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Search: Author = F.Rickey

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1998CR01      Phys.Rev. C57, 590 (1998)

B.Crowe, H.Aslan, T.Dague, D.G.Savage, S.Zeghib, F.A.Rickey, P.C.Simms

⁹⁹Tc Produced by the (³He, pnγ) Reaction

NUCLEAR REACTIONS ⁹⁸Mo(³He, np), E=13.5, 15, 16.5, 18 MeV; measured Eγ, Iγ, γγ-, pγ-coin. ⁹⁹Tc deduced levels, J, π, band structure. Nilsson model calculations. Other Tc isotopes compared.

doi: 10.1103/PhysRevC.57.590
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1997SA01      Phys.Rev. C55, 120 (1997)

D.G.Savage, H.Aslan, B.Crowe, T.Dague, S.Zeghib, F.A.Rickey, P.C.Simms

¹⁰¹Tc Produced by the (³He, pnγ) Reaction

NUCLEAR REACTIONS ¹⁰⁰Mo(³He, np), E=15-19.5 MeV; measured pγ-, γγ-coin, Iγ(θ), Eγ, γγ(θ). ¹⁰¹Tc deduced levels, J, π, δ. Symmetric rotor model.

doi: 10.1103/PhysRevC.55.120
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1996AS01      Phys.Rev. C54, 576 (1996)

H.Aslan, B.Crowe, T.Dague, D.G.Savage, S.Zeghib, F.A.Rickey, P.C.Simms

⁹⁷Tc Produced by the (³He, pnγ) Reaction

NUCLEAR REACTIONS ⁹⁶Mo(³He, np), E=18 MeV; measured pγ-, pγγ-coin, Eγ, Iγ, γ(θ). ⁹⁷Tc deduced levels, J, π.

doi: 10.1103/PhysRevC.54.576
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1988SA01      Phys.Rev. C37, 605 (1988)

G.S.Samudra, K.D.Carnes, F.A.Rickey, P.C.Simms, S.Zeghib

Non-Yrast States in Even-Even ⁹⁸Ru

NUCLEAR REACTIONS ⁹⁷Mo(³He, 2nγ), E=13 MeV; measured Eγ, Iγ, Iγ(θ), γ(θ), linear polarization, γγ(θ), γ yields, σ(Eγ, E). ⁹⁸Ru deduced levels, J, π, two-quasiparticle plus rotor model.

doi: 10.1103/PhysRevC.37.605
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1988WA03      Phys.Rev. C37, 613 (1988)

N.Wang, F.A.Rickey, G.S.Samudra, P.C.Simms, S.Zeghib

¹¹¹Cd from the (³He, 2nγ) Reaction and a Rotational Interpretation

NUCLEAR REACTIONS ¹¹⁰Pd(³He, 2nγ), E=13 MeV; measured Eγ, Iγ, Iγ(E), γ(θ), γγ-coin, σ(Eγ, E). ¹¹¹Cd deduced levels, J, π. Particle-rotor model.

doi: 10.1103/PhysRevC.37.613
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1987CA04      Phys.Rev. C35, 525 (1987)

K.D.Carnes, F.A.Rickey, G.S.Samudra, P.C.Simms

Particle-Core Multiplets in ⁹⁷Mo Populated via the (³He, 2nγ) Reaction

NUCLEAR STRUCTURE ⁹⁷Mo; calculated levels, γ-branching ratio. Particle plus symmetric rotor model.

NUCLEAR REACTIONS ⁹⁶Zr(³He, 2nγ), E=11 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, linear polarization, σ(Eγ, E). ⁹⁷Mo deduced levels, decay characteristics, γ-branching ratio, J, π. Enriched target, Ge(Li) detector. Particle plus symmetric rotor model.

doi: 10.1103/PhysRevC.35.525
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1987ZE04      Phys.Rev. C36, 939 (1987)

S.Zeghib, F.A.Rickey, G.S.Samudra, P.C.Simms, Ning Wang

¹¹¹Ag utilizing the (³He, pnγ) Reaction: A rotational nucleus with intermediate deformation

NUCLEAR STRUCTURE ¹¹¹Ag; calculated levels, γ-branching ratio. Particle-rotor model.

NUCLEAR REACTIONS ¹¹⁰Pd(³He, np), E=18 MeV; measured Eγ, Iγ(θ), σ(Eγ, E), γγ-coin. ¹¹¹Ag deduced levels, J, π, γ-branching ratio. Particle-rotor model.

doi: 10.1103/PhysRevC.36.939
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1986WH04      Phys.Rev. C34, 443 (1986)

C.S.Whisnant, K.D.Carnes, R.H.Castain, F.A.Rickey, G.S.Samudra, P.C.Simms

Levels in ⁹⁹Ru Populated by the (³He, 2nγ) Reaction: Complete particle-core multiplets

NUCLEAR REACTIONS ⁹⁸Mo(³He, 2nγ), E=13 MeV; measured Eγ, Iγ, σ(Eγ, E), γ(θ), γγ-coin, γ-linear polarization. ⁹⁹Ru deduced levels, J, π, γ-branching, ratio, δ. Particle-rotor model.

doi: 10.1103/PhysRevC.34.443
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1986ZE02      Phys.Rev. C34, 1451 (1986)

S.Zeghib, F.A.Rickey, P.C.Simms

Interpretation of States in ¹⁰⁵Ag utilizing a Particle-Rotor Model

NUCLEAR STRUCTURE ¹⁰⁵Ag; calculated levels, J, π, γ-branching ratios. Particle-rotor model.

doi: 10.1103/PhysRevC.34.1451
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1983WH01      Phys.Rev.Lett. 50, 724 (1983)

C.S.Whisnant, R.H.Castain, F.A.Rickey, P.C.Simms

Complete Particle-Core Multiplets Populated in ⁹⁹Ru by the (³He, 2nγ) Reaction

NUCLEAR REACTIONS ⁹⁸Mo(³He, 2nγ), E=13 MeV; measured γ(θ), γγ-coin, linear polarization, γγ(θ), oriented nuclei. ⁹⁹Ru deduced levels, J, π, γ-branching. Particle-rotor model.

doi: 10.1103/PhysRevLett.50.724
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1981DE03      Phys.Rev. C23, 213 (1981); Erratum Phys.Rev. C23, 2380 (1981)

A.P.de Lima, A.V.Ramayya, J.H.Hamilton, B.Van Nooijen, R.M.Ronningen, H.Kawakami, R.B.Piercey, E.de Lima, R.L.Robinson, H.J.Kim, L.K.Peker, F.A.Rickey, R.Popli, A.J.Caffrey, J.C.Wells

Multiple Band Structures in ⁶⁸Ge

NUCLEAR REACTIONS ⁵⁸Ni(¹²C, 2p), E=39 MeV; ⁶³Cu(⁷Li, 2n), E=18 MeV; ⁵²Cr(¹⁹F, 2np), E=50 MeV; measured Eγ, Iγ, γ(θ), γγ(θ), oriented nuclei, DSA, linear polarization. ⁶⁸Ge deduced levels, J, π, δ, T_1/2, rotational band structure. Interacting boson, rotation-aligned models.

doi: 10.1103/PhysRevC.23.213
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1981PO06      Phys.Rev. C23, 1085 (1981)

R.Popli, F.A.Rickey, L.E.Samuelson, P.C.Simms

High-Angular-Momentum States in ¹⁰⁶Ag and Their Rotational Interpretation

NUCLEAR STRUCTURE ¹⁰⁶Ag; calculated levels, T_1/2, B(λ), γ-branching ratios, δ. Two-particle plus rotor model, Coriolis, recoil effects, variable moment of inertia.

NUCLEAR REACTIONS ⁹⁶Zr(¹⁴N, 4n), E=49 MeV; measured σ(Eγ), Iγ(θ), γγ-coin, γγ(θ), oriented nuclei, linear polarization, Eγ, Iγ. ¹⁰⁶Ag deduced levels, J, π, γ-mixing ratios. Ge(Li) detectors. Two-particle plus rotor model.

doi: 10.1103/PhysRevC.23.1085
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1980PO06      Phys.Rev. C22, 1121 (1980)

R.Popli, F.A.Rickey, P.C.Simms

Non-yrast States in ¹⁰¹Pd and Their Rotational Interpretation

NUCLEAR REACTIONS ⁹²Zr(¹²C, 3n), E=48 MeV; measured Iγ(θ), γγ-coin, γγ(θ), oriented nuclei. ¹⁰¹Pd deduced levels, J, π, δ, γ-branching ratios. Rotational model.

doi: 10.1103/PhysRevC.22.1121
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1979DE12      Phys.Lett. 83B, 43 (1979)

A.P.de Lima, J.H.Hamilton, A.V.Ramayya, B.van Nooijen, R.M.Ronningen, H.Kawakami, R.B.Piercey, E.de Lima, R.L.Robinson, H.J.Kim, W.K.Tuttle, L.K.Peker, F.A.Rickey, R.Popli

Evidence for Ground and Both Neutron and Proton Rotational Aligned Bands in ⁶⁸Ge

NUCLEAR REACTIONS ⁵⁸Ni(¹²C, 2pγ), E=39 MeV; measured γ(θ), γγ-coin, T_1/2. ⁶³Cu(⁷Li, 2nγ), E=26 MeV; measured γ(θ). ⁶⁸Ge deduced levels, branching of yrast band. Rotational aligned model calculations.

doi: 10.1016/0370-2693(79)90884-0
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1979PO13      Phys.Rev. C20, 1350 (1979)

R.Popli, J.A.Grau, S.I.Popik, L.E.Samuelson, F.A.Rickey, P.C.Simms

States in ^105,107Ag Populated by Heavy-Ion Reactions and Interpreted by a Quasiparticle-Plus-Rotor Model

NUCLEAR REACTIONS ⁹²Zr(¹⁶O, 2np), E=60 MeV; ⁹⁶Zr(¹⁴N, 3n), E=49 MeV; measured Iγ, Iγ(θ), γγ-coin, γγ(θ). ^105,107Ag deduced levels, J, π, δ ratios. Rotational model, Coriolis calculations. Ge(Li) detectors, oriented nuclei.

doi: 10.1103/PhysRevC.20.1350
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1979SA01      Phys.Rev. C19, 73 (1979)

L.E.Samuelson, J.A.Grau, S.I.Popik, F.A.Rickey, P.C.Simms

States in ¹⁰⁶Cd Populated by Heavy-Ion (xn) Reactions Interpreted by A Two-Quasiparticle-Plus-Rotor Model

NUCLEAR REACTIONS ⁹⁶Mo(¹³C, 3nγ), ⁹⁷Mo(¹²C, 3nγ), E=45 MeV; ⁹⁴Zr(¹⁶O, 4nγ), E=63 MeV; measured Iγ, Iγ(θ), γ-linear polarization, γγ-coin, γγ(θ), oriented nuclei. ¹⁰⁶Cd deduced levels, J, π, γ-multipolarity. Rotational model calculations. Enriched targets.

doi: 10.1103/PhysRevC.19.73
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1978SA13      Nucl.Phys. A301, 159 (1978)

L.E.Samuelson, F.A.Rickey, J.A.Grau, S.I.Popik, P.C.Simms

Levels of ¹⁰⁸Cd Populated in the ⁹⁶Zr(¹⁶O, 4nγ)¹⁰⁸Cd Reaction

NUCLEAR REACTIONS ⁹⁶Zr(¹⁶O, 4nγ), E=56 MeV; measured Iγ(E, θ), pγ, γγ-coin, γγ DCO. ¹⁰⁸Cd deduced levels, J, π, γ-multipolarity.

doi: 10.1016/0375-9474(78)90135-5
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1978ST01      Phys.Rev. C17, 143 (1978)

D.C.Stromswold, D.O.Elliott, Y.K.Lee, L.E.Samuelson, J.A.Grau, F.A.Rickey, P.C.Simms

Parity Determinations in ^105-109Cd from Linearly Polarized Gamma Rays Following (¹⁶O, xn) Reactions

NUCLEAR REACTIONS ⁹²Zr(¹⁶O, 3nγ), E=58 MeV; ⁹⁴Zr(¹⁶O, 4nγ), E=63 MeV; ⁹⁴Zr(¹⁶O, 3nγ), E=59 MeV; ⁹⁶Zr(¹⁶O, 4nγ), (¹⁶O, 3nγ), E=56 MeV; measured linear polarization, Eγ, Iγ, γ(θ). ^{105,106,107,108,109}Cd deduced levels, J, π, λ, δ.

doi: 10.1103/PhysRevC.17.143
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1977RI05      Phys.Rev. C15, 1530 (1977)

F.A.Rickey, J.A.Grau, L.E.Samuelson, P.C.Simms

Observation and Analysis of Particle-Core Multiplets in ¹⁰⁵Pd

NUCLEAR REACTIONS ⁹⁶Zr(¹²C, 3nγ), E=45 MeV; measured Eγ, Iγ(θ), γγ(θ, H). ¹⁰⁵Pd deduced levels, K, J, π, λ, δ.

doi: 10.1103/PhysRevC.15.1530
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1976GR12      Phys.Rev. C14, 2297 (1976)

J.A.Grau, L.E.Samuelson, F.A.Rickey, P.C.Simms, G.J.Smith

Collective and Two-Quasiparticle Excitations in ^102,104,106Pd Following (¹³C, 3nγ) Reactions

NUCLEAR REACTIONS ^92,94,96Zr(¹³C, 3nγ), E=45-56 MeV; measured Iγ(E, θ), γγ-coin, linear polarization, γγ(θ) from oriented nuclei. ^102,104,106Pd deduced levels, K, J, π, λ, δ.

doi: 10.1103/PhysRevC.14.2297
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1976SM06      Phys.Rev. C14, 1946 (1976)

H.A.Smith, Jr., F.A.Rickey

Particle-Core Coupling in ^101-105Pd: The Rotational Model at Intermediate Deformation

NUCLEAR STRUCTURE ^101,103,105Pd; calculated energy levels, B(λ), S, γ-branching. Nilsson model, Coriolis coupling, variable moment of inertia.

doi: 10.1103/PhysRevC.14.1946
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1976ST03      Phys.Rev. C13, 1510 (1976)

D.C.Stromswold, D.O.Elliott, Y.K.Lee, J.A.Grau, L.E.Samuelson, F.A.Rickey, P.C.Simms

Linear Polarization Measurements on Gamma Rays from ¹⁰⁴Pb and ¹⁰⁶Pd

NUCLEAR REACTIONS ⁹⁴Zr(¹³C, 3n), E=47 MeV; ⁹⁶Zr(¹³C, 3n), E=42 MeV; measured linear polarization. ^104,106Pd levels deduced π, λ.

doi: 10.1103/PhysRevC.13.1510
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1975KI13      Phys.Rev. C12, 499 (1975)

J.S.Kim, Y.K.Lee, K.A.Hardy, P.C.Simms, J.A.Grau, G.J.Smith, F.A.Rickey

Gamma-Ray Linear Polarization Measurements Following Heavy-Ion Bombardment of Odd Isotopes of Pd

NUCLEAR REACTIONS ^90,92,94Zr(¹²C, 3nγ), E=48-56 MeV; measured linear polarization (θ). ^99,101,103Pd levels deduced K, J, π, λ, δ.

doi: 10.1103/PhysRevC.12.499
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1974GR04      Phys.Rev.Lett. 32, 677 (1974)

J.A.Grau, Z.W.Grabowski, F.A.Rickey, P.C.Simms, R.M.Steffen

Measurements of Directional Correlation from Oriented Nuclei (DCO) and the Band Structure in ¹⁰²Pd

NUCLEAR REACTIONS ⁹²Zr(¹³C, 3nγ), E=51 MeV; measured γγ(θ). ¹⁰²Pd deduced γ-mixing, J, π.

doi: 10.1103/PhysRevLett.32.677
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1974GR07      Nucl.Phys. A229, 346 (1974)

J.A.Grau, F.A.Rickey, G.J.Smith, P.C.Simms, J.R.Tesmer

The Collective Excitation of ¹⁰³Pd Following (Heavy Ion, xn) Reactions

NUCLEAR REACTIONS ¹⁰⁰Ru(α, nγ), E=16-24 MeV; ⁹⁴Zr(¹²C, 3nγ), E=44-54 MeV; measured σ(Eα, Eγ), σ(E(¹²C), Eγ), σ(Eγ, θ), γγ-coin, pγ. ¹⁰³Pd deduced levels, J, π, T_1/2, γ-multipolarity.

doi: 10.1016/0375-9474(74)90792-1
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1974SI02      Phys.Rev. C9, 684 (1974)

P.C.Simms, G.J.Smith, F.A.Rickey, J.A.Grau, J.R.Tesmer, R.M.Steffen

Collective Excitation of ¹⁰¹Pd Following (Heavy Ion, xn) Reactions

NUCLEAR REACTIONS ⁹⁹Ru(α, 2nγ), E=16-24 MeV; ⁹²Zr(¹²C, 3nγ), E=45-56 MeV; ⁸⁸Sr(¹⁶O, 3nγ), E=56-64 MeV; measured σ(E)γ, γ-γcoin, σ(θ)γ, linear p; ¹⁰¹Pd deduced levels, J, π.

doi: 10.1103/PhysRevC.9.684
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1973RI10      Phys.Rev.Lett. 31, 404 (1973)

F.A.Rickey, P.C.Simms

Systematic Behavior of Quasirotational Bands in Odd-A Pd Nuclei

NUCLEAR REACTIONS ^100,101,102Ru(α, xnγ), ^94,96Zr(¹²C, 3nγ), E=47 MeV; measured Eγ, Iγ(θ), γγ-coin. ^101,103,105Pd deduced levels, J, π.

doi: 10.1103/PhysRevLett.31.404
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1973SI07      Phys.Rev.Lett. 30, 710 (1973)

P.C.Simms, F.A.Rickey, J.R.Tesmer

Evidence for Well-Developed Band Structure in ¹⁰¹Pd

NUCLEAR REACTIONS ⁹⁹Ru(α, 2nγ), ⁹²Zr(¹²C, 3nγ), ⁸⁸Sr(¹⁶O, 3nγ), E(¹⁶O)=56 MeV; measured σ(E), Eγ, Iγ, γ(θ), γγ-coin. ¹⁰¹Pd deduced levels, J, π, ±.

doi: 10.1103/PhysRevLett.30.710
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1973SI09      Phys.Rev. C7, 1631 (1973)

P.C.Simms, R.Anderson, F.A.Rickey, G.Smith, R.M.Steffen, J.R.Tesmer

Level Structure of ¹⁰²Pd Investigated by (α, xn;γ) Reactions

NUCLEAR REACTIONS ⁹⁹Ru(α, nγ), E=16-20 MeV; measured Eγ, Iγ, γγ-coin, Iγ(θ). ¹⁰²Pd deduced levels, J, π.

doi: 10.1103/PhysRevC.7.1631
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1972RI08      Phys.Rev. C5, 2072 (1972)

F.A.Rickey, E.T.Jurney, H.C.Britt

Level Scheme of ²³⁵U and the Distribution of Single-Particle Strength in its Excited States

NUCLEAR REACTIONS ²³⁴U(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. ²³⁴U(d, p), E=20 MeV; measured σ(Ep, θ). ²³³U(t, p), E=20 MeV; measured σ(Ep). ²³⁵U(d, d'), E=20 MeV; measured σ(Ed'). ²³⁶U(d, t), E=20 MeV; measured σ(Et). ²³⁵U deduced levels, J, π, L.

doi: 10.1103/PhysRevC.5.2072
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1968AL09      Phys.Letters 27B, 11 (1968)

D.L.Allan, H.C.Britt, F.A.Rickey, Jr.

Analogue States and the Nuclear Structure of ¹⁸¹Hf

NUCLEAR STRUCTURE ¹⁸¹Ta; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90319-5
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1968BR32      Phys.Rev. 175, 1525 (1969)

H.C.Britt, F.A.Rickey, Jr., W.S.Hall

Characteristics of the Transition-State Spectra for ²³⁴U, ²³⁶U, and ²⁴⁰Pu from (d, pf) and (t, pf) Angular-Correlation Experiments

NUCLEAR REACTIONS ^233,235U, ²³⁹Pu(d, pF), E = 15, 18 MeV; ²³⁴U(t, pF), E = 18 MeV; measured σ(Ep, θ(fragment)). ^234,236U, ²⁴⁰Pu deduced vibrational bands. ²³⁶U, ²⁴⁰Pu deduced pairing energy gap.

doi: 10.1103/PhysRev.175.1525
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1968RI07      Phys.Rev. 170, 1157 (1968)

F.A.Rickey, Jr., R.K.Sheline

Analysis of the Nuclear Reaction Spectroscopy of ¹⁷⁷Hf, ¹⁷⁹Hf, and ¹⁸¹Hf

NUCLEAR STRUCTURE ¹⁷⁷Hf, ¹⁷⁹Hf, ¹⁸¹Hf; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.170.1157
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1967MO25      Phys.Rev. 164, 1559 (1967)

C.F.Moore, J.G.Kulleck, P.Von Brentano, F.Rickey

Neutron Particle Hole Structure in ²⁰⁸Pb

NUCLEAR STRUCTURE ²⁰⁸Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1559
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1967RI12      Bull.Am.Phys.Soc. 12, No.4, 522, EF8 (1967); Priv.Comm. (1970)

F.A.Rickey, Jr., H.C.Britt

Levels in ²³⁵U Excited by (d, p), (d, t), and (t, p) Reactions

NUCLEAR STRUCTURE ²³⁵U; measured not abstracted; deduced nuclear properties.

1966RI10      Phys.Rev.Letters 17, 1057 (1966)

F.A.Rickey, Jr., R.K.Sheline

Experimental Exploration of the Limits of the Nilsson Model; Vibrational States in Hf¹⁷⁷ and Hf¹⁸¹

NUCLEAR STRUCTURE ¹⁸¹Hf, ¹⁷⁷Hf; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.17.1057
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Note: The following list of authors and aliases matches the search parameter F.Rickey: , F.A.RICKEY