NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = H.W.Schmitt Found 38 matches. 1994HE11 Nucl.Phys. A571, 541 (1994) R.Henneck, G.Masson, P.D.Eversheim, R.Gebel, F.Hinterberger, U.Lahr, H.W.Schmitt, J.Schleef, B.von Przewoski Depolarization in Proton-6Li Elastic Scattering NUCLEAR REACTIONS 6Li(polarized p, p), E=72 MeV; measured depolarization parameter; deduced nucleon-nucleus isoscalar spinflip interaction. Optical model.
doi: 10.1016/0375-9474(94)90224-0
1974BO23 Phys.Rev. C10, 231 (1974) J.R.Boyce, T.D.Hayward, R.Bass, H.W.Newson, E.G.Bilpuch, F.O.Purser, H.W.Schmitt Absolute Cross Sections for Proton-Induced Fission of the Uranium Isotopes NUCLEAR REACTIONS 233,234,235,236,238U(p, xnF), E=5-30 MeV; measured σ(E, fragment mass, E(fragment), θ); deduced angular anisotrophies. 232,233,234,235,236,237,238,239Np deduced fission thresholds, n-width/F-width.
doi: 10.1103/PhysRevC.10.231
1974KO17 Phys.Rev. C10, 1529 (1974) D.Kolb, R.Y.Cusson, H.W.Schmitt Asymmetric Fission of 236U in a Self-Consistent K-Matrix Model NUCLEAR STRUCTURE, Fission 236U; calculated fission path, shape asymmetry, static total energy, single particle energies. Self-consistent Brueckner-Hartree-Fock method.
doi: 10.1103/PhysRevC.10.1529
1973FE01 Phys.Rev. C7, 2510 (1973) R.L.Ferguson, F.Plasil, F.Pleasonton, S.C.Burnett, H.W.Schmitt Systematics of Fragment Mass and Energy Distributions for Proton-Induced Fission of 233U, 235U, and 238U NUCLEAR REACTIONS 233,235,238U(p, F), E=7-13 MeV; measured σ(E, E(fragment)), (fragment)(fragment)-coin. Deduced fragment mass vs total kinetic energy distribution.
doi: 10.1103/PhysRevC.7.2510
1973FE07 Phys.Rev. C8, 1104 (1973) R.L.Ferguson, F.Plasil, H.Freiesleben, C.E.Bemis, Jr., H.W.Schmitt Fragment Kinetic Energy in 18O-Induced Fission of 232Th and 246Cm NUCLEAR REACTIONS, Fission 232Th, 246Cm(18O, F), E=93.7-125.6 MeV; measured E(fragment). Deduced fragment, kinetic energy.
doi: 10.1103/PhysRevC.8.1104
1973MU03 Phys.Rev. C7, 1519 (1973) M.G.Mustafa, U.Mosel, H.W.Schmitt Asymmetry in Nuclear Fission NUCLEAR STRUCTURE 202Pb, 210Po, 236U, 248Cm, 252,258,264Fm calculated potential energies based on two-center model with asymmetric deformations.
doi: 10.1103/PhysRevC.7.1519
1973MU16 Phys.Rev. C8, 1924 (1973) Potential-Energy Surface for the Fission of the Superheavy Nucleus 298X NUCLEAR REACTIONS 298Fl(n, F), (p, F); calculated potential energy surface.
doi: 10.1103/PhysRevC.8.1924
1973PL01 Phys.Rev. C7, 1186 (1973) F.Plasil, R.L.Ferguson, F.Pleasonton, H.W.Schmitt Fission of 209Bi by 36.1-MeV Protons; Search for an Asymmetric Component in the Mass Distribution, and Neutron-Emission Results NUCLEAR REACTIONS 209Bi(p, F), E=36.1 MeV; measured σ(F). Deduced mass yield distribution, average number of neutrons as a function of fragment mass.
doi: 10.1103/PhysRevC.7.1186
1973ST04 Nucl.Sci.Eng. 50, 169 (1973) R.W.Stoughton, J.Halperin, C.E.Bemis, H.W.Schmitt Neutron Multiplicity Distributions in the Spontaneous Fission of 246Cm, 248Cm, and 252Cf RADIOACTIVITY, Fission 246,248Cm, 252Cf(SF); measured (n)(fragment)-coin, deduced neutron multiplicity distribution.
doi: 10.13182/NSE73-A23241
1972MA82 Nucl.Instrum.Methods 102, 181 (1972) R.L.Macklin, F.M.Glass, J.Halperin, R.T.Roseberry, H.W.Schmitt, R.W.Stoughton, M.Tobias Neutron Multiplicity Counter RADIOACTIVITY, Fission 252Cf (SF); measured neutron multiplicity ν-bar.
doi: 10.1016/0029-554X(72)90537-X
1972MU06 Phys.Rev.Lett. 28, 1536 (1972) M.G.Mustafa, U.Mosel, H.W.Schmitt Asymmetric Fission in the Two-Center Model NUCLEAR STRUCTURE 252,258,264Fm, 236U; calculated 4-dimensional potential energy surfaces. 2-center model.
doi: 10.1103/PhysRevLett.28.1536
1972PL01 Phys.Rev. C5, 528 (1972) Mass and Energy Distributions from 77.3-MeV-4He-Induced Fission of 181Ta, 209Bi, and 233U: A Test of Liquid-Drop-Model Predictions NUCLEAR REACTIONS, Fission 181Ta, 209Bi, 233U(α, F), E=77.3 MeV; measured fragment energy, mass distributions.
doi: 10.1103/PhysRevC.5.528
1972PL05 Phys.Rev. C6, 1023 (1972) F.Pleasonton, R.L.Ferguson, H.W.Schmitt Prompt Gamma Rays Emitted in the Thermal-Neutron-Induced Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured (fragment)(fragment)(γ)(γ)-coin; deduced average γ-ray energy, number.
doi: 10.1103/PhysRevC.6.1023
1972RO09 Phys.Lett. 38B, 501 (1972) H.Rosler, F.Plasil, H.W.Schmitt High-Resolution Cross Section Measurement for 236U(n, f) NUCLEAR REACTIONS, Fission 236U(n, F), E=0.5-2.6 MeV; measured σ(E). 237U deduced possible collective levels in second potential.
doi: 10.1016/0370-2693(72)90527-8
1972SC16 Nucl.Phys. A186, 1 (1972) Fission Properties of Heavy and Superheavy Nuclei NUCLEAR STRUCTURE, Fission Z=184, A=220-310; calculated total fragment kinetic energies, excitation energies, neutron number.
doi: 10.1016/0375-9474(72)90120-0
1971BU06 Phys.Rev. C3, 2034 (1971) S.C.Burnett, R.L.Ferguson, F.Plasil, H.W.Schmitt Neutron Emission and Fission Energetics in the Proton-Induced Fission of 233U and 238U NUCLEAR REACTIONS, Fission 233U(p, F), E=8.5, 13 MeV; 238U(p, F), E=12 MeV; measured neutron numbers, fragment mass, energy distributions.
doi: 10.1103/PhysRevC.3.2034
1971FE09 Nucl.Phys. A172, 33 (1971) R.L.Ferguson, F.Plasil, G.D.Alam, H.W.Schmitt Fission Fragment Mass Distributions and Kinetic Energies for Spontaneous Fission Isomers RADIOACTIVITY, Fission 239mAm, 237mPu, 236mU, 238mU(SF); measured fragment mass, energy distributions; deduced mean values, widths.
doi: 10.1016/0375-9474(71)90114-X
1971MO09 Nucl.Phys. A165, 73 (1971) Potential Energy Surfaces for Heavy Nuclei in the Two-Center Model NUCLEAR STRUCTURE 226Ra, 232Th, 236U, 242Pu, 244Cm, 248Cf, 252Fm; calculated potential energy surfaces. Two-center model.
doi: 10.1016/0375-9474(71)90150-3
1971MO30 Phys.Rev. C4, 2185 (1971) Fragment-Shell Influences in Nuclear Fission NUCLEAR STRUCTURE 202Pb, 212Rn, 226Ra, 244Cm, 252Fm, 264Fm, 272Fm, 232Th, 236U, 242Pu, 248Cf; calculated potential energy surfaces, shell-correction- energy surfaces. 2-center model.
doi: 10.1103/PhysRevC.4.2185
1971MO38 Phys.Lett. 37B, 335 (1971) Fission Barriers for Light Elements (A = 180-212) NUCLEAR STRUCTURE, Fission A=180-212, Z=74-86; 188Os; calculated fission barriers. Two-center shell model, Strutinsky approximation.
doi: 10.1016/0370-2693(71)90194-8
1971MU21 Nucl.Phys. A178, 9 (1971) M.G.Mustafa, H.W.Schmitt, U.Mosel Dipole Excitations in Fission Fragments NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; calculated fragment dipole excitations at scission points.
doi: 10.1016/0375-9474(71)90180-1
1970FE03 Phys.Lett. 31B, 526 (1970) R.L.Ferguson, F.Plasil, G.D.Alam, H.W.Schmitt Fission Fragment Mass Distributions and Kinetic Energies for Spontaneously Fissioning Isomers NUCLEAR REACTIONS 235U(d, p), E=13 MeV; 240Pu(p, 2n), E=13 MeV; measured fission fragment energy, mass distributions.
doi: 10.1016/0370-2693(70)90081-X
1969KO28 Nucl.Phys. A139, 513 (1969) E.Konecny, W.Norenberg, H.W.Schmitt Fragment Energy Correlation Measurements for the Proton Induced Fission of 226Ra NUCLEAR REACTIONS, Fission 226Ra(p, F), E=9, 11, 13 MeV; measured mass yield, average kinetic energy, variance of total kinetic energy.
doi: 10.1016/0375-9474(69)90275-9
1965SC25 Phys.Rev. 137, B837 (1965) H.W.Schmitt, W.E.Kiker, C.W.Williams Precision measurements of correlated energies and velocities of 252Cf fragments RADIOACTIVITY 252Cf(SF); measured products; deduced yields. Data were imported from EXFOR entry 13081.
doi: 10.1103/PhysRev.137.B837
1964WA26 Phys.Rev. 133, B1500 (1964) F.J.Walter, H.W.Schmitt, J.H.Neiler Fragment Mass Distributions for Thermal-Neutron-Induced Fission of Pu239 and Pu241 NUCLEAR REACTIONS 239,241Pu(n, F), E thermal; deduced fragment mass distributions, fission yields.
doi: 10.1103/physrev.133.b1500
1961SC20 Phys.Rev. 121, 827 (1961) Al27(n, α)Na24 Cross Section as a Function of Neutron Energy NUCLEAR STRUCTURE 24Na; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.121.827
1960SC10 Nuclear Phys. 20, 202 (1960) Absolute Neutron Absorption Cross Sections for Sb-Be Photoneutrons
doi: 10.1016/0029-5582(60)90170-X
1960SC11 Nuclear Phys. 20, 220 (1960) Determination of the Energy of Antimony-Beryllium Photoneutrons NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90171-1
1960SC15 Nuclear Phys. 17, 109 (1960) H.W.Schmitt, R.C.Block, R.L.Bailey Total Neutron Cross Section of B10 in the Thermal Neutron Energy Range NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90105-X
1959CO58 Bull.Am.Phys.Soc. 4, No.6, 359, J7 (1959) Neutron Absorption Cross Sections with Sb-Be Neutrons
1959GI48 Phys.Rev. 114, 1319 (1959) J.H.Gibbons, R.L.Macklin, J.B.Marion, H.W.Schmitt Precision Measurement of the Be9(γ, n) Cross Section
doi: 10.1103/PhysRev.114.1319
1959MU25 Phys.Rev. 115, 1707 (1959) Cross Section for the Li6(n, α)H3 Reaction for 1.2 < E < 8.0 MeV
doi: 10.1103/PhysRev.115.1707
1959SC70 ORNL-2610, p.17 (1959) H.W.Schmitt, R.B.Murray, J.J.Manning Li6(n, α)H3 Cross Section as a Function of Neutron Energy from 1.2 to 8 MeV
1959SC73 Phys.Rev. 116, 1575 (1959) Neutron Induced Fission Cross Section Of Np237 NUCLEAR REACTIONS 237Np(n, f), E=910 keV-7.4 MeV; measured products ; deduced σ, σ(E). Data were imported from EXFOR entry 12488.
doi: 10.1103/PhysRev.116.1575
1959SC74 Bull.Am.Phys.Soc. 4, No.1, 43, R8 (1959) H.W.Schmitt, J.H.Gibbons, C.N.Inskeep Neutron Absorption Cross Sections at 27 kev NUCLEAR REACTIONS Ag, 197Au, Sb, Pb(n, X), E=27 keV; measured reaction products; deduced tabulated σ.
1958MU07 Bull.Am.Phys.Soc. 3, No.7, 381, T5 (1958) Cross Section of the Li6(n, α)T Reaction from 1.2 to 8 MeV
1957LE21 J.Nuclear Energy 4, 38 (1957) The Cross-Section for U238 Fission by Fission Neutrons Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12448. 1955GI54 Phys.Rev. 100, 167 (1955) J.H.Gibbons, R.L.Macklin, H.W.Schmitt V51(p, n)Cr51 Reaction as a 5- to 120-keV Neutron Source
doi: 10.1103/PhysRev.100.167
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