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NSR database version of April 27, 2024.

Search: Author = S.Penner

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1980CA07      Phys.Lett. 91B, 203 (1980)

L.S.Cardman, J.W.Lightbody, Jr., S.Penner, S.P.Fivozinsky, X.K.Maruyama, W.P.Trower, S.E.Williamson

The Charge Distribution of ¹²C

NUCLEAR REACTIONS ¹²C(e, e), E=25-115 MeV; measured absolute σ. ¹²C deduced ground-state charge distribution shape, rms charge radius.

doi: 10.1016/0370-2693(80)90431-1
Citations: PlumX Metrics

1979MA13      Phys.Rev. C19, 1624 (1979)

X.K.Maruyama, F.J.Kline, J.W.Lightbody, Jr., S.Penner, W.J.Briscoe, M.Lunnon, H.Crannell

Electroexcitation of ²²Ne below E = 8.6 MeV

NUCLEAR REACTIONS ²²Ne(e, e'), E=60-110 MeV; measured σ(E). ²²Ne levels deduced J, π, B(λ). Enriched ²²Ne target.

doi: 10.1103/PhysRevC.19.1624
Citations: PlumX Metrics

1978SZ02      Phys.Rev. C17, 435 (1978)

Z.M.Szalata, K.Itoh, G.A.Peterson, J.Flanz, S.P.Fivozinsky, F.J.Kline, J.W.Lightbody, Jr., X.E.Maruyama, S.Penner

Electroexcitation of ²⁰Ne Giant Electric-Dipole and -Quadrupole Resonances

NUCLEAR REACTIONS ²⁰Ne(e, e'), E=59.5-119.7 MeV; measured σ(E, θ). ²⁰Ne giant resonance region deduced dipole, quadrupole strength.

doi: 10.1103/PhysRevC.17.435
Citations: PlumX Metrics

1977FI09      Nucl.Phys. A290, 99 (1977)

J.M.Finn, H.Crannell, P.L.Hallowell, J.T.O'Brien, S.Penner

Inelastic Electron Scattering from Low-Lying States in the Nuclei ³⁶Ar And ⁴⁰Ar

NUCLEAR REACTIONS ^36,40Ar(e, e'), E=65-115 MeV; measured σ(E, θ). ^36,40Ar deduced levels, J, π, Γ. Enriched ³⁶Ar target.

doi: 10.1016/0375-9474(77)90668-6
Citations: PlumX Metrics

1977SZ02      Phys.Rev. C15, 1200 (1977)

Z.M.Szalata, J.M.Finn, J.Flanz, F.J.Kline, G.A.Peterson, J.W.Lightbody, Jr., X.K.Maruyama, S.Penner

Low-Momentum-Transfer Elastic Electron Scattering from ³He

NUCLEAR REACTIONS ³He(e, e), E=28.8-95.0 MeV; measured σ(E) at 75°. ³He deduced rms charge radius.

doi: 10.1103/PhysRevC.15.1200
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1976CO08      Phys.Rev. C13, 1083 (1976)

T.Cooper, W.Bertozzi, J.Heisenberg, S.Kowalski, W.Turchinetz, C.Williamson, L.Cardman, S.Fivozinsky, J.Lightbody, Jr., S.Penner

Shapes of Deformed Nuclei as Determined by Electron Scattering: ¹⁵²Sm, ¹⁵⁴Sm, ¹⁶⁶Er, ¹⁷⁶Yb, ²³²Th, and ²³⁸U

NUCLEAR REACTIONS ^152,154Sm, ¹⁶⁶Er, ¹⁷⁶Yb, ²³²Th, ²³⁸U(e, e'); measured σ(Ee'). ^152,154Sm, ¹⁶⁶Er, ¹⁷⁶Yb, ²³²Th, ²³⁸U deduced shape parameters.

doi: 10.1103/PhysRevC.13.1083
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1976FI12      Nucl.Phys. A274, 28 (1976)

J.M.Finn, H.Crannell, P.L.Hallowell, J.T.O'Brien, S.Penner

Elastic Electron Scattering from the Isotopes ³⁶Ar and ⁴⁰Ar

NUCLEAR REACTIONS ^36,40Ar(e, e'), E=65-115 MeV; measured σ(E, θ). ^36,40Ar deduced nuclear charge distributions. Enriched targets.

doi: 10.1016/0375-9474(76)90224-4
Citations: PlumX Metrics

1976LI19      Phys.Rev. C14, 952 (1976)

J.W.Lightbody, Jr., S.Penner, S.P.Fivozinsky, P.L.Hallowell, H.Crannell

Electron Scattering from Vibrational Nuclei

NUCLEAR REACTIONS ⁵²Cr, ¹¹⁰Pd, ¹¹⁴Cd, ¹¹⁶Sn(e, e), E=40-110 MeV; measured σ; deduced form factors. ¹¹⁰Pd, ¹¹⁴Cd, ¹¹⁶Sn deduced charge distribution parameters, B(λ), quadrupole moment.

doi: 10.1103/PhysRevC.14.952
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1976NE06      Nucl.Phys. A263, 249 (1976)

R.Neuhausen, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner

Electron Scattering Studies of Low-Lying Collective States of Even Zn Isotopes

NUCLEAR REACTIONS ^64,66,68,70Zn(e, e'), E=40-112 MeV; measured σ(E, Ee', θ). ^64,66,68,70Zn deduced B(E2), B(E3). Application of anharmonic vibrator model. Enriched targets.

doi: 10.1016/0375-9474(76)90171-8
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1975KA02      Phys.Rev. C11, 323 (1975)

P.T.Kan, G.A.Peterson, D.V.Webb, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electroexcitation of ¹¹B

NUCLEAR REACTIONS ¹¹B(e, e'), E=52.3-90 MeV; measured σ(E, Ee', θ). ¹¹B giant resonances, levels deduced B(E2), B(M1), form factors.

doi: 10.1103/PhysRevC.11.323
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1975KA04      Phys.Rev.Lett. 34, 899 (1975)

P.T.Kan, G.A.Peterson, D.V.Webb, Z.M.Szalata, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Observation of Electric Monopole Strength in the Electrodisintegration Of ³He

NUCLEAR REACTIONS ³He(e, e'), E=60, 75, 90, 110, 120 MeV; ⁴He(e, e'), E=elastic peak to breakup threshold; measured σ. ³He deduced E0 excitation.

doi: 10.1103/PhysRevLett.34.899
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1975KA28      Phys.Rev. C12, 1118 (1975)

P.T.Kan, G.A.Peterson, D.V.Webb, Z.M.Szalata, J.S.O'Connell, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electrodisintegration of ³He

NUCLEAR REACTIONS ³He(e, e'), E=60-120 MeV; measured σ(E, Ee', θ). ³He deduced form factors, strength functions.

doi: 10.1103/PhysRevC.12.1118
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1975KL03      Nucl.Phys. A241, 299 (1975)

F.J.Kline, C.L.Lin, G.A.Peterson, S.Penner

Inelastic Electron Scattering from ³¹P

NUCLEAR REACTIONS ³¹P(e, e'), E=49.6-110.6, 250 MeV; measured σ(E, Ee', θ). ³¹P levels deduced B(E2, omega), form factors. Natural ³¹P target.

doi: 10.1016/0375-9474(75)90319-X
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1974EN01      Phys.Rev. C9, 1705 (1974)

N.Ensslin, W.Bertozzi, S.Kowalski, C.P.Sargent, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electron Scattering from Excited States in ¹⁴N and ⁹Be

NUCLEAR REACTIONS ⁹Be, ¹⁴N(e, e'), E=117, 122 MeV; measured σ(Ee', θ). ⁹Be, ¹⁴N levels deduced form factors, B(EL), B(ML).

doi: 10.1103/PhysRevC.9.1705
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1974FI05      Phys.Rev. C9, 1533 (1974)

S.P.Fivozinsky, S.Penner, J.W.Lightbody, Jr., D.Blum

Electron Scattering from ⁸⁸Sr and ⁸⁹Y

NUCLEAR REACTIONS ⁸⁸Sr, ⁸⁹Y(e, e'), E=45-121 MeV; measured σ(E, θ), deduced form factors. ⁸⁸Sr, ⁸⁹Y levels deduced B(EL).

doi: 10.1103/PhysRevC.9.1533
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1974KL12      Nuovo Cim. 23A, 137 (1974)

F.J.Kline, H.Crannell, J.M.Finn, P.L.Hallowell, J.T.O'Brien, C.W.Werntz, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Search for the Lowest T = 2 State in ¹⁴C by Inelastic Electron Scattering

NUCLEAR REACTIONS ¹⁴C(e, e'), E=61, 81 MeV; measured σ(Ee'). ¹⁴C deduced upper limit for T=2 level.

doi: 10.1007/BF02748297
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1974OB01      Phys.Rev. C9, 1418 (1974)

J.T.O'Brien, H.Crannell, F.J.Kline, S.Penner

Ionization Loss for High-Energy Electrons in Thin Targets

NUCLEAR REACTIONS C, Al, Cu(e, e'), E=50, 100 MeV; measured most-probable energy loss for electrons.

doi: 10.1103/PhysRevC.9.1418
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1973CH16      Phys.Rev. C8, 23 (1973)

B.T.Chertok, C.Sheffield, J.W.Lightbody, Jr., S.Penner, D.Blum

Low-q² Electron Scattering from the 15.109-MeV State of ¹²C and the Conserved-Vector-Current Test

NUCLEAR REACTIONS ¹²C(e, e'), E=150 MeV; measured σ(Ee', θ). ¹²C deduced B(M1), γ-width.

doi: 10.1103/PhysRevC.8.23
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1973HA13      Phys.Rev. C7, 1396 (1973)

P.L.Hallowell, W.Bertozzi, J.Heisenberg, S.Kowalski, X.Maruyama, C.P.Sargent, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electron Scattering from ¹⁹F and ⁴⁰Ca

NUCLEAR REACTIONS ¹⁹F, ⁴⁰Ca(e, e), (e, e'), E=120 MeV; measured σ(Ee), form factors; ¹⁹F, ⁴⁰Ca deduced levels, charge radius, deformation parameters.

doi: 10.1103/PhysRevC.7.1396
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1973HE28      Proc.Int.Conf.Nuclear Physics, Munich, J.de Boer, H.J.Mang, Eds., North-Holland Publ.Co., Amsterdam, Vol.1, p.629 (1973)

J.Heisenberg, W.Bertozzi, T.Cooper, N.Ensslin, P.L.Hallowell, S.Kowalski, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Deformed Charge Distributions of Some Rotational Heavy Nuclei

NUCLEAR REACTIONS ¹⁶⁶Er, ¹⁷⁶Yb, ²³²Th, ²³⁸U(e, e), E=35-110 MeV; measured σ(θ). ¹⁶⁶Er, ¹⁷⁶Yb, ²³²Th, ²³⁸U deduced charge distribution.

1972BE26      Phys.Rev.Lett. 28, 1711 (1972)

W.Bertozzi, T.Cooper, N.Ensslin, J.Heisenberg, S.Kowalski, M.Mills, W.Turchinetz, C.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Deformation Parameters of ¹⁵²Sm by Electron Scattering

NUCLEAR REACTIONS ¹⁵²Sm(e, e'), E=50-105 MeV; measured σ(Ee'). ¹⁵²Sm deduced nuclear charge distribution, deformation parameters β(L).

doi: 10.1103/PhysRevLett.28.1711
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1972NE01      Phys.Rev. C5, 124 (1972)

R.Neuhausen, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner

Elastic Electron Scattering from Zn Isotopes

NUCLEAR REACTIONS ^64,66,68,70Zn(e, e), E=61-120 MeV; measured σ(E;θ). ^64,66,68,70Zn deduced rms radii, charge distribution parameters.

doi: 10.1103/PhysRevC.5.124
Citations: PlumX Metrics

1971RO20      Nucl.Phys. A173, 124 (1971)

E.F.Romberg, N.S.Wall, D.Blum, J.W.Lightbody, Jr., S.Penner

Elastic Scattering of 60-120 MeV Electrons from ^46,48,50Ti

NUCLEAR REACTIONS ^46,48,50Ti(e, e), E=60-120 MeV; measured σ(E;θ=127.50°). ^46,48,50Ti deduced relative charge density. Enriched targets.

doi: 10.1016/0375-9474(71)90751-2
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1970BE03      Phys.Rev.Lett. 24, 152 (1970)

J.C.Bergstrom, W.Bertozzi, S.Kowalski, X.K.Maruyama, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner

Electroexcitation of the Low-Lying States of O¹⁶

NUCLEAR REACTIONS ¹⁶O(e, e'), E=51-105 MeV; measured σ(E;E'); deduced inelastic form factors. ¹⁶O levels deduced deformation parameters.

doi: 10.1103/PhysRevLett.24.152
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1970LI02      Phys.Rev.Lett. 24, 274 (1970)

J.W.Lightbody, Jr., S.Penner

Electroexcitation of the C¹² Giant Resonance

NUCLEAR REACTIONS ¹²C(e, e'), E=52-102 MeV; measured σ(E;Ee', θ); deduced form factors. ¹²C deduced reduced matrix elements for giant resonance region.

doi: 10.1103/PhysRevLett.24.274
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1959PE22      Phys.Rev. 114, 1101 (1959)

S.Penner, J.E.Leiss

Photoproton Cross Sections of Carbon

doi: 10.1103/PhysRev.114.1101
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