NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of May 10, 2024.

Search: Author = H.W.Schmitt

Found 38 matches.

Back to query form



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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0426.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0527.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0799.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1973MU16      Phys.Rev. C8, 1924 (1973)

M.G.Mustafa, H.W.Schmitt

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10605.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1972PL01      Phys.Rev. C5, 528 (1972)

F.Plasil, H.W.Schmitt

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2483.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14197.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10262.


1972SC16      Nucl.Phys. A186, 1 (1972)

H.W.Schmitt, U.Mosel

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1971MO09      Nucl.Phys. A165, 73 (1971)

U.Mosel, H.W.Schmitt

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
Citations: PlumX Metrics


1971MO30      Phys.Rev. C4, 2185 (1971)

U.Mosel, H.W.Schmitt

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
Citations: PlumX Metrics


1971MO38      Phys.Lett. 37B, 335 (1971)

U.Mosel, H.W.Schmitt

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2429.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2428.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13081.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14612.


1961SC20      Phys.Rev. 121, 827 (1961)

H.W.Schmitt, J.Halperin

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11530.


1960SC10      Nuclear Phys. 20, 202 (1960)

H.W.Schmitt, C.W.Cook

Absolute Neutron Absorption Cross Sections for Sb-Be Photoneutrons

doi: 10.1016/0029-5582(60)90170-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11778.


1960SC11      Nuclear Phys. 20, 220 (1960)

H.W.Schmitt

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11245.


1959CO58      Bull.Am.Phys.Soc. 4, No.6, 359, J7 (1959)

C.W.Cook, H.W.Schmitt

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0441.


1959MU25      Phys.Rev. 115, 1707 (1959)

R.B.Murray, H.W.Schmitt

Cross Section for the Li6(n, α)H3 Reaction for 1.2 < E < 8.0 MeV

doi: 10.1103/PhysRev.115.1707
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11105.


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)

H.W.Schmitt, R.B.Murray

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12488.


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)

R.B.Murray, H.W.Schmitt

Cross Section of the Li6(n, α)T Reaction from 1.2 to 8 MeV


1957LE21      J.Nuclear Energy 4, 38 (1957)

R.B.Leachman, H.W.Schmitt

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
Citations: PlumX Metrics


Back to query form