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Search: Author = J.J.Hogan

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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
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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, ^{233,234,235,238}U, 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
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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
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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
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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
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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
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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
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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
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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
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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
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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, ^{48,47,46,44,43}Sc, ^43,42K, ^34,38,39Cl. Activation technique, Enriched target. Exciton model.

doi: 10.1007/BF01421692
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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
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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
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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 T_1/2. 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 ^{231,228,227,226}Th, ^215,224,223Ra.

doi: 10.1103/PhysRevC.20.1831
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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, T_1/2, 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
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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
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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 T_1/2, Eγ, Iγ; deduced (β++EC)-branching. ¹³⁸Pr; measured Eγ, Iγ. ¹³⁸Ce levels deduced γ-branching.

doi: 10.1139/v70-360
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0357.