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Search: Author = P.C.Simms

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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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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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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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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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1973SC02      Nucl.Phys. A199, 424 (1973)

J.S.Schweitzer, P.C.Simms

Energy-Dependent β-γ Circular Polarization and Nuclear Matrix Elements in ⁸⁴Rb

RADIOACTIVITY ⁸⁴Rb; measured βγ-circular polarization; deduced nuclear matrix elements.

doi: 10.1016/0375-9474(73)90559-9
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1973SC06      Nucl.Phys. A202, 602 (1973)

J.S.Schweitzer, P.C.Simms

Nuclear Matrix Elements in the First-Forbidden β-Decay of ¹²⁵Sb

RADIOACTIVITY ¹²⁵Sb measured nothing; ¹²⁵Te deduced nuclear matrix elements in β-decay.

doi: 10.1016/0375-9474(73)90646-5
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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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1973SM01      Nucl.Phys. A202, 409 (1973)

G.J.Smith, P.C.Simms

Centroid-Shift Measurement of the Mean Lifetimes of the 316 and 612 keV States of ¹⁹²Pt

RADIOACTIVITY ¹⁹²Ir; measured βγγ-coin. ¹⁹²Pt levels deduced T_1/2.

doi: 10.1016/0375-9474(73)90234-0
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1973SM07      Nucl.Phys. A211, 473 (1973)

H.A.Smith, Jr., J.S.Schweitzer, P.C.Simms

Nuclear Matrix Elements in the First-Forbidden β-Decays of ¹²²Sb and ¹²⁴Sb

RADIOACTIVITY ^122,124Sb; deduced β-decay, nuclear matrix elements.

doi: 10.1016/0375-9474(73)90437-5
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1972SC43      Nucl.Phys. A198, 481 (1972)

J.S.Schweitzer, P.C.Simms

A Comparison of Methods for Determining Nuclear Matrix Elements in First-Forbidden β-Decay

RADIOACTIVITY ¹⁹⁸Au; analyzed βγ(θ), βγ-CP, β-shape factor; deduced nuclear matrix elements.

doi: 10.1016/0375-9474(72)90703-8
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1971BO11      Phys.Rev. C3, 1168 (1971)

J.J.Bosken, D.E.Ohlms, P.C.Simms

Energy - Dependent Beta-Gamma Circular Polarization and Nuclear Matrix Elements of Rb⁸⁶

RADIOACTIVITY ⁸⁶Rb; measured βγ-CP(Eβ); deduced nuclear matrix elements.

doi: 10.1103/PhysRevC.3.1168
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1971SM03      Phys.Rev. C3, 2278 (1971)

H.A.Smith, P.C.Simms

Beta-Gamma Circular-Polarization Correlation and Nuclear Matrix Elements of As⁷⁶

RADIOACTIVITY ⁷⁶As; measured βγ-CP(Eβ); deduced nuclear matrix elements.

doi: 10.1103/PhysRevC.3.2278
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1970OH02      Phys.Rev. C1, 1803 (1970)

D.E.Ohlms, J.J.Bosken, P.C.Simms

Energy-Dependent Beta-Gamma Circular Polarization of La¹⁴⁰

RADIOACTIVITY ⁶⁰Co, ¹⁴⁰La; measured βγ-CP(Eβ); deduced β-decay matrix elements.

doi: 10.1103/PhysRevC.1.1803
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1970SM03      Phys.Rev. C1, 1809 (1970)

H.A.Smith, P.C.Simms

Beta-Decay Matrix Elements of La¹⁴⁰ and the Implications for Isobaric Analog States

RADIOACTIVITY ¹⁴⁰La; measured nothing; analyzed available data; deduced first-forbidden matrix elements, impurities in isobaric analog of ¹⁴⁰La ground state.

doi: 10.1103/PhysRevC.1.1809
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1970SM08      Nucl.Phys. A159, 143 (1970)

H.A.Smith, P.C.Simms

Nuclear Matrix Elements in the First Forbidden Beta Decay of ¹⁹⁸Au

RADIOACTIVITY ¹⁹⁸Au; calculated first-forbidden β-decay nuclear matrix elements.

doi: 10.1016/0375-9474(70)90032-1
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1969KU04      COO-1746-8

H.Kuhlman, P.C.Simms, G.Smith

NUCLEAR STRUCTURE ⁴⁶Sc; measured not abstracted; deduced nuclear properties.

1966SI01      Phys.Rev. 141, 1078 (1966)

R.M.Singru, P.C.Simms, R.M.Steffen

Nuclear Matrix Elements in the First-Forbidden 2.2-MeV β Transition of La¹⁴⁰

NUCLEAR STRUCTURE ¹⁴⁰La; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.141.1078
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1965SI09      Phys.Rev. 138, B777 (1965)

P.C.Simms, A.Namenson, T.H.Wei, C.S.Wu

Beta-Gamma Angular-Correlation Measurements on Rb⁸⁶ and Rb⁸⁴

NUCLEAR STRUCTURE ⁸⁶Rb, ⁸⁴Rb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.138.B777
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1965SI10      Phys.Rev. 138, B784 (1965)

P.C.Simms

Nuclear-Matrix Elements in First-Forbidden Beta Decay-Rb⁸⁶ and Rb⁸⁴

NUCLEAR STRUCTURE ⁸⁴Rb, ⁸⁶Rb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.138.B784
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1964SI12      CU(PNPL)-234, 40 (1964)

P.C.Simms

Beta-Gamma Angular Correlation Measurements

NUCLEAR STRUCTURE ¹²⁶I, ¹²⁴I, ⁷⁴As, ⁷⁶As, ⁸⁴Rb, ⁸⁶Rb; measured not abstracted; deduced nuclear properties.

1964WE04      Bull.Am.Phys.Soc. 9, No.4, 395, BC10 (1964)

T.H.Wei, P.C.Simms, C.S.Wu

β-γ Circular Polarization of ⁴⁶Sc

NUCLEAR STRUCTURE ⁴⁶Sc; measured not abstracted; deduced nuclear properties.

1963GA01      Bull.Am.Phys.Soc. 8, No.1, 73, VA1 (1963)

C.J.Gallagher, Jr., A.Namenson, P.C.Simms

Determination of J-Quantum Number of Lu^176m by a β-Branching Ratio Measurement

NUCLEAR STRUCTURE ¹⁷⁶Lu; measured not abstracted; deduced nuclear properties.

1963GA13      Nucl.Phys. 49, 443 (1963)

C.J.Gallagher, Jr., A.Namenson, P.C.Simms

A Measurement of the Beta-Branching Ratio of Lu^176m

NUCLEAR STRUCTURE ¹⁷⁶Lu; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90107-X
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1962SI01      Bull.Am.Phys.Soc. 7, No.1, 34 J5 (1962)

P.C.Simms, A.Namenson, C.S.Wu

Comparison of the Beta-Decay Matrix Elements of Rb⁸⁶ and Rb⁸⁴

NUCLEAR STRUCTURE ⁸⁶Rb, ⁸⁴Rb; measured not abstracted; deduced nuclear properties.

1961SI01      Phys.Rev. 121, 1169 (1961)

P.C.Simms, N.Benczer-Koller, C.S.Wu

New Application of Delayed Coincidence Techniques for Measuring Lifetimes of Excited Nuclear States - Ca⁴² and Sc⁴⁷

NUCLEAR STRUCTURE ¹⁹⁸Hg, ⁴⁷Sc, ⁴²K, ⁴²Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.121.1169
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1961SI17      Cu(Pnpl)-214, p.10 (1961)

P.C.Simms, A.Namenson, C.S.Wu

Energy Dependent Beta-Gamma Angular COrrelation in Rb⁸⁶ and Rb⁸⁴

NUCLEAR STRUCTURE ⁸⁴Rb, ⁸⁶Rb; measured not abstracted; deduced nuclear properties.

1960SI01      Phys.Rev. 118, 768 (1960)

P.C.Simms, R.M.Steffen

Beta-Gamma Angular Correlation Measurements on Au¹⁹⁸. II. Transverse Polarization of the Beta Particles

NUCLEAR STRUCTURE ¹⁹⁸Au; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.118.768
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1960SI05      Bull.Am.Phys.Soc. 5, No.6, 424, P3 (1960)

P.C.Simms, N.Koller, C.S.Wu

New Application of Delayed Coincidence Techniques for Measuring Lifetimes of Excited Nuclear States-Ca⁴² and Sc⁴⁷

NUCLEAR STRUCTURE ¹⁹⁸Hg, ⁴⁷Sc, ⁴²K, ⁴²Ca; measured not abstracted; deduced nuclear properties.

1960SI07      Cu(Pnpl)-205, 30 (1960)

P.C.Simms

NUCLEAR STRUCTURE ⁴²Ca, ⁴⁷Sc; measured not abstracted; deduced nuclear properties.

1958SI80      Phys.Rev.Letters 1, 289 (1958)

P.C.Simms, R.M.Steffen

β-γ Angular Correlation Experiments and Time-Reversal Invariance of the Beta Interaction

doi: 10.1103/PhysRevLett.1.289
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1957SI63      Phys.Rev. 108, 1459 (1957)

P.C.Simms, R.M.Steffen

Lifetime of the 247-keV Excited State of Cd¹¹¹

doi: 10.1103/PhysRev.108.1459
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