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Search: Author = J.J.Hogan

Found 34 matches.

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1993TO01      J.Phys.(London) G19, 187 (1993)

J.R.D.Todd, A.R.Wolf, J.J.Hogan, D.J.Parker

Fission Events in the 120 MeV 12C + 238U System

NUCLEAR REACTIONS 238U(12C, F), E=120 MeV; measured fission fragment σ(θ), differential range distribution, production σ, kinetic energy distributions. Recoil method.

doi: 10.1088/0954-3899/19/1/013
Citations: PlumX Metrics


1991HO11      Z.Phys. A338, 325 (1991)

J.J.Hogan, D.J.Parker, J.Asher

Fission following Complete or Incomplete Fusion of 135 MeV 16O and 238U

NUCLEAR REACTIONS, ICPND 238U(16O, X), E=315 MeV; measured residuals σ(fragment θ), complete, imcomplete fusion product σ for X=91Sr-143Ce.

doi: 10.1007/BF01288197
Citations: PlumX Metrics


1991PA09      Phys.Rev. C44, 1528 (1991)

D.J.Parker, P.Vergani, E.Gadioli, J.J.Hogan, F.Vettore, E.Gadioli-Erba, E.Fabrici, M.Galmarini

Recoil Range Study of Complete and Incomplete Fusion of C and Au at 10 MeV/Nucleon

NUCLEAR REACTIONS 197Au(12C, X), E=120 MeV; measured residue production σ, X=196Au-204Po; deduced reaction mechanism. Monte Carlo calculations.

doi: 10.1103/PhysRevC.44.1528
Citations: PlumX Metrics


1990HO16      Phys.Rev. C42, 1043 (1990)

J.J.Hogan, E.Gadioli, P.Vergani, R.F.Fantoni

Alpha-Induced Reactions on Fissile Nuclei at Energies to 50 MeV

NUCLEAR REACTIONS, ICPND 232Th, 233,234,235,238U, 237Np, 238,239,242Pu(α, xnyp), E=20-50 MeV; compiled, analyzed σ(E) data; deduced fission barrier role. Fission competition in reaction mechanism.

doi: 10.1103/PhysRevC.42.1043
Citations: PlumX Metrics


1990PA17      Z.Phys. A336, 411 (1990)

D.J.Parker, J.J.Hogan, J.Asher

Fission Product Energies and Anisotropies following Complete Fusion of 16O + 238U

NUCLEAR REACTIONS, ICPND 238U(16O, F), E=101 MeV; measured fission product cumulative, independent yields following complete fusion.


1989PA06      Phys.Rev. C39, 2256 (1989)

D.J.Parker, J.J.Hogan, J.Asher

Complete and Incomplete Fusion of 6 MeV/Nucleon Light Heavy Ions on 51V

NUCLEAR REACTIONS, ICPND 51V(12C, X), (15N, X), (16O, X), (19F, X), (20Ne, X), E=6 MeV/nucleon; measured light charged particle yields, radioactive 54Mn-66Ga residues yields. Incomplete fusion sum rule model analysis.

doi: 10.1103/PhysRevC.39.2256
Citations: PlumX Metrics


1987PA01      Phys.Rev. C35, 161 (1987)

D.J.Parker, J.J.Hogan, J.Asher

Complete and Incomplete Fusion in 20Ne + 93Nb Reactions

NUCLEAR REACTIONS 93Nb(20Ne, X)109In/109mIn/108Sn/108In/108mIn/107In/107mIn/105Ag/105mAg/104Cd/103Ag/103mAg/101Pd/100Pd/99Pd/101Rh/101mRh/100Rh/99Pd/99Rh/99mRh/97Rh/97Ru/96Tc/96mTc/95Tc/94Tc/93Tc/93Mo/93mMo/93mMo/92Nb/92mNb/90Nb/90mNb/89Zr/89mZr/88Zr/87Y/87mY, E=106, 148 MeV; measured σ(θ), σ(E, θ), X=C, N, O, F, B, P, α, recoil distributions, residues yields; deduced complete, incomplete fusion contributions. ΔE-E telescope.

doi: 10.1103/PhysRevC.35.161
Citations: PlumX Metrics


1986MO16      Phys.Rev. C34, 899 (1986)

K.J.Moody, J.J.Hogan

Deexcitation of the Complete Fusion Nucleus 155Tb

NUCLEAR REACTIONS, ICPND 133Cs(22Ne, 4n), (22Ne, 3n), (22Ne, 5n), (22Ne, 6n), (22Ne, 7n), (22Ne, 8n), (22Ne, 9n), (22Ne, 3nα), (22Ne, 4nα), (22Ne, 5nα), (22Ne, 6nα), E=92.6-145 MeV; measured residual production σ(E); deduced favored high-spin isomeric species production. Hauser-Feshbach evaporation code. Activation technique.

doi: 10.1103/PhysRevC.34.899
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0352.


1985HO05      Phys.Rev. C31, 477 (1985)

J.J.Hogan, J.Asher, D.J.Parker

Recoil of Products from Reactions of 20,22Ne with 93Nb at 100 and 142 MeV

NUCLEAR REACTIONS 93Nb(20Ne, X), (22Ne, X)87Y/87mY/88Zr/89Zr/90Nb/92Nb/92mNb/95Nb/93Mo/93mMo/93Tc/94Tc/95Tc/96Tc/96mTc/97Rh/98Rh/99Rh/99mRh/100Rh/100Pd/101Pd/101Ag/102Ag/103Ag/104Ag/105Ag/105mAg/104Cd/105Cd/105In/106In/106mIn/107In/108In/109In/110In/110mIn/111In/108Sn/109Sn/110Sn/111Sn, E=100, 142 MeV; measured residuals thick target yields; deduced mean recoil velocity, range, angle. Stacked, tilted catcher foils. Heavy ion fusion, mass transfer.

doi: 10.1103/PhysRevC.31.477
Citations: PlumX Metrics


1984GA01      Phys.Rev. C29, 76 (1984)

E.Gadioli, E.Gadioli-Erba, J.J.Hogan, B.V.Jacak

Model for Alpha Particle Induced Nuclear Reactions: 93Nb(α, xαypzn) from 40-140 MeV

NUCLEAR REACTIONS, ICPND 93Nb(α, n), (α, 2n), (α, 3n), (α, 4n), (α, 5n), (α, 6np), (α, n2p), (α, 5n2p), (α, 6n2p), (α, 7n2p), (α, 5n3p), (α, 6n3p), (α, 7n3p), (α, 8n3p), (α, 10n3p), (α, 9n5p), (α, 7n6p), (α, 5n4p), (α, 6n4p), (α, 7n4p), (α, 9n4p), E=40-140 MeV; measured residuals production σ(E); deduced reaction mechanism. Comprehensive theoretical model, inelastic scattering, nucleon pickup, binary fragmentation, projectile breakup preequilibrium processes.

doi: 10.1103/PhysRevC.29.76
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0312.


1983BE35      Can.J.Phys. 61, 641 (1983)

P.A.Beeley, J.Aaronson, K.Kokkas, J.J.Hogan

45Sc(α, αn)44m+gSc: A monitor reaction for alpha particle induced reactions

NUCLEAR REACTIONS, ICPND 45Sc(α, αn), E=20-90 MeV; measured Eγ, Iγ; deduced production σ(E) for 44m,44Sc, isomeric ratios.


1983CH32      Can.J.Chem. 61, 646 (1983)

C.Chung, J.J.Hogan, H.H.Muller

Fission Probability in the 232Th(p, p'xnf) Reaction at Low Energy

NUCLEAR REACTIONS, ICPND 232Th(p, p'), E=52.5 MeV; calculated fission probability following neutron evaporation vs excitation energy, product yield. Modified preequilibrium exciton models.

doi: 10.1139/v83-118
Citations: PlumX Metrics


1982CH03      Phys.Rev. C 25, 899 (1982)

C.Chung, J.J.Hogan

238U fission at energies up to 100 MeV

NUCLEAR REACTIONS 238U(n, F), E=10-100 MeV; calculated spallation yields and fissionability; deduced interpretation of mass distribution and charge dispersion. Extended exciton model.

doi: 10.1103/physrevc.25.899
Citations: PlumX Metrics


1981CH14      Phys.Rev. C24, 180 (1981)

C.Chung, J.J.Hogan

Fission of 232Th at Energies up to 90 MeV

NUCLEAR REACTIONS, Fission 232Th(p, F), E=8-90 MeV; analyzed fragment mass distribution, charge dispersion data. Exciton model.

doi: 10.1103/PhysRevC.24.180
Citations: PlumX Metrics


1981GA22      Z.Phys. A301, 289 (1981)

E.Gadioli, E.Gadioli Erba, J.J.Hogan, K.I.Burns

Emission of Alpha Particles in the Interaction of 10-85 MeV Protons with 48,50Ti

NUCLEAR REACTIONS 48,50Ti(p, xnypzα), E ≈ 10-85 MeV; measured production σ(E) for 48,47V, 48,47,46,44,43Sc, 43,42K, 34,38,39Cl. Activation technique, Enriched target. Exciton model.

doi: 10.1007/BF01421692
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4060.


1981HO11      Z.Phys. A299, 163 (1981)

J.J.Hogan

Decay of the Complete Fusion Nucleus, 151Eu

NUCLEAR REACTIONS 133Cs(18O, xn), E=75-125 MeV; measured σ(E) for x=3, 4, 5, 6. 151Eu deduced L(critical), moment of inertia, yrast line. Diamond-Stephens evaporation model.

doi: 10.1007/BF01440917
Citations: PlumX Metrics


1980HO12      Z.Phys. A295, 169 (1980)

J.J.Hogan

An Evaluation of Alpha Particle Clustering in Heavy Nuclei

NUCLEAR STRUCTURE 50Ti, 90Zr, 141Pr, 202Hg, 232Th; calculated rate of nucleon-nucleon, nucleon-α interactions; deduced number of α clusters. Pre-equilibrium models of α emission.

doi: 10.1007/BF01413074
Citations: PlumX Metrics


1980HO33      Radiochim.Acta 27, 73 (1980)

J.J.Hogan

Half Lives of Neutron-Deficient Europium Nuclides

RADIOACTIVITY 145,146Eu(EC), (β+); 147,148Eu(EC), (β+), (α) [from 133Cs(18O, xn), E=75-122 MeV]; measured T1/2. Activation technique.


1979HO22      Phys.Rev. C20, 1831 (1979)

J.J.Hogan, E.Gadioli, E.Gadioli-Erba, C.Chung

Fissionability of Nuclides in the Thorium Region at Excitation Energies to 100 MeV

NUCLEAR REACTIONS 232Th(p, xn), (p, xnyp), E=10-100 MeV; measured σ(E), production σ for 231,228,227,226Th, 215,224,223Ra.

doi: 10.1103/PhysRevC.20.1831
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0030.


1978HO22      Nuovo Cim. 45A, 341 (1978)

J.J.Hogan, E.Gadioli

Production of 24Na from 27Al by (35-100) MeV Protons

NUCLEAR REACTIONS 27Al(p, n3p), E=35-100 MeV; measured production σ(E) for 24Na; deduced reaction mechanism.

doi: 10.1007/BF02730075
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0131.


1977GA16      Phys.Rev. C16, 1404 (1977)

E.Gadioli, E.Gadioli Erba, J.J.Hogan

Preequilibrium Decay of Nuclei with A ≈ 90 at Excitation Energies to 100 MeV

NUCLEAR REACTIONS 88Sr(p, xn), (p, 3np), (p, xn2p), 89Y(p, xn), (p, xnp), 90Zr(p, xn), (p, xn2p), (p, xn3p), (p, xn4p), E=10-100 MeV; calculated σ(E), Ep, Eα.

doi: 10.1103/PhysRevC.16.1404
Citations: PlumX Metrics


1977GA20      Nuovo Cim. 40A, 383 (1977)

E.Gadioli, E.Gadioli Erba, J.J.Hogan

Pre-Equilibrium Decay of Nuclei with A ≈ 200 at Excitation Energies to 90 MeV

NUCLEAR REACTIONS 197Au, 202Hg(p, X), E=10-90 MeV; calculated σ(E).

doi: 10.1007/BF02812508
Citations: PlumX Metrics


1976BR21      J.Inorg.Nucl.Chem. 38, 1581 (1976)

J.C.Brodovitch, J.J.Hogan, K.I.Burns

The Pre-Equilibrium Statistical Model: Comparison of Calculations with Two (p, xn) Reactions

NUCLEAR REACTIONS 75As, 96Mo(p, n), (p, 3n), 96Mo(p, 2n), (p, 4n), E=10-85 MeV; calculated σ(E).

doi: 10.1016/0022-1902(76)80639-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2016.


1976GA28      Phys.Lett. 65B, 311 (1976)

E.Gadioli, E.Gadioli Erba, G.Tagliaferri, J.J.Hogan

Nucleon Mean Free Path in Nuclear Matter

NUCLEAR REACTIONS 88Sr(p, 3n), E=39 MeV; 88Sr(p, 4n), (p, 3np), 89Y(p, 4n), E=54 MeV; 88Sr(p, 5n), E=69 MeV; 88Sr(p, 3n2p), E=73 MeV; 89Y(p, 3n), E=40 MeV; 89Y(p, 2np), E=42.5 MeV; 89Y(p, 4np), E=72 MeV; 90Zr(p, 2n2p), E=60 MeV; 90Zr(p, 3n2p), E=77.5 MeV; calculated σ.

doi: 10.1016/0370-2693(76)90229-X
Citations: PlumX Metrics


1976KA06      Phys.Rev. C13, 1095 (1976)

M.V.Kantelo, J.J.Hogan

Radiochemical Study of Alpha Particle Emission in Reactions of 202Hg with 10-86 MeV Protons

NUCLEAR REACTIONS 202Hg(p, xn2p), E=10-86 MeV; measured σ(E); deduced α yields.

doi: 10.1103/PhysRevC.13.1095
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0105.


1976KA18      Phys.Rev. C14, 64 (1976)

M.V.Kantelo, J.J.Hogan

Charged-Particle Emission in Reactions of 90Zr with 10-86 MeV Protons

NUCLEAR REACTIONS 90Zr(p, n2p), (p, 2n2p), (p, 3n2p), (p, 4n2p), (p, 5n2p), 90Zr(p, 3n3p), (p, 5n3p), (p, 6n3p), (p, 3n4p), (p, 4n4p), (p, 5n4p), E=10-86 MeV; measured σ; deduced α-yields, charged-particle emission probabilities. Enriched target.

doi: 10.1103/PhysRevC.14.64
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0130.


1973HO07      J.Inorg.Nucl.Chem. 35, 705 (1973)

J.J.Hogan

Isomer Ratios of Tc Isotopes Produced in 10-65 MeV Bombardments of 96Mo

NUCLEAR REACTIONS 96Mo(p, xn), E=10-65 MeV; measured σ(E), isomeric σ ratios.

doi: 10.1016/0022-1902(73)80437-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0025.


1973HO13      J.Inorg.Nucl.Chem. 35, 1429 (1973)

J.J.Hogan

The 96Mo(p, n)96Tc-m, g Reaction from 10 to 65 MeV

NUCLEAR REACTIONS 96Mo(p, n), E=10-65 MeV; measured σ(E); 96Tc deduced isomeric σ ratio.

doi: 10.1016/0022-1902(73)80228-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0025.


1973HO17      J.Inorg.Nucl.Chem. 35, 2123 (1973)

J.J.Hogan

Comparison of the 94Mo(p, n)94Tc-m, g and 96Mo(p, n)96Tc-mg Reactions

NUCLEAR REACTIONS 96Mo(p, n), E=10-65 MeV; measured isomer ratio.

doi: 10.1016/0022-1902(73)80168-X
Citations: PlumX Metrics


1973LA20      Phys.Rev. C8, 715 (1973)

J.C.F.Lau, J.J.Hogan

Investigation of Branching Ratios between Isomeric States of 154Tb

RADIOACTIVITY 154Tb; measured Eγ, T1/2, Iγ. 154Tb levels deduced J, π, γ-branching.

doi: 10.1103/PhysRevC.8.715
Citations: PlumX Metrics


1972HO35      Phys.Rev. C6, 810 (1972)

J.J.Hogan

96Mo(p, xn) Reaction from 10 to 80 MeV

NUCLEAR REACTIONS 96Mo(p, xn), E=10-80 MeV; measured σ(E).

doi: 10.1103/PhysRevC.6.810
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0025.


1971HO34      J.Inorg.Nucl.Chem. 33, 3627 (1971)

J.J.Hogan

Study of the 141Pr(p, xn) Reaction from 10-85 MeV

NUCLEAR REACTIONS 141Pr(p, xn), E=10-85 MeV; measured σ(E). 139Nd deduced isomeric σ ratio.

doi: 10.1016/0022-1902(71)80267-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0003.


1970HO28      Can.J.Chem. 48, 2151 (1970)

J.J.Hogan

The Radioactive Decay Series 138Nd → 138Pr → 138Ce

RADIOACTIVITY 138Nd, 138mPr; measured T1/2, Eγ, Iγ; deduced (β++EC)-branching. 138Pr; measured Eγ, Iγ. 138Ce levels deduced γ-branching.

doi: 10.1139/v70-360
Citations: PlumX Metrics


1969HO47      Phys.Rev. 182, 1210 (1969)

J.J.Hogan, N.Sugarman

Production of Heavy Nuclides in 440-MeV Proton Fission Of Uranium

NUCLEAR REACTIONS U(p, f), E=147 MeV; measured products, 139Ba, 139Cs, 139Ce, 139Pr; deduced yields. Data were imported from EXFOR entry O0357.

doi: 10.1103/PhysRev.182.1210
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0357.


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