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NSR database version of April 11, 2024.

Search: Author = R.Avida

Found 16 matches.

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1988DU10      Phys.Rev. C37, 2881 (1988)

J.S.Dunham, R.T.Westervelt, R.Avida, S.S.Hanna

Magnetic Moments of the First Excited 2+ States of the Even-Even Te Isotopes

NUCLEAR REACTIONS 122,124,126,128,130Te(35Cl, 35Cl'), E=70 MeV; measured γ(35Cl)(θ, H) following Coulomb excitation. 122,124,126,128,130Te level deduced g.

doi: 10.1103/PhysRevC.37.2881
Citations: PlumX Metrics

1974BO28      Nucl.Phys. A228, 253 (1974)

R.N.Boyd, R.Arking, J.C.Lombardi, A.B.Robbins, S.Yoshida, D.C.Slater, H.T.King, R.Avida

Decay of the 7/2- Isobaric Analogue Resonance in 125Sb

NUCLEAR REACTIONS 124Sn(p, p'), (polarized p, p'), E=10.0-10.9 MeV; measured σ(Ep', θ), A(Ep', θ). 125Sb deduced isobaric analog resonance, p-width.

doi: 10.1016/0375-9474(74)90431-X
Citations: PlumX Metrics

1974HA01      Phys.Rev.Lett. 32, 114 (1974)

S.S.Hanna, H.F.Glavish, R.Avida, J.R.Calarco, E.Kuhlmann, R.LaCanna

Evidence for a Giant Quadrupole Resonance in 16O

NUCLEAR REACTIONS 15N(polarized p, γ), E=8.69, 12.6, 14.5 MeV; measured σ(E;θ), A(θ). 16O deduced resonances, J, π.

doi: 10.1103/PhysRevLett.32.114
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1973CH35      Nucl.Phys. A212, 189 (1973)

C.C.Chang, H.F.Glavish, R.Avida, R.N.Boyd

Elastic Scattering of Vector Polarized Deuterons by 4He

NUCLEAR REACTIONS 4He(polarized d, d), E=11.5-17 MeV; measured vector analyzing power iT11(E, θ).

doi: 10.1016/0375-9474(73)90044-4
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1973GL01      Phys.Rev.Lett. 30, 391 (1973)

H.F.Glavish, R.Avida, S.S.Hanna, E.Diener, R.N.Boyd, C.C.Chang

Measurement of Multipole Mixing in Nuclear Radiation by a New Method

NUCLEAR REACTIONS 24Mg(polarized p, p'γ), E=8-10 MeV; measured Iγ(θ). 24Mg deduced γ-mixing. vector polarized beam.

doi: 10.1103/PhysRevLett.30.391
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1972AV01      Nucl.Phys. A182, 359 (1972)

R.Avida, I.Ben-Zvi, G.Goldring, S.S.Hanna, P.N.Tandon, Y.Wolfson

Magnetic Moment of the First Excited State of 10B

NUCLEAR REACTIONS 9Be(p, γγ), E=1.084 MeV, H= 17.6 kG; measured γγ(θ, H). 10B deduced g-factor 1+ first excited state.

doi: 10.1016/0375-9474(72)90283-7
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1972BO40      Phys.Rev.Lett. 29, 955 (1972)

R.N.Boyd, D.Slater, R.Avida, H.F.Glavish, C.Glashausser, G.Bissinger, S.Davis, C.F.Haynes, A.B.Robbins

Observation of Polarization-Analyzing Power Inequality in the Reaction 88Sr(p, p'γ)88Sr Using Polarized Protons

NUCLEAR REACTIONS 88Sr(p, p'γ), E=7.00, 7.08, 7.53 MeV; measured σ(θ), analyzing power(θ), spin-flip probability(θ). 89Y deduced isobaric analog resonance level-width, wave functions.

doi: 10.1103/PhysRevLett.29.955
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1972GL01      Phys.Rev.Lett. 28, 766 (1972)

H.F.Glavish, S.S.Hanna, R.Avida, R.N.Boyd, C.C.Chang, E.Diener

Giant Dipole Resonances in 12C Observed with the Polarized Proton Capture Reaction

NUCLEAR REACTIONS 11B(polarized p, γ), E=6-14 MeV; measured analyzing power(E;θ). 12C deduced giant E1 resonance configurations.

doi: 10.1103/PhysRevLett.28.766
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1972HA52      Phys.Lett. 40B, 631 (1972)

S.S.Hanna, H.F.Glavish, E.M.Diener, J.R.Calarco, C.C.Chang, R.Avida, R.N.Boyd

The Giant Dipole Resonance in 16O Observed with the Polarized Proton Capture Reaction

NUCLEAR REACTIONS 15N(polarized p, γ), E=7.4-15 MeV; measured σ(E), analyzing power(E;θ). 16O deduced giant E1 resonance structure.

doi: 10.1016/0370-2693(72)90614-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2680.

1971AV04      Nucl.Phys. A172, 113 (1971)

R.Avida, M.B.Goldberg, Y.Horowitz, K.-H.Speidel, Y.Wolfson

Angular Correlation Studies of Electromagnetic Transitions Following the 16O(tau, α)15O Reaction

NUCLEAR REACTIONS 16O(3He, αγ), E=9.55, 10.84 MeV; measured σ(Eα, Eγ, E(αγ)). 15O levels deduced γ-mixing.

doi: 10.1016/0375-9474(71)90119-9
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1970AV02      Nucl.Phys. A147, 200 (1970)

R.Avida, I.Ben Zvi, P.Gilad, M.B.Goldberg, G.Goldring, K.H.Speidel, A.Sprinzak

Angular Correlation Measurements on 191,193Ir Following Coulomb Excitation

NUCLEAR REACTIONS 191,193Ir(16O, 16O'γ), E = 40 MeV; measured σ(Eγ, θ(γ)). 191,193Ir levels deduced g, γ-mixing. Natural targets, Ge(Li) detectors.

doi: 10.1016/0375-9474(70)90522-1
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1969AV01      Nucl.Phys. A127, 412 (1969)

R.Avida, Y.Dar, P.Gilad, M.B.Goldberg, K.H.Speidel, Y.Wolfson

Lifetime Measurements Following Coulomb Excitation

NUCLEAR REACTIONS 158Gd, 160Gd, 164Dy, 170Er(16O, 16O'γ), E=30 MeV; measured 16O'γ-delay. 158Gd, 160Gd, 164Dy, 170Er levels deduced T1/2.

doi: 10.1016/0375-9474(69)90581-8
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1969AV03      Nucl.Phys. A135, 678 (1969)

R.Avida, M.B.Goldberg, G.Goldring, A.Sprinzak

Electromagnetic Moments of Transitions in 191Ir, 193Ir Following Coulomb Excitation

NUCLEAR REACTIONS 191,193Ir(16O, 16O'γ), E = 9-30 MeV; measured σ(E;Eγ). 191,193Ir levels deduced transition probabilities, branching ratios. Enriched, natural targets. Ge(Li) detector.

doi: 10.1016/0375-9474(69)90012-8
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1968AV01      Nucl.Phys. A114, 365 (1968)

R.Avida, J.Burde, A.Molchadzki, Z.Berant

The Excited States of 193Ir Populated by the Beta Decay of 193Os

RADIOACTIVITY 193Os [from 192Os(n, γ)]; measured Eγ, Iγ, I(ce), γγ-coin, γγ(θ). 193Ir deduced levels J, π, ICC. Enriched target. Ge(Li) detector.

doi: 10.1016/0375-9474(68)90360-6
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1968AV02      Nucl.Phys. A115, 405 (1968)

R.Avida, J.Burde, A.Molchadzki

Absolute Transition Probabilities in 193Ir

RADIOACTIVITY 193Os [from 192Os(n, γ)]; measured βce-, βγ-delay. 193Ir deduced levels, T1/2. Enriched target.

doi: 10.1016/0375-9474(68)90013-4
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1968AV03      Phys.Rev.Letters 21, 441 (1968)

R.Avida, J.Burde, A.Molchadzki

Core Excitation in Ir193

RADIOACTIVITY 193Os; measured γγ-delay. 193Ir levels deduced T1/2.

doi: 10.1103/PhysRevLett.21.441
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