O.Christensen, B.Fernandez, J.D.Garrett, G.B.Hagemann, B.Herskind, D.L.Hillis, F.Plasil, R.L.Ferguson, M.Blann, H.H.Gutbrod Angular Momentum Limits in Fusion Reactions Induced by Argon and Krypton Projectiles NUCLEAR REACTIONS 122,124Sn(40Ar, X), 76Ge(86Kr, X); measured γ-multiplicity. 70,74Ge(86Kr, X); measured σ(A, Z).
doi: 10.1103/PhysRevLett.39.1458
1977DA14 Nucl.Phys. A287, 179 (1977) P.David, J.Bisplinghoff, M.Blann, T.Mayer-Kuckuk, A.Mignerey Evaporation Residue Excitation Functions for 35Cl Induced Reactions of 112,120Sn and 141Pr NUCLEAR REACTIONS 112,120Sn, 141Pr(35Cl, X), E=135-170 MeV; measured evaporation residue cross sections, fission cross sections; deduced complete fusion cross sections σcf(E), fusion radii, fusion barriers. Enriched targets. Gas-proportional-solid-state detector telescopes.
doi: 10.1016/0375-9474(77)90570-X
1977GI07 Phys.Lett. 68B, 405 (1977) Influence of Nucleon Mean-Free Paths on Intranuclear Cascade Results NUCLEAR REACTIONS 54Fe, 89Y(p, p'), E=62 MeV; calculated σ.
doi: 10.1016/0370-2693(77)90453-1
1977SC23 Nucl.Phys. A287, 301 (1977) A Quasi-Free Scattering Preequilibrium Model for (N, α) Reactions NUCLEAR REACTIONS 54Fe(p, α), E=29, 39, 62 MeV; 56Fe, 89Y, 197Au(p, α), E=62 MeV; 57Fe(p, α), E=32 MeV; 59Co(p, α), E=48 MeV; 66Zn, 118Sn(p, α), E=50.5 MeV; 120Sn(p, α), E=29, 62 MeV; 209Bi(p, α), E=39, 43, 62 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(77)90498-5
1976BL02 Nucl.Phys. A257, 15 (1976) M.Blann, R.R.Doering, A.Galonsky, D.M.Patterson, F.E.Serr Preequilibrium Analysis of (p, n) Spectra on Various Targets at Proton Energies of 25 to 45 MeV NUCLEAR REACTIONS 48Ca, 90Zr, 120Sn(p, n), E=25, 35, 45 MeV; 208Pb(p, n), E=35, 45 MeV; measured σ(En, θ). Enriched targets.
doi: 10.1016/0375-9474(76)90471-1
1976BR10 Phys.Rev. C13, 1483 (1976) H.C.Britt, B.H.Erkkila, R.H.Stokes, H.H.Gutbrod, F.Plasil, R.L.Ferguson, M.Blann Argon- and Krypton-Induced Reactions at Energies of 4-7 MeV/amu NUCLEAR REACTIONS 109Ag(40Ar, X), E=169-337 MeV; 121Sb(40Ar, X), E=282, 340 MeV; 65Cu(84Kr, X), E=494, 604 MeV; measured elastic scattering, evaporation residue, fission, fusion σ.
doi: 10.1103/PhysRevC.13.1483
1976MI20 Nucl.Phys. A273, 125 (1976) A Quasi-Free Scattering Model for Reactions Involving Clusters NUCLEAR REACTIONS 54Fe, 209Bi(p, p'), E=39, 62 MeV; 51V, 56Fe, 59Co, 63Cu, 93Nb, 115In, 181Ta, 206Pb(α, α'), E=55 MeV; 61Ni(α, α'), (α, p), E=35 MeV; 54Fe(α, α'), (α, p), E=55 MeV; 197Au(α, α'), E=42, 50, 65, 90 MeV; 181Ta(α, α'), E=55, 65 MeV; calculated σ. Quasi-free scattering model.
doi: 10.1016/0375-9474(76)90304-3
1976SC29 Phys.Rev. C14, 1808 (1976) W.Scobel, H.H.Gutbrod, M.Blann, A.Mignerey Fusion and Interaction Barrier Parameters and Critical Angular Momenta From 35Cl-Induced Reactions NUCLEAR REACTIONS 27Al, 48Ti, 54,56Fe, 58,60,62,64Ni, 90Zr, 116,124Sn(35Cl, 35Cl), (35Cl, F), (35Cl, X), E=70-170 MeV; measured σ(E, θ), complete fusion σ; deduced fusion barrier heights, radii, critical angular momenta.
doi: 10.1103/PhysRevC.14.1808
1975HI08 Nucl.Phys. A252, 496 (1975) M.Hille, P.Hille, H.H.Gutbrod, M.Blann Activation Cross Sections for Reactions of 109Ag Induced with 40Ar Ions NUCLEAR REACTIONS 109Ag(40Ar, X), E=228, 288 MeV; measured σ. Enriched target.
doi: 10.1016/0375-9474(75)90515-1
1975SC10 Phys.Rev. C11, 1701 (1975) W.Scobel, A.Mignerey, M.Blann, H.H.Gutbrod Barrier Penetrability and/or Deformation Effects in 35Cl Induced Fusion on 58,60,62,64Ni NUCLEAR REACTIONS 58,60,62,64Ni(35Cl, X), E=91-170 MeV; measured σ(E, E(fragment mass), θ) for evaporation residues, complete fusion σ.
doi: 10.1103/PhysRevC.11.1701
1974BL04 Nukleonika 19, 183 (1974) A-Priori Pre-Equilibrium Decay Models NUCLEAR REACTIONS 54Fe, 209Bi(p, p'), E=39, 62 MeV; calculated σ(Ep').
1974BL09 Nucl.Phys. A235, 211 (1974) On the Possible Role of Precompound Decay in Heavy Ion Reactions NUCLEAR REACTIONS 141Pr(12C, 4n), E=100, 200 MeV; calculated σ, precompound decay.
doi: 10.1016/0375-9474(74)90188-2
1974FL09 Phys.Rev. C10, 1350 (1974) D.G.Fleming, A.Arima, H.W.Fulbright, M.Blann 18O(p, t)16O Reaction and the Coexistence Model of 16O NUCLEAR REACTIONS 18O(p, t), E=20 MeV; measured σ(Et, θ). 16O deduced levels, J, π, L.
doi: 10.1103/PhysRevC.10.1350
1973AL17 Phys.Rev. C8, 1481 (1973) Realistic Partial State Densities for Proton-Neutron Configurations in Nuclei Near Closed Shells NUCLEAR STRUCTURE 115Pd, 115Cd, 115Sn, 115Te, 206,208,210Pb; calculated partial state densities.
doi: 10.1103/PhysRevC.8.1481
1973BL09 Nucl.Phys. A213, 570 (1973) A Priori Pre-Equilibrium Decay Models NUCLEAR REACTIONS 54Fe, 209Bi(p, p'), E=39, 62 MeV; calculated σ(Ep').
doi: 10.1016/0375-9474(73)90753-7
1973GU07 Phys.Rev.Lett. 30, 1259 (1973) H.H.Gutbrod, W.G.Winn, M.Blann Fusion Barriers in Heavy-Ion Reactions NUCLEAR REACTIONS 24Mg, 27Al, 40Ca, 58Ni(32S, X), E=68-110 MeV; measured σ(E) for fusion reaction.
doi: 10.1103/PhysRevLett.30.1259
1973GU15 Nucl.Phys. A213, 267 (1973) H.H.Gutbrod, W.G.Winn, M.Blann Measurement and Interpretation of Heavy Ion Fusion Excitation Functions NUCLEAR REACTIONS 24Mg, 27Al, 40Ca, 58Ni(32S, X), E=67-132 MeV; measured σ(E, θ), σ(fusion); deduced fusion barrier heights, radii.
doi: 10.1016/0375-9474(73)90149-8
1973GU16 Nucl.Phys. A213, 285 (1973) H.H.Gutbrod, M.Blann, W.G.Winn Elastic Scattering of 32S on 24Mg, 27Al and 40Ca and the Effect of Nuclear Forces on the Grazing Collision NUCLEAR REACTIONS 24Mg, 27Al, 40Ca(32S, 32S), E=67-120 MeV; measured σ(θ); compared with optical model, search parameters found, contact radii extracted.
doi: 10.1016/0375-9474(73)90150-4
1972BL03 Phys.Rev.Lett. 28, 757 (1972) Importance of the Nuclear Density Distribution on Pre-Equilibrium Decay NUCLEAR REACTIONS 54Fe(p, p'), E=29, 39, 62 MeV; calculated σ(Ep'); analyzed nuclear density distribution effects on pre-equilibrium decay.
doi: 10.1103/PhysRevLett.28.757
1972BL06 Nucl.Phys. A186, 245 (1972) Pre-Equilibrium Decay at Moderate Excitations and the Hybrid Model NUCLEAR REACTIONS 59Co, 58Ni, 60Ni, 63Cu, 65Cu, 93Nb, 103Rh, 106Pd, 195Pt(α, p), E = 42 MeV; 54Fe(α, p), E=59 MeV; 181Ta(p, n), E=18 MeV; 197Au(p, p'), E=62 MeV; calculated σ(Ep), σ(En), σ(Ep'). Pre-equilibrium decay, hybrid model.
doi: 10.1016/0375-9474(72)90043-7
1972BL09 Phys.Rev.Lett. 29, 303 (1972) Limits on Angular Momentum in Heavy-Ion Compound-Nucleus Reactions
doi: 10.1103/PhysRevLett.29.303
1972WI14 Nucl.Phys. A188, 423 (1972) W.G.Winn, H.H.Gutbrod, M.Blann Predicted Limits for Production of New Proton-Rich Nuclei by a Heavy-Ion Compound-Nucleus Mechanism
doi: 10.1016/0375-9474(72)90067-X
1971BL08 Phys.Rev.Lett. 27, 337 (1971) Hybrid Model for Pre-Equilibrium Decay in Nuclear Reactions NUCLEAR REACTIONS 93Nb(α, p), E=30.5, 42 MeV; calculated σ, pre-equilibrium particle emission.
doi: 10.1103/PhysRevLett.27.337
1971CL10 Nucl.Phys. A172, 225 (1971) The Pre-Equilibrium Statistical Model: Description of the Nuclear Equilibration Process and Parameterization of the Model NUCLEAR REACTIONS Pt, 63Cu, 58Ni, 93Nb, 59Co, 62Ni, 65Cu, 103Rh, 106Pd(α, p), E approx 40, 42 MeV; 56Fe, 181Ta(p, n), E=24, 25 MeV;93Nb(α, n), E=43 MeV; calculated σ(Ep), σ(En), σ(En). Pre-equilibrium statistical model.
doi: 10.1016/0375-9474(71)90713-5
1971DO01 Nucl.Phys. A161, 12 (1971) Decay Scheme Studies of Short-Lived Isotopes of 69 < A < 88 Produced by Heavy-Ion Bombardment RADIOACTIVITY 69As, 72Br, 81Sr, 84Y, 85Zr, 87Nb, 88g,88mNb, 88Mo [from HI-induced reactions]; measured T1/2, Eγ, Iγ. 71Se, 77mKr, 78mRb, 83mY[from HI-induced reactions]; measured T1/2, Eγ. 69Ge deduced levels. 72Se, 81Rb, 84Sr, 88Zr deduced levels, J, π. Ge(Li) detector.
doi: 10.1016/0375-9474(71)90318-6
1971DO07 Nucl.Phys. A167, 247 (1971) Decay of 104Cd and Levels of 104Ag RADIOACTIVITY 104Cd[from 106Cd(p, p2n), 107Ag(p, 4n), 104Pd(3He, 3n)]; measured Eγ, Iγ. 104Ag deduced levels. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(71)90073-X
1971DO08 Nucl.Phys. A167, 577 (1971) The Decay of 96,96mRh and Levels of 96Ru RADIOACTIVITY 96,96mRh[from 96Ru(p, n)]; measured T1/2, Eγ, Iγ. 96Ru(α, α')E=18.000 MeV. Enriched target. 96Ru levels deduced J, π.
doi: 10.1016/0375-9474(71)90064-9
1971DO10 Nucl.Phys. A171, 273 (1971) The Decay of 104,104mAg, 104,104mRh and Levels of 104Pd RADIOACTIVITY 104,104mAg[from 106Cd(p, 2pn), 107Ag(p, p3n), 104Pd(p, n), 103Rh(3He, 2n)]; measured Eγ, Iγ. 104,104mRh[from 103Rh(d, p)]; measured Eγ, Iγ. 104Pd deduced levels, J, π, γ-branching. Ge(Li) detector. 104Pd(p, p'), Ep=12.000 MeV; measured σ(Ep). 104Pd deduced levels.
doi: 10.1016/0375-9474(71)90023-6
1971FL05 Nucl.Phys. A163, 401 (1971) D.G.Fleming, M.Blann, H.W.Fulbright Blocking Observed in (p, t) Reactions on the Odd Tin Isotopes NUCLEAR REACTIONS 115,117,119Sn(p, t), E=20 MeV; measured σ(Et, θ); observed blocking effect of Pauli exclusion principle. 115Sn deduced level, J, π. 113,115,117Sn levels deduced L.
doi: 10.1016/0375-9474(71)90497-0
1970FL08 Nucl.Phys. A157, 1 (1970) D.G.Fleming, M.Blann, H.W.Fulbright, J.A.Robbins (p, t) Reactions on the Even Tin Isotopes NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(p, t), E=20 MeV; measured σ(Et, θ). 112Sn(p, t) deduced Q. 110Sn deduced mass excess. 110,112,114,116,118,120,122Sn deduced levels. 122Sn levels deduced J, π.
doi: 10.1016/0375-9474(70)90094-1
1970LA01 Nucl.Phys. A142, 545 (1970) Reactions of 197Au with 19 to 100 MeV 4He Ions: Equilibrium Statistical Model Analyses NUCLEAR REACTIONS 197Au(α, xαynzp), E=19-100 MeV; measured σ(E) for production of 195,196,197,198m,198,199,200Tl, 195m,197mHg, 194,195,196,198Au, mean recoil ranges.
doi: 10.1016/0375-9474(70)90811-0
Back to query form [Next] |