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NSR database version of April 29, 2024.

Search: Author = G.A.Fisher

Found 8 matches.

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1988KU08      Phys.Rev. C37, 2281 (1988)

P.M.Kurjan, J.R.Calarco, G.A.Fisher, S.S.Hanna

Giant E1 Resonances in ²⁰Ne Observed with the ¹⁹F(p(pol), γ₀γ₁)²⁰Ne Reactions

NUCLEAR REACTIONS, ICPND ¹⁹F(polarized p, γ), E=3-10 MeV; measured γ yield, σ(θγ). ²⁰Ne deduced transition γ multipolarity, GDR features.

doi: 10.1103/PhysRevC.37.2281
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0086.

1983CA14      Phys.Rev. C28, 483 (1983); Erratum Phys.Rev. C29, 672 (1983)

J.R.Calarco, S.S.Hanna, C.C.Chang, E.M.Diener, E.Kuhlmann, G.A.Fisher

Absolute Cross Section for the Reaction ³H(p, γ₀)⁴He and a Review of ⁴He(γ, p₀)³H Measurements

NUCLEAR REACTIONS ³H(p, γ₀), E=8.34, 13.6 MeV; measured σ(θ=90°).

doi: 10.1103/PhysRevC.28.483
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1222.

1980CA11      Phys.Lett. 92B, 67 (1980)

J.R.Calarco, P.M.Kurjan, G.A.Fisher, S.S.Hanna

Intermediate Structure in the Giant E1 Resonance in the ¹⁹F(p, γ₀)²⁰Ne Reaction

NUCLEAR REACTIONS ¹⁹F(p, γ), (polarized p, γ), E=3.5-10 MeV; measured σ(E, θ); deduced E1, E2 capture amplitudes, intermediate structure. Doorway resonances model.

doi: 10.1016/0370-2693(80)90305-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0086.

1979VE02      Phys.Rev. C19, 1705 (1979)

E.Ventura, J.R.Calarco, C.C.Chang, E.M.Diener, D.G.Mavis, S.S.Hanna, G.A.Fisher

Structure in the Giant Resonance Region of ¹⁶O Observed with the Reaction ¹³C(³He, γ)¹⁶O

NUCLEAR REACTIONS ¹³C(³He, γ), E=3.0-8.5 MeV; measured σ(E(³He), Eγ, θ). ¹⁶O deduced resonances, structure in giant resonance region. Enriched ¹³C target.

doi: 10.1103/PhysRevC.19.1705
Citations: PlumX Metrics

1976FI05      Phys.Rev. C14, 28 (1976)

G.A.Fisher, P.Paul, F.Riess, S.S.Hanna

Giant E1 Resonances in ⁸Be from the Reaction ⁷Li(p, γ)⁸Be

NUCLEAR REACTIONS ⁷Li(p, γ), E=0.8-17.6 MeV; measured σ(E, Eγ, θ). ⁸Be deduced giant resonances, Γγ.

doi: 10.1103/PhysRevC.14.28
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0022.

1973HA62      Nucl.Phys. A216, 221 (1973)

M.Hasinoff, G.A.Fisher, S.S.Hanna

Isospin Splitting of Giant E1 Excitations in ⁹⁰Zr

NUCLEAR REACTIONS ⁸⁹Y(p, γ), Ep=5.4-17.0 MeV; measured σ(Ep;Eγ, θ(γ)). ⁹⁰Zr deduced giant dipole resonances, analog resonances, resonance parameters, isospin splitting, γ-hindrance, level-width. Natural target.

doi: 10.1016/0375-9474(73)90466-1
Citations: PlumX Metrics

1972HA62      Nucl.Phys. A195, 78 (1972)

M.Hasinoff, G.A.Fisher, P.Kurjan, S.S.Hanna

Isospin Splitting of Giant E1 Excitations in the N = 82 Nucleus ¹⁴²Nd

NUCLEAR REACTIONS ¹⁴¹Pr(p, γ), Ep=6-17 MeV; measured σ(Ep;Eγ, θ(γ)). ¹⁴²Nd deduced giant dipole resonances, analog resonances, resonance parameters, isospin splitting. Natural targets.

doi: 10.1016/0375-9474(72)90722-1
Citations: PlumX Metrics

1969HA41      Phys.Letters 30B, 337 (1969)

M.Hasinoff, G.A.Fisher, H.M.Kuan, S.S.Hanna

Isospin Splitting of E1 Resonances in ⁸⁸Sr and ⁹⁰Zr

NUCLEAR REACTIONS ⁸⁷Rb(p, γ), E = 4-15 MeV; ⁸⁷Rb(p, p), E = 5-12 MeV; measured σ(E;Eγ), σ(E). ⁸⁸Sr deduced resonances, level-width, isospin splitting. ⁸⁹Y(p, γ), E = 7-14 MeV; ⁸⁹Y(p, p), E = 10-14 MeV; measured σ(E;Eγ, θ(γ)), σ(E). ⁹⁰Zr deduced resonances, level-width, isospin splitting.

doi: 10.1016/0370-2693(69)90498-5
Citations: PlumX Metrics