NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = H.R.Bowman Found 13 matches. 1985FR13 Phys.Rev. C32, 975 (1985) K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.L.Murphy, J.O.Rasmussen, J.P.Sullivan, E.Yoo, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert Pion Production Near Mid-Rapidity in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS C, Ca, U(40Ar, X), E=1050 MeV/nucleon; 9Be, 23Na, 19F(20Ne, X), E=655 MeV/nucleon; measured σ(θ(π+), E(π+)), σ(θ(π-), E(π-)); deduced ratio. Coulomb effect calculation comparison.
doi: 10.1103/PhysRevC.32.975
1982FR05 Phys.Rev. C25, 1102 (1982) K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.Murphy, J.O.Rasmussen, J.P.Sullivan, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert Pions Produced near the Center-of-Mass Velocity in Heavy-Ion Collisions NUCLEAR REACTIONS C, Ca, U(40Ar, π+), (40Ar, π-), E=1.05 GeV/nucleon; measured σ(E, θ).
doi: 10.1103/PhysRevC.25.1102
1982SU01 Phys.Rev. C25, 1499 (1982) J.P.Sullivan, J.A.Bistirlich, H.R.Bowman, R.Bossingham, T.Buttke, K.M.Crowe, K.A.Frankel, C.J.Martoff, J.Miller, D.L.Murphy, J.O.Rasmussen, W.A.Zajc, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr. Strong Coulomb Effects on Pions Produced in Heavy Ion Collisions NUCLEAR REACTIONS C, Na, F, Cu, U(20Ne, π+), (20Ne, π-), E=280-480 MeV/nucleon; C, K, Cl(40Ar, π+), (40Ar, π-), E=535 MeV/nucleon; measured σ(Eπ, θπ); deduced Coulomb effects, projectile fragment charges.
doi: 10.1103/PhysRevC.25.1499
1976RA37 Z.Phys. A279, 301 (1976); Erratum Z.Phys. A282, 124 (1977) D.G.Raich, H.R.Bowman, R.E.Eppley, J.O.Rasmussen, I.Rezanka Gamma and Alpha Decay from the 2.1-msec Isomer 213mRa RADIOACTIVITY 213mRa [from 209Bi(10B, 6n), Pb+12C, Bi+14N, Hg+16O]; measured Eγ, Iγ, I(X)-ray, Eα, Iα, γγ-coin, T1/2, γce-coin; deduced α-branching, IT. 213Ra, 209Rn deduced levels, J, π, ICC, λ.
doi: 10.1007/BF01408303
1972WI15 Phys.Rev. C5, 2041 (1972) J.B.Wilhelmy, E.Cheifetz, R.C.Jared, S.G.Thompson, H.R.Bowman, J.O.Rasmussen Angular Momentum of Primary Products Formed in the Spontaneous Fission Of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured (fragment)(fragment)(γ)-, (fragment)(fragment)(γ)(γ)-, (fragment)(fragment)(X)(γ)-coin, γγ-coin, Iγ(θ); deduced angular momentum of primary products. 100,102Zr, 104,106Mo, 108,110,112Ru, 112,114,116Pd, 118Cd, 138,140Xe, 142,144,146Ba, 146,148,150Ce, 152,154Nd, 158Sm; measured Iγ.
doi: 10.1103/PhysRevC.5.2041
1971CH14 Phys.Rev. C3, 2017 (1971) E.Cheifetz, H.R.Bowman, J.B.Hunter, S.G.Thompson Prompt Neutrons from Spontaneous Fission of 257Fm RADIOACTIVITY, Fission 257Fm(SF); measured average prompt neutron number.
doi: 10.1103/PhysRevC.3.2017
1970WA05 Nucl.Phys. A141, 449 (1970) R.L.Watson, J.B.Wilhelmy, R.C.Jared, C.Rugge, H.R.Bowman, S.G.Thompson, J.O.Rasmussen A Study of the Low-Energy Transitions Arising from the Prompt de-Excitation of Fission Fragments RADIOACTIVITY, Fission 252Cf(SF); measured E(ce), I(ce), E(X-ray), I(X-ray), I(ce)(t), (fragment)(fragment)(ce)(X)-coin. 102Zr, 106Mo, 108,109Tc, 110Ru, 116Rh, 140Cs, 144Ba, 146La, 148Ce, 149,150Pr; measured E(ce), I(ce); deduced Eγ, K/L, T1/2 (level). Detector - Si(Li), Si(P) fragment detectors.
doi: 10.1016/0375-9474(70)90982-6
1966WA01 Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn. (1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.423 (1966) R.L.Watson, H.R.Bowman, S.G.Thompson, J.O.Rasmussen Internal Conversion Electrons from Primary Fission Fragments NUCLEAR STRUCTURE 252Cf; measured not abstracted; deduced nuclear properties.
1963BO45 Phys.Rev. 129, 2133 (1963) H.R.Bowman, J.C.D.Milton, S.G.Thompson, W.J.Swiatecki Further Studies of the Prompt Neutrons from the Spontaneous Fission of Cf252 RADIOACTIVITY 252Cf(SF); measured decay products, neutron and fission fragments TOF; deduced neutron density distributions, number of neutrons per fragment as a fragment mass, the average c.m. neutron and fragment kinetic energies, nuclear temperature. Comparison with available data and calculations.
doi: 10.1103/PhysRev.129.2133
1963FR16 Can.J.Phys. 41, 2080 (1963) J.S.Fraser, J.C.D.Milton, H.R.Bowman, S.G.Thompson Precise kinetic energy measurements and fine structure in the spontaneous fission of Cf252 RADIOACTIVITY 252Cf(SF); measured decay products; deduced fission fragment kinetic energy spectra, energy, velocity, mass, mass ratio distributions, mass yields, mass-energy contours.
doi: 10.1139/p63-205
1957HU70 Phys.Rev. 107, 1294 (1957) E.K.Hulet, R.W.Hoff, H.R.Bowman, M.C.Michel Thermal-Neutron Fission Cross Sections for Isotopes of Plutonium, Americium, and Curium
doi: 10.1103/PhysRev.107.1294
1956CR69 Phys.Rev. 101, 1804 (1956) W.W.T.Crane, G.H.Higgins, H.R.Bowman Average Number of Neutrons per Fission for Several Heavy-Element Nuclides RADIOACTIVITY 236Pu(SF), 238Pu(SF), 240Pu(SF), 242Pu(SF), 242Cm(SF), 244Cm(SF), 252Cf(SF); measured products; deduced miscellaneous fission parameters. Data were imported from EXFOR entry 13717.
doi: 10.1103/PhysRev.101.1804
1956HU97 Phys.Rev. 102, 1621 (1956) E.K.Hulet, H.R.Bowman, M.C.Michel, R.W.Hoff Thermal-Neutron Fission Cross Section Of Pu240 NUCLEAR REACTIONS 240Pu(n, f), E=0.0253 eV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 13466.
doi: 10.1103/PhysRev.102.1621
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