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NSR database version of April 11, 2024.

Search: Author = K.A.Snover

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2011AD03      Rev.Mod.Phys. 83, 195 (2011)

E.G.Adelberger, A.Garcia, R.G.H.Robertson, K.A.Snover, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, D.Bemmerer, A.Junghans, D.Bemmerer, A.Junghans, C.A.Bertulani, K.-W.Chen, H.Costantini, P.Prati, M.Couder, E.Uberseder, M.Wiescher, R.Cyburt, B.Davids, S.J.Freedman, M.Gai, D.Gazit, L.Gialanella, G.Imbriani, U.Greife, M.Hass, W.C.Haxton, T.Itahashi, K.Kubodera, K.Langanke, D.Leitner, M.Leitner, P.Vetter, L.Winslow, L.E.Marcucci, T.Motobayashi, A.Mukhamedzhanov, R.E.Tribble, F.M.Nunes, T.-S.Park, R.Schiavilla, E.C.Simpson, C.Spitaleri, F.Strieder, H.-P.Trautvetter, K.Suemmerer, S.Typel

Solar fusion cross sections. II. The pp chain and CNO cycles

NUCLEAR REACTIONS 2H(p, γ), 3He(3He, 2p), (α, γ), (p, e), 7Be, 12C, 14N, 15N, 17O(p, γ), 15N, 16,17,18O(p, α), E<3 MeV; analyzed and evaluated experimental data; deduced recommended values and uncertainties.

doi: 10.1103/RevModPhys.83.195
Citations: PlumX Metrics


2011SA12      Phys.Rev. C 83, 034611 (2011)

A.L.Sallaska, C.Wrede, A.Garcia, D.W.Storm, T.A.D.Brown, C.Ruiz, K.A.Snover, D.F.Ottewell, L.Buchmann, C.Vockenhuber, D.A.Hutcheon, J.A.Caggiano, J.Jose

Absolute determination of the 22Na( p, γ )23Mg reaction rate in novae

NUCLEAR REACTIONS 22Na(p, γ), E=150-700 keV; measured Eγ, Iγ; deduced absolute yields, excitation functions for resonances, resonance strengths and thermonuclear reaction rates. 23Mg; deduced levels, J, π, branching ratios, resonances. Estimated flux of 22Na gamma rays from novae.

doi: 10.1103/PhysRevC.83.034611
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1827. Data from this article have been entered in the XUNDL database. For more information, click here.


2010JU01      Phys.Rev. C 81, 012801 (2010)

A.R.Junghans, K.A.Snover, E.C.Mohrmann, E.G.Adelberger, L.Buchmann

Updated S factors for the 7Be(p, γ)8B reaction

NUCLEAR REACTIONS 7Be(p, γ)8B, E(cm)=0-2500 keV; analyzed previous data for σ using detailed target analysis and improved stopping powers; deduced updated astrophysical S-factors.

doi: 10.1103/PhysRevC.81.012801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


2010SA26      Phys.Rev.Lett. 105, 152501 (2010)

A.L.Sallaska, C.Wrede, A.Garcia, D.W.Storm, T.A.D.Brown, C.Ruiz, K.A.Snover, D.F.Ottewell, L.Buchmann, C.Vockenhuber, D.A.Hutcheon, J.A.Caggiano

Direct Measurements of 22Na(p, γ)23Mg Resonances and Consequences for 22Na Production in Classical Novae

NUCLEAR REACTIONS 22Na(p, γ), E not given; measured Eγ, Iγ; deduced proton resonances energies and strengths, σ, reaction rates.

doi: 10.1103/PhysRevLett.105.152501
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1816. Data from this article have been entered in the XUNDL database. For more information, click here.


2007BA41      Phys.Rev. C 75, 058801 (2007)

G.Baur, K.A.Snover, S.Typel

E0 emission in α + 12C fusion at astrophysical energies

NUCLEAR REACTIONS 12C(α, γ), E(cm)< 1.5 MeV; calculated the contribution of E0 emission compared to E1 and E2 emissions.

doi: 10.1103/PhysRevC.75.058801
Citations: PlumX Metrics


2007BR32      Phys.Rev. C 76, 055801 (2007)

T.A.D.Brown, C.Bordeanu, K.A.Snover, D.W.Storm, D.Melconian, A.L.Sallaska, S.K.L.Sjue, S.Triambak

3He+4He → 7Be astrophysical S factor

NUCLEAR REACTIONS 3He(α, γ)7Be, E(cm)=0.33-1.23 MeV; measured Eγ, Iγ, cross sections; deduced astrophysical S-factors.

doi: 10.1103/PhysRevC.76.055801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1610.


2005ES02      Phys.Rev.Lett. 94, 042502 (2005)

H.Esbensen, G.F.Bertsch, K.A.Snover

Reconciling Coulomb Dissociation and Radiative Capture Measurements

NUCLEAR REACTIONS Pb(8B, p7Be), E=51.9 MeV/nucleon; calculated relative energy spectra, angular distributions. 7Be(p, γ), E=low; analyzed astrophysical S-factor data.

doi: 10.1103/PhysRevLett.94.042502
Citations: PlumX Metrics


2005JU03      Nucl.Phys. B(Proc.Supp.) S138, 112 (2005)

A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.R.Buchmann, A.Laird, S.Park, A.Y.Zyuzin

The new Seattle-TRIUMF 7Be(p, γ)8B S-factor determination

NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460 MeV; measured σ; deduced astrophysical S-factors. Comparison with previous results.

doi: 10.1016/j.nuclphysbps.2004.11.028
Citations: PlumX Metrics


2005SN03      Nucl.Phys. A758, 685c (2005)

K.A.Snover, A.R.Junghans, E.C.Mohrmann, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin, A.M.Laird

The 7Be(p, γ)8B astrophysical S-factor

doi: 10.1016/j.nuclphysa.2005.05.122
Citations: PlumX Metrics


2004JU08      Nucl.Phys. A746, 210c (2004)

A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.R.Buchmann, A.M.Laird, S.Park, A.Y.Zyuzin

New determination of the 7Be(p, γ)8B S-factor

NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460 MeV; measured σ; deduced astrophysical S-factors. Comparison with previous results.

doi: 10.1016/j.nuclphysa.2004.09.035
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


2003HE03      Phys.Lett. B 555, 43 (2003)

P.Heckman, D.Bazin, J.R.Beene, Y.Blumenfeld, M.J.Chromik, M.L.Halbert, J.F.Liang, E.Mohrmann, T.Nakamura, A.Navin, B.M.Sherrill, K.A.Snover, M.Thoennessen, E.Tryggestad, R.L.Varner

Low-temperature measurement of the giant dipole resonance width

NUCLEAR REACTIONS 120Sn(17O, 17O'), E=80 MeV/nucleon; measured particle spectra, Eγ, Iγ, (particle)γ-coin. 120Sn deduced width of GDR built on excited states, influence of thermal shape fluctuations. Comparison with model predictions.

doi: 10.1016/S0370-2693(03)00017-0
Citations: PlumX Metrics


2003JU04      Phys.Rev. C 68, 065803 (2003)

A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin, A.M.Laird

Precise measurement of the 7Be(p, γ)8B S factor

NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460; measured σ; deduced astrophysical S-factors. Comparison with previous results.

doi: 10.1103/PhysRevC.68.065803
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


2003PA33      Nucl.Phys. A718, 113c (2003)

S.H.Park, A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, A.Zyuzin, A.Laird

A new measurement of 7Be(p, γ)8B cross section and its astrophysical meaning

NUCLEAR REACTIONS 7Be(p, γ), E=221, 1379 keV; measured σ; deduced astrophysical S-factor.

doi: 10.1016/S0375-9474(03)00687-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1479.


2003SN01      Phys.Rev. C 67, 055801 (2003)

K.A.Snover, A.E.Hurd

Is e+e-pair emission important in the determination of the 3He+4He S factor?

NUCLEAR REACTIONS 4He(3He, X)7Be, E(cm) ≈ 0-3 MeV; calculated E0 and E1 pair emission and internal conversion contributions to capture σ.

doi: 10.1103/PhysRevC.67.055801
Citations: PlumX Metrics


2002JU01      Phys.Rev.Lett. 88, 041101 (2002)

A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin

7Be(p, γ)8B Astrophysical S Factor from Precision Cross Section Measurements

NUCLEAR REACTIONS 7Be(p, γ), E(cm)=186-1200 keV; measured σ; deduced astrophysical S-factor.

doi: 10.1103/PhysRevLett.88.041101
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


2001HE17      Nucl.Phys. A687, 225c (2001)

P.Heckman, D.Bazin, J.R.Beene, Y.Blumenfeld, M.J.Chromik, M.L.Halbert, J.F.Liang, E.Mohrmann, T.Nakamura, A.Navin, B.M.Sherrill, K.A.Snover, M.Thoennessen, E.Tryggestad, R.L.Varner

Temperature Dependence of the GDR Width in 120Sn

NUCLEAR REACTIONS 120Sn(17O, 17O'), E=80 MeV/nucleon; measured Eγ, (recoil)γ-coin, excitation energy spectra, preliminary GDR parameters. Comparison with α-induced reaction data.

doi: 10.1016/S0375-9474(01)00625-X
Citations: PlumX Metrics


2001KI07      Acta Phys.Pol. B32, 825 (2001)

M.Kicinska-Habior, Z.Trznadel, M.P.Kelly, J.P.S.van Schagen, K.A.Snover

Giant Dipole Resonance Studied in Heavy-Ion Reactions at Projectile Energies 6-11 MeV/u


2001KU10      Nucl.Phys. A687, 212c (2001)

D.Kusnezov, Y.Alhassid, K.A.Snover, W.E.Ormand

Giant Dipole Resonances in Hot, Rotating Nuclei: Nuclear shapes and shell corrections

NUCLEAR STRUCTURE Sc, Cu, Zr, Mo, Sn, Dy, Pb; calculated GDR width vs temperature and angular momentum. 92,96,100Mo; calculated GDR width as a function of temperature and angular momentum. 44Ti, 90Zr, 120Sn, 168Er, 208Pb; calculated deformation parameters vs temperature and spin for hot rotating nuclei. Shell effects discussed, comparison with data.

doi: 10.1016/S0375-9474(01)00623-6
Citations: PlumX Metrics


2001SN01      Nucl.Phys. A687, 337c (2001)

K.A.Snover

The Giant Dipole Resonance Strength and Width at High Temperature

NUCLEAR REACTIONS 90Zr(36Ar, X), E not given; calculated compound nucleus γ multiplicities vs excitation energy, GDR widths and GDR inhibition factor. Statistical Model, equilibration times discussed.

doi: 10.1016/S0375-9474(01)00640-6
Citations: PlumX Metrics


2001TR09      Nucl.Phys. A687, 198c (2001)

Z.Trznadel, M.Kicinska-Habior, M.P.Kelly, J.P.S.van Schagen, K.A.Snover

Giant Dipole Resonance in Hot Se Nuclei and Bremsstrahlung Emission in 12C + 58, 64Ni Experiments at 6-11 MeV/u

NUCLEAR REACTIONS 58,64Ni(12C, X), E=5.5-11 MeV/nucleon; measured Eγ, Iγ(θ), γγ-coin. 70Se, 76Se deduced GDR parameters. Statistical model calculations including precompound effects.

doi: 10.1016/S0375-9474(01)00621-2
Citations: PlumX Metrics


2000KI16      Acta Phys.Pol. B31, 423 (2000)

M.Kicinska-Habior, K.A.Snover, J.A.Behr, Z.M.Drebi, O.Kijewska

Bremsstrahlung Radiation in Heavy-Ion Collisions 18O + 27Al → 45Sc at 8.3 MeV/u

NUCLEAR REACTIONS 27Al(18O, X), E=8.3 MeV/nucleon; measured Eγ, Iγ(θ). 45Sc deduced GDR parameters. Transport model calculations.


1999KE02      Phys.Rev.Lett. 82, 3404 (1999)

M.P.Kelly, K.A.Snover, J.P.S.van Schagen, M.Kicinska-Habior, Z.Trznadel

Giant Dipole Resonance in Highly Excited Nuclei: Does the width saturate ?

NUCLEAR REACTIONS 100Mo(18O, X), E=122-214 MeV; measured Eγ, Iγ(θ), proton-, α-spectra; deduced pre-equilibrium emission features. 118Sn deduced GDR parameters, no saturation of width.

doi: 10.1103/PhysRevLett.82.3404
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1999KE06      Nucl.Phys. A649, 123c (1999)

M.P.Kelly, K.A.Snover, J.P.S.van Schagen, M.Kicinska-Habior, Z.Trznadel

The GDR Width in Hot Sn Nuclei

NUCLEAR REACTIONS 100Mo(18O, xnypzα), E=125, 150, 169, 200, 217 MeV; measured Eγ, Iγ(θ), γ multiplicity, (charged particle)γ-coin; deduced GDR width vs temperature.

doi: 10.1016/S0375-9474(99)00049-4
Citations: PlumX Metrics


1999KI14      Nucl.Phys. A649, 130c (1999)

M.Kicinska-Habior, Z.Trznadel, A.Maj, M.P.Kelley, J.P.S.van Schagen, K.A.Snover

Giant Dipole Resonances Decay and Bremsstrahlung Emission as a Source of High Energy γ-Rays in 12C + 24, 26Mg and 12C + 58, 64Ni Reactions at 6-11 MeV/u

NUCLEAR REACTIONS 24,26Mg, 58,64Ni(12C, X), E=6-11 MeV/nucleon; measured Eγ, Iγ(θ); deduced GDR, bremsstrahlung parameters.

doi: 10.1016/S0375-9474(99)00050-0
Citations: PlumX Metrics


1999KU14      Nucl.Phys. A649, 193c (1999)

D.Kusnezov, Y.Alhassid, K.A.Snover

Systematics of the Nuclear Giant Dipole Resonance

NUCLEAR STRUCTURE A=45-208; analyzed GDR widths vs temperature, spin, mass; deduced phenomenological function. Liquid drop, Nilsson-Strutinsky approaches.

doi: 10.1016/S0375-9474(99)00059-7
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1998AD12      Rev.Mod.Phys. 70, 1265 (1998)

E.G.Adelberger, S.M.Austin, J.B.Bahcall, A.B.Balantekin, G.Bogaert, L.S.Brown, L.Buchmann, F.E.Cecil, A.E.Champagne, L.de Braeckeleer, C.A.Duba, S.R.Elliott, S.J.Freedom, M.Gai, G.Goldring, C.R.Gould, A.Gruzinov, W.C.Haxton, K.M.Heeger, E.Henley, C.W.Johnson, M.Kamionkowski, R.W.Kavanagh, S.E.Koonin, K.Kubodera, K.Langanke, T.Motobayashi, V.Pandharipande, P.Parker, R.G.H.Robertson, C.Rolfs, R.F.Sawyer, N.Shaviv, T.D.Shoppa, K.A.Snover, E.Swanson, R.E.Tribble, S.Turck-Chieze, J.F.Wilkerson

Solar Fusion Cross Sections

NUCLEAR REACTIONS 7Be, 12,13C, 15N, 16,17,18O(p, γ), 14,15N, 17,18O(p, α), 7Li(d, p), 3He(p, e+), (α, γ), (3He, 2p), 1H(p, e+), E=low; compiled, analyzed S-factor data, calculations; deduced implications for solar neutrino flux calculations.

doi: 10.1103/RevModPhys.70.1265
Citations: PlumX Metrics


1998KU16      Phys.Rev.Lett. 81, 542 (1998)

D.Kusnezov, Y.Alhassid, K.A.Snover

Scaling Properties of the Giant Dipole Resonance Width in Hot Rotating Nuclei

NUCLEAR STRUCTURE A=45-208; compiled, analyzed GDR widths vs temperature, spin, mass; deduced phenomenological formula.

doi: 10.1103/PhysRevLett.81.542
Citations: PlumX Metrics


1997KE12      Phys.Rev. C56, 3201 (1997)

M.P.Kelly, J.F.Liang, A.A.Sonzogni, K.A.Snover, J.P.S.van Schagen, J.P.Lestone

Preequilibrium Particle Emission and the Giant-Dipole Resonance in Sn Nuclei

NUCLEAR REACTIONS 100Mo(18O, X), E=200 MeV; measured Eγ, Iγ, (particle)γ-coin, p-, α-spectra; deduced pre-equilibrium emission features. 115In, 118Sn deduced GDR pre-equilibrium emission effects.

doi: 10.1103/PhysRevC.56.3201
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1997KI13      Acta Phys.Pol. B28, 189 (1997)

M.Kicinska-Habior, Z.Trznadel, K.A.Snover, A.Maj, M.P.Kelly

New Results in High-Energy γ-Ray Studies from Heavy-Ion Reactions at Around 10 MeV/u

NUCLEAR REACTIONS 26Mg(12C, X), E=6, 8.5, 11 MeV/nucleon; 24Mg(12C, X), E=11 MeV/nucleon; measured Eγ, Iγ(θ); deduced GDR, bremsstrahlung parameters. Statistical models, BUU nuclear transport equation.


1996BE13      Phys.Rev. C53, 1759 (1996)

J.A.Behr, K.A.Snover, C.A.Gossett, G.Feldman, J.H.Gundlach, M.Kicinska-Habior

Nonstatistical γ Emission in 3He- and α-Induced Reactions

NUCLEAR REACTIONS 61Ni, 95Mo, 119,124Sn, 148,154Sm, 181Ta(α, γ), E=11-28 MeV; C, O, 61,62Ni, 95,96Mo, 120,124Sn, 148Sm, 181Ta(3He, γ), E=11-28 MeV; measured γ-ray production σ(Eγ) at θγ=90°; deduced systematics of nonstatistical γ-ray yields. Statistical model, direct plus semdirect excitation of the giant dipole resonance, including Coulomb, projectile excitation.

doi: 10.1103/PhysRevC.53.1759
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1995DE18      Phys.Rev. C51, 2778 (1995); Erratum Phys.Rev. C52, 3509 (1995)

L.De Braeckeleer, E.G.Adelberger, J.H.Gundlach, M.Kaplan, D.Markoff, A.M.Nathan, W.Schieff, K.A.Snover, D.W.Storm, K.B.Swartz, D.Wright, B.A.Brown

Radiative Decays of the 16.6 and 16.9 MeV States in 8Be and Tests of the Conservation of the Vector Current in the A = 8 Multiplet

NUCLEAR REACTIONS, ICPND 4He(α, γ), E=33-34.7 MeV; measured γ yield vs E, Iγ(θ). 8Be deduced doublet decay features, δ(E2/M1), Γγ, B(λ). Other A=8 nuclei data included in analysis, vector current conservation features discussed.

doi: 10.1103/PhysRevC.51.2778
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1995DR05      Phys.Rev. C52, 578 (1995)

Z.M.Drebi, K.A.Snover, A.W.Charlop, M.S.Kaplan, D.P.Wells, D.Ye, Y.Alhassid

Spin-Induced Shape Changes in Light-Medium Mass Compound Nuclei

NUCLEAR REACTIONS 27Al(32S, X), E=90-215 MeV; 45Sc(18O, X), E=54-149 MeV; measured γ(θ), production σ. 59,63Cu deduced GDR characteristics.

doi: 10.1103/PhysRevC.52.578
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1995KI13      Acta Phys.Pol. B26, 439 (1995)

M.Kicinska-Habior, K.A.Snover, A.Maj, Z.Drebi, D.Ye, M.Kelly

Ultradipole Radiation from Low-Energy Heavy-Ion Reactions

NUCLEAR REACTIONS 26Mg(12C, X), E=6-11 MeV/nucleon; 24Mg(12C, X), E=11 MeV/nucleon; measured Eγ, Iγ(θ); deduced ultradipole radiation related features.


1994KI03      Nucl.Phys. A569, 17c (1994)

M.Kicinska-Habior, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, Z.M.Drebi, M.S.Kaplan, D.P.Wells

Shape Changes and Isospin Purity in Highly Excited Light Mass Nuclei

NUCLEAR REACTIONS 27Al(12C, X), (18O, X), (19F, X), E not given; analyzed γ-spectra, σ(Eγ), Iγ(θ) data; deduced shape changes, isospin purity in hot nuclei. Other data discussed.

doi: 10.1016/0375-9474(94)90092-2
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1993AD09      Phys.Lett. 314B, 185 (1993)

E.G.Adelberger, L.De Braeckeleer, W.C.Haxton, K.A.Snover

Accelerator Calibration of Solar Neutrino Detectors

NUCLEAR REACTIONS 12C(p, n), E not given; calculated neutrino flux from 12N source.

doi: 10.1016/0370-2693(93)90447-P
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1993BE17      Phys.Rev.Lett. 70, 3201 (1993)

J.A.Behr, K.A.Snover, C.A.Gossett, M.Kicinska-Habior, J.H.Gundlach, Z.M.Drebi, M.S.Kaplan, D.P.Wells

Restoration of Isospin Symmetry in Highly Excited Compound Nuclei

NUCLEAR REACTIONS 12C, 13C(16O, X), (18O, X), (13C, X), (14N, X), (15N, X), E=22-108 MeV; measured γ production σ. 28Si, 26Al deduced isospin admixture, spreading widths.

doi: 10.1103/PhysRevLett.70.3201
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1993FE01      Phys.Rev. C47, 1436 (1993)

G.Feldman, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, M.Kicinska-Habior

Statistical γ Decay of the Giant Dipole Resonance in Highly Excited 46Ti and 52Cr

NUCLEAR REACTIONS 27Al(19F, X), E=30-60 MeV; 48Ti(α, X), E=12-28 MeV; measured inclusive γ production σ(E). 46Ti, 52Cr deduced GDR built on excited states, parameters.

doi: 10.1103/PhysRevC.47.1436
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1993KI08      Acta Phys.Pol. B24, 433 (1993)

M.Kicinska-Habior, K.A.Snover

Evidence for a Shape Change of Hot, Fast Rotating 45Sc Nuclei from GDR Studies

NUCLEAR REACTIONS 27Al(18O, X), E=44.9-109.6 MeV; measured γ-spectral shapes; deduced absorption σ(Eγ). 45Sc deduced structure near GDR, shape change evidence. Hot rotating nuclei.


1993KI12      Phys.Lett. 308B, 225 (1993)

M.Kicinska-Habior, K.A.Snover, J.A.Behr, C.A.Gossett, Y.Alhassid, N.Whelan

Search for a Phase Transition in the Nuclear Shape at Finite Temperature and Rapid Rotation

NUCLEAR REACTIONS 27Al(18O, X), E=44.9-109.6 MeV; measured Eγ, Iγ; deduced σ(E). 45Sc deduced GDR strength function, deformation features. Liquid drop model.

doi: 10.1016/0370-2693(93)91276-S
Citations: PlumX Metrics


1993SN01      Nucl.Phys. A553, 153c (1993)

K.A.Snover

The Giant Dipole Resonance at High Excitation Energy and Spin

NUCLEAR REACTIONS 45Sc, 28,30Si(γ, X), E ≤ 30 MeV; compiled, reviewed σ(E). 92Zr(58Ni, X), E=241 MeV; compiled, reviewed inclusive Eγ, Iγ data, calculations.

doi: 10.1016/0375-9474(93)90621-4
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1992KI01      Phys.Rev. C45, 569 (1992)

M.Kicinska-Habior, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, G.Feldman

Comparison of Giant Dipole Resonance Decay in Stiff 92Mo and Soft 100Mo Excited Nuclei

NUCLEAR REACTIONS 76Se(17O, X), E=50, 72.2 MeV; 82Se(18O, X), E=49.1-72.8 MeV; measured σ(Eγ), θ=90°. 92,100Mo deduced GDR built on excited states, decay features.

doi: 10.1103/PhysRevC.45.569
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1990GO23      Phys.Rev. C42, R1800 (1990)

C.A.Gossett, J.A.Behr, S.J.Luke, B.T.McLain, D.P.Rosenzweig, K.A.Snover, W.T.Hering

High-Energy Gamma Emission in Heavy-Ion Collisions at 9-14 MeV/Nucleon

NUCLEAR REACTIONS 92,100Mo(12C, X), E=9-14 MeV/nucleon; measured σ(E, Eγ); 92,100Mo(12C, X), E=11 MeV/nucleon; measured σ(θ, Eγ); 92,100Mo(13C, X), E=10, 11 MeV/neucleon; measured σ(Eγ). Enriched targets. Comparision with collective and nucleon-nucleon bremsstrahlung photon production mechanisms.

doi: 10.1103/PhysRevC.42.R1800
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1990GU20      Phys.Rev.Lett. 65, 2523 (1990)

J.H.Gundlach, K.A.Snover, J.A.Behr, C.A.Gossett, M.Kicinska-Habior, K.T.Lesko

Oblate Deformed Shapes of Hot Rotating Nuclei Deduced from Giant-Dipole-Resonance Decay Studies

NUCLEAR REACTIONS 72Ge(18O, X), E=50, 74 MeV; 64Ni(28Si, X), E=137 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ). 90Zr, 92Mo deduced GDR parameters, shape features. Hot rotating nuclei.

doi: 10.1103/PhysRevLett.65.2523
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1990KI04      Phys.Rev. C41, 2075 (1990)

M.Kicinska-Habior, K.A.Snover, J.A.Behr, G.Feldman, C.A.Gossett, J.H.Gundlach

Spin Dependence of the Giant-Dipole-Resonance Strength Function in Highly Excited Nuclei in the Mass Region A = 39-45

NUCLEAR REACTIONS, ICPND 27Al(12C, X), E=33.8-62.7 MeV; 27Al(13C, X), E=39.7 MeV; 27Al(15N, X), E=29.2, 44.7 MeV; 27Al(18O, X), E=31.5-72.5 MeV; measured continuum Eγ, Iγ, γ(θ); deduced fusion σ. 39,40K, 42Ca, 45Sc deduced GDR strength function.

doi: 10.1103/PhysRevC.41.2075
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1988GO05      J.Phys.(London) G14, Supplement S267 (1988)

C.A.Gossett, J.A.Behr, G.Feldman, J.H.Gundlach, M.Kicinska-Habior, K.A.Snover

Systematic Behaviour of the Giant Dipole Resonance in Highly Excited Nuclei

NUCLEAR REACTIONS 154Sm(12C, X), E=61.2 MeV; calculated σ(Eγ, E). 166Er deduced GDR role.

NUCLEAR STRUCTURE 108Sn, 140Ce, 156,166Er; calculated photoabsorption σ; deduced GDR role.

doi: 10.1088/0305-4616/14/S/028
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1987KI17      Phys.Rev. C36, 612 (1987)

M.Kicinska-Habior, K.A.Snover, C.A.Gossett, J.A.Behr, G.Feldman, H.K.Glatzel, J.H.Gundlach, E.F.Garman

Statistical Giant Dipole Resonance Decay of Highly Excited States of 63Cu

NUCLEAR REACTIONS 59Co(α, γ), E=17.8-28.4 MeV; 57Fe(6Li, X), E=13.9-36 MeV; 51V(12C, X), E=26.3-64.7 MeV; 45Sc(18O, X), E=39.9-75.1 MeV; measured σ(Eγ). 63Cu deduced giant dipole resonance parameters. 62,63Cu, 60,62Ni, 59Co, 56Fe deduced level densities. NaI detector. Statistical model analyses.

doi: 10.1103/PhysRevC.36.612
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1986HA30      Phys.Lett. 176B, 297 (1986)

M.N.Harakeh, D.H.Dowell, G.Feldman, E.F.Garman, R.Loveman, J.L.Osborne, K.A.Snover

Role of Isospin in the Statistical Decay of the Giant Dipole Resonance Built on Excited States

NUCLEAR REACTIONS 25Mg(3He, γ), E=11.8 MeV; 12C(16O, γ), E=40.2 MeV; 12C(12C, γ), 12,13C(13C, γ), E=40 MeV; measured σ vs Eγ, γ yields. 28Si, 24,25,26Mg deduced GDR, Γ, EWSR, T-mixing parameters.

doi: 10.1016/0370-2693(86)90167-X
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1985GO04      Phys.Rev.Lett. 54, 1486 (1985)

C.A.Gossett, K.A.Snover, J.A.Behr, G.Feldman, J.L.Osborne

Deformation of Heated Nuclei Observed in the Statistical Decay of the Giant Dipole Resonance

NUCLEAR REACTIONS 154,148Sm(12C, X), E=63 MeV; measured Eγ, Iγ, continuum spectra, σ(Eγ). 160,166Er deduced excited state based GDR parameters, splitting, deformation at high temperature.

doi: 10.1103/PhysRevLett.54.1486
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1984SN01      J.Phys.(Paris), Colloq.C-4, 337 (1984)

K.A.Snover

Giant Resonances Built on Highly Excited States

NUCLEAR REACTIONS 27Al(p, γ), E=22 MeV; 28Si(p, γ), E=11-39 MeV; 11B(p, γ), E=29.5 MeV; calculated σ(Eγ, θγ), σ(E). 25Mg(3He, γ), E=11.8 MeV; 12C(16O, γ), E=40 MeV; 64Ni(12C, γ), 58Ni(18O, γ), E not given; calculated σ(Eγ). 28Si(γ, p), E=15.6-22.5 MeV; calculated branching ratios. 130Te(34S, γ), E=141 MeV; 124Sn(29Si, γ), E=127 MeV; 60Ni(18O, γ), E=60 MeV; 28Si(18O, γ), E=40 MeV; calculated transition number per reaction.


1983DO03      Phys.Rev.Lett. 50, 1191 (1983)

D.H.Dowell, G.Feldman, K.A.Snover, A.M.Sandorfi, M.T.Collins

Excited-State Giant Dipole Resonances in (p, γ): A new probe of single-particle strengths

NUCLEAR REACTIONS 27Al(p, γ), E=11-39 MeV; measured Eγ, Iγ, σ(θγ) vs Eγ. 28Si deduced GDR, Γ, configuration.

doi: 10.1103/PhysRevLett.50.1191
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1983EA01      Nucl.Phys. A396, 221c (1983)

E.D.Earle, A.B.McDonald, E.G.Adelberger, K.A.Snover, H.E.Swanson, R.von Lintig, H.B.Mak, C.A.Barnes

Parity Mixing in 21Ne; Evidence for weak neutral currents in nuclei

NUCLEAR STRUCTURE 18,19F, 21Ne; analyzed data; deduced isoscalar, isovector weak nucleon-nucleon coupling constants.

NUCLEAR REACTIONS 21Ne(p, p'γ), E=4.08 MeV; measured Eγ, Iγ, γ CP; deduced isoscalar, isovector weak nucleon-nucleon coupling constants. 21Ne levels deduced parity mixing matrix element. Parity mixing input from 19,18F data.

doi: 10.1016/0375-9474(83)90021-0
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1983GA19      Phys.Rev. C28, 2554 (1983)

E.F.Garman, K.A.Snover, S.H.Chew, S.K.B.Hesmondhalgh, W.N.Catford, P.M.Walker

Giant Dipole Resonance in the Statistical Decay of 63Cu, 76Kr, and 127Cs Compound Nuclei

NUCLEAR REACTIONS, ICPND 51V, 64Zn, 115In(12C, γ), 45Sc, 58Ni, 109Ag(18O, γ), E=42-60 MeV; measured σ vs Eγ. 63Cu, 76Kr, 127Cs deduced average angular momentum, GDR parameters. Statistical model.

doi: 10.1103/PhysRevC.28.2554
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1983HO05      Phys.Rev. C27, 1244 (1983)

C.D.Hoyle, E.G.Adelberger, J.S.Blair, K.A.Snover, H.E.Swanson, R.D.Von Lintig

Isospin Mixing in 24Mg

RADIOACTIVITY 24Al(β+) [from 24Mg(p, n)]; measured βγ CP asymmetry, Eγ, Iγ; deduced isospin forbidden transition matrix element. 24Mg levels deduced isospin mixing.

doi: 10.1103/PhysRevC.27.1244
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1983KU01      Phys.Rev. C27, 948 (1983)

E.Kuhlmann, K.A.Snover, G.Feldman, M.Hindi

Alpha Capture into the Giant Quadrupole Resonance in 28Si

NUCLEAR REACTIONS, ICPND 24Mg(α, γ), E=4.3-14 MeV; measured Eγ, Iγ, σ(E, Eγ, θγ); deduced E1, E2 capture σ. 28Si deduced E1, E2 transition strengths. Enriched target. Hauser-Feshbach formalism, isospin effects.

doi: 10.1103/PhysRevC.27.948
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1983SN02      Phys.Rev. C27, 493 (1983)

K.A.Snover, G.Feldman, M.M.Hindi, E.Kuhlmann, M.N.Harakeh, M.Sasao, M.Noumachi, Y.Fujita, M.Fujiwara, K.Hosono

27Al(p, γ)28Si and 27Al(3He, d)28Si to the Stretched 11.58 MeV (6-, 0) and 14.36 MeV (6-, 1) Levels

NUCLEAR REACTIONS 27Al(p, γ), E ≈ 2876 keV; measured σ(Eγ, E). 28Si resonance deduced Γ, Γp, Γγ, configuration, B(M1). 27Al(3He, d), E=40, 60 MeV; measured σ(θ); deduced optical model parameters. 28Si levels deduced S, configuration. DWBA analysis.

doi: 10.1103/PhysRevC.27.493
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1983SN03      Phys.Rev. C27, 1837 (1983)

K.A.Snover, E.G.Adelberger, P.G.Ikossi, B.A.Brown

Proton Capture to Excited States of 16O: M1, E1, and Gamow-Teller transitions and shell model calculations

NUCLEAR STRUCTURE 16N; calculated levels, B(M1); deduced IAS. 16O, 16C; calculated M1, E1, Gamow-Teller, (p, n) transition rates. 15C, 17,18N; calculated Gamow-Teller transition rates. Shell model.

NUCLEAR REACTIONS 15N(p, γ), (p, p'γ), (p, αγ), (polarized p, γ), (polarized p, p'γ), (polarized p, αγ), E=2.5-9.5 MeV; measured capture σ(Eγ), σ(θγ), Eγ, Iγ, analyzing power vs θ. 16O deduced resonances, J, π, T, Γ, ΓpΓγ/Γ, B(M1) ratios, Γp/Γ, M1, E1 transition strengths. Shell model.

doi: 10.1103/PhysRevC.27.1837
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1982PR05      Phys.Lett. 115B, 291 (1982)

D.M.Pringle, E.F.Garman, S.H.Chew, K.A.Snover, W.N.Catford, S.K.B.Hesmondhalgh, K.W.Allen

Decay of the Lowest T = 2 State in 40Ca

NUCLEAR REACTIONS 36Ar(α, γ), E=5.495-5.505 MeV; measured Eγ, Iγ, γ yields. 40Ca deduced γ-transitions, B(M1), ΓαΓγ/Γ, Γγ/Γ, Γγ.

doi: 10.1016/0370-2693(82)90372-0
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1980HE04      Nucl.Phys. A336, 219 (1980)

R.L.Helmer, M.D.Hasinoff, J.E.Bussoletti, K.A.Snover, T.A.Trainor

Investigation of the Electric Quadrupole Strength in 13N Using the 12C(p, γ0)13N Reaction

NUCLEAR REACTIONS 12C(polarized p, γ), E=10-17 MeV; measured σ(Ep, θγ), asymmetry. 13N deduced E1, E2 σ. Enriched target.

doi: 10.1016/0375-9474(80)90621-1
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1980SN01      Phys.Rev.Lett. 44, 927 (1980)

K.A.Snover, P.G.Ikossi, E.G.Adelberger, K.T.Lesko

Unique Determination of the Amplitude and Phase for the Population of The Giant-Dipole Resonance in the Reaction 12C(p(pol), γ0)13N

NUCLEAR REACTIONS 12C(polarized p, γ), E=5-30 MeV; measured σ(E). 13N deduced GDR, T=3/2 M1(E2) interference.

doi: 10.1103/PhysRevLett.44.927
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1979AD01      Phys.Rev. C19, 1 (1979)

E.G.Adelberger, R.E.Marrs, K.A.Snover

Isospin Nonconserving Proton Decays of 13N(T = 3/2) to Negative Parity States of 12C

NUCLEAR REACTIONS 11B(3He, np), E=7 MeV; measured np-coin. 12C levels deduced isospin-forbidden excitation by proton decay from lowest T=3/2 level in 13N.

doi: 10.1103/PhysRevC.19.1
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1979IK02      Nucl.Phys. A319, 109 (1979)

P.G.Ikossi, K.A.Snover, J.L.Osborne, E.G.Adelberger, A.B.McDonald

The α-Width of the Lowest T = 2 State in 28Si

NUCLEAR REACTIONS 24Mg(α, α), E=5.9-6.25 MeV; measured σ(Eα, θ). 28Si deduced resonances, L, J, π, Γ, Γα, T. Enriched target.

doi: 10.1016/0375-9474(79)90174-X
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1979SN01      Phys.Rev.Lett. 43, 117 (1979)

K.A.Snover, P.G.Ikossi, T.A.Trainor

Observation of Magnetic Dipole Strength in 16O

NUCLEAR REACTIONS 15N(polarized p, γ), E=4-9 MeV; measured σ(θ), A(θ). 16O deduced M1 strength between 16-20 MeV excitation, B(M1), Γp, Γ, Γγ.

doi: 10.1103/PhysRevLett.43.117
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1978BL04      Phys.Rev.Lett. 41, 1712 (1978)

J.S.Blair, P.Dyer, K.A.Snover, T.A.Trainor

Nuclear 'Time-Delay' and X-Ray-Proton Coincidences Near a Nuclear Scattering Resonance

NUCLEAR REACTIONS 58Ni(p, p), E=3.13-3.18 MeV; measured pX-coin; deduced interference between nuclear scattering amplitude, products of atomic ionization.

doi: 10.1103/PhysRevLett.41.1712
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1978DI08      Phys.Rev. C18, 1973 (1978)

P.A.Dickey, P.L.Dyer, K.A.Snover, E.G.Adelberger

Gamma Decays of the First T = 3/2 States in 9Be and 9B

NUCLEAR REACTIONS 7Li(3He, pγ), E=7.5 MeV; 7Li(3He, nγ), E=13 MeV; measured pγ-, nγ-coin. 9Be, 9B levels deduced γ-branching, Γ.

doi: 10.1103/PhysRevC.18.1973
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1978MI10      Phys.Rev. C18, 1878 (1978)

D.J.Millener, E.K.Warburton, K.A.Snover, R.von Lintig, P.G.Ikossi

Electromagnetic Transitions between the Low-Lying Levels of 21Ne and their Relation to Parity Mixing of the 2.80-MeV 1/2± Doublet

NUCLEAR STRUCTURE 21Ne; calculated γ CP. 21Ne, 21Na; calculated nuclear wave functions, electromagnetic, parity-mixing matrix elements.

NUCLEAR REACTIONS 18O(α, n), E=5.1 MeV; measured γγ(θ). 21Ne deduced δ E3/M2.

doi: 10.1103/PhysRevC.18.1878
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1978OS04      Nucl.Phys. A305, 144 (1978)

J.L.Osborne, E.G.Adelberger, K.A.Snover

Total Width of the Lowest T = 2 State in 24Mg

NUCLEAR REACTIONS 23Na(p, γ), E=3906 keV; 27Al(p, γ), E=3671 keV; measured σγ(Ep, θ=90°). 24Mg T=2 resonance, 28Si resonance deduced Γ(cm). Natural targets.

doi: 10.1016/0375-9474(78)90168-9
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1978SN01      Phys.Rev.Lett. 41, 145 (1978)

K.A.Snover, R.von Lintig, E.G.Adelberger, H.E.Swanson, T.A.Trainor, A.B.McDonald, E.D.Earle, C.A.Barnes

Upper Limit on Parity Mixing in 21Ne

NUCLEAR REACTIONS 21Ne(p, p'), E=4.08 MeV; measured parity nonconserving γ-CP. 21Ne levels deduced parity-mixing matrix element.

doi: 10.1103/PhysRevLett.41.145
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1977AD02      Phys.Rev. C15, 484 (1977)

E.G.Adelberger, R.E.Marrs, K.A.Snover, J.E.Bussoletti

Radiative Transitions and Isospin Mixing in 12C

NUCLEAR REACTIONS 10B(3He, pγ), E=4.1 MeV; measured pγ-coin. 11B(p, γ), E=163 keV; measured σ(Eγ). 12C resonances deduced Γγ, isospin mixing.

doi: 10.1103/PhysRevC.15.484
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1977DI01      Phys.Rev.Lett. 38, 156 (1977)

F.S.Dietrich, D.W.Heikkinen, K.A.Snover, K.Ebisawa

Investigation of E2 and E3 Radiation Above the Giant Dipole Resonance in 89Y(p, γ0)90Zr

NUCLEAR REACTIONS 89Y(p, γ), E=14-27 MeV; measured σ(E, Eγ, θ). 90Zr deduced resonances, λ.

doi: 10.1103/PhysRevLett.38.156
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1977MA07      Nucl.Phys. A277, 429 (1977)

R.E.Marrs, E.G.Adelberger, K.A.Snover

Gamma Decays of Some T = 0, T = 1 and T = 2 States Above E(x) = 9.5 MeV in 20Ne

NUCLEAR REACTIONS 19F(3He, dγ), E=15.0 MeV; measured dγ-coin. 16O(α, γ), (α, α'γ), E=6.93, 9.2-9.7 MeV; measured σ(E, θ). 20Ne deduced levels, J, π, T, γ-branching, Γ, Γγ, Γα. NaI spectrometer.

doi: 10.1016/0375-9474(77)90711-4
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1977MA16      Phys.Rev. C16, 61 (1977)

R.E.Marrs, E.G.Adelberger, K.A.Snover

Electromagnetic Transitions in 13C and 13N

NUCLEAR REACTIONS 12C(p, γ), E ≈ 14.25 MeV; measured thick target yield. 11B(3He, pγ), E=5.3 MeV; 11B(3He, nγ), E=7.0 MeV; measured particle γ-coin. 13C, 13N levels deduced partial, total Γ, B(λ).

doi: 10.1103/PhysRevC.16.61
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1977SN01      Nucl.Phys. A285, 189 (1977)

K.A.Snover, P.Paul, H.M.Kuan

Radiative Proton Capture to the Ground State and First Three Excited States of 12C

NUCLEAR REACTIONS 11B(p, γ), E=6-23 MeV; measured σ(90°) for transitions to the 01+, 2+, 02+, , 3- levels in 12C. 11B(p, γ), E=12.4, 14.4 MeV; measured σ(θ). Enriched target.

doi: 10.1016/0375-9474(77)90245-7
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1976AD03      Phys.Lett. 62B, 29 (1976)

E.G.Adelberger, R.E.Marrs, K.A.Snover, J.E.Bussoletti

Isospin Mixing in 12C

NUCLEAR REACTIONS 10B(3He, pγ), E=4.1 MeV; measured γγ-coin. 11B(p, γ); measured resonance γ. 12C levels deduced γ-branching.

doi: 10.1016/0370-2693(76)90039-3
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1976MA01      Nucl.Phys. A256, 1 (1976)

R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper

Upper Limits for Isospin-Forbidden γ-Decays of T=2 States in 20Ne

NUCLEAR REACTIONS 19F(p, γ), E ≈ 4.09, 5.88 MeV; measured σ(E, Eγ). 20Ne deduced isospin-forbidden transition strengths, T=2 levels.

doi: 10.1016/0375-9474(76)90090-7
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1976SN01      Phys.Rev.Lett. 37, 273 (1976)

K.A.Snover, J.E.Bussoletti, K.Ebisawa, T.A.Trainor

Application of the Direct-Semidirect Model to the Interpretation of E1 And E2 Strength

NUCLEAR REACTIONS 14C(polarized p, γ), E=10-18 MeV; measured σ(E, Eγ, θ).

doi: 10.1103/PhysRevLett.37.273
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1975BR07      Phys.Rev. C11, 1122 (1975)

B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover

Recoil-Distance Lifetime Measurements of 48V Levels

NUCLEAR REACTIONS 45Sc(α, nγ), E=9.5 MeV; measured nγ-coin, recoil distance. 48V deduced levels, π, T1/2, B(λ).

doi: 10.1103/PhysRevC.11.1122
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1975HA06      Phys.Rev. C11, 998 (1975)

M.N.Harakeh, P.Paul, K.A.Snover

E1 Transitions in 17F. I. The Low-Lying T = 3/2 States

NUCLEAR REACTIONS 16O(p, γ), E=14.8 MeV; measured σ(Eγ, θ). 17F deduced resonances, level-width, B(E1).

doi: 10.1103/PhysRevC.11.998
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1975MA21      Phys.Rev.Lett. 35, 202 (1975)

R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper

Mirror γ Decays in 13C and 13N

NUCLEAR REACTIONS 12C(p, γ), E=14.2-14.3 MeV; measured resonance γ-yield. 11B(3He, pγ), (3He, nγ); measured pγ-, nγ-coin. 13N level deduced γ-mixing, B(λ).

doi: 10.1103/PhysRevLett.35.202
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1974BR04      Phys.Rev. C9, 1033 (1974)

B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover

Lifetime Measurements and E2 Effective Charges for Nuclei in the 1f7/2 Shell

NUCLEAR REACTIONS 39K(α, n), E=10.4 MeV; 16O, 40Ca(3He, p), E=10.5 MeV; 40Ca, 41K(α, p), E=14.0 MeV; 45Sc(α, p), E=10.0 MeV; 46Ti(α, p), E=11.0 MeV; 40Ca(16O, 2pα), E=47 MeV; 49Ti(α, n), E=14.5 MeV; 40Ca(16O, 3p), E=47 MeV; 40Ca(16O, 2p), E=47 MeV; measured recoil distance. 18F, 42,43Sc, 44Ca, 48Ti, 49V, 50,52Cr, 51,53Mn levels deduced T1/2, B(E2). Deduced 40 < A < 56 effective charges. Natural, enriched targets, Ge(Li) detector.

doi: 10.1103/PhysRevC.9.1033
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1974SN01      Phys.Rev.Lett. 32, 317 (1974)

K.A.Snover, K.Ebisawa, D.R.Brown, P.Paul

Evidence for a Collective E2 Resonance in the Reaction 208Pb(p, γ)209Bi

NUCLEAR REACTIONS 208Pb(p, γ), E=17.5-25 MeV; measured γ(θ). 209Bi deduced resonance.

doi: 10.1103/PhysRevLett.32.317
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1974SN02      Phys.Rev.Lett. 32, 1061 (1974)

K.A.Snover, E.G.Adelberger, D.R.Brown

Isoscalar Electric Quadrupole Strength in 16O

NUCLEAR REACTIONS 12C(α, γ), E=7-27.5 MeV; measured σ(E). 16O deduced giant E2 resonance.

doi: 10.1103/PhysRevLett.32.1061
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1972WA18      Phys.Rev. C6, 375 (1972)

E.K.Warburton, H.M.Kuan, D.E.Alburger, P.Paul, K.A.Snover

Comment on a Possible Jπ = 0+, T = 2 Resonance in Be9(He3, γγ)C12

NUCLEAR REACTIONS 9Be(3He, γ), E approx 1.74 MeV; measured σ(E;Eγ). 12C deduced no T=2 resonance, upper limit for level-width.

doi: 10.1103/PhysRevC.6.375
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1971PA30      Phys.Rev.Lett. 27, 1013 (1971)

P.Paul, J.F.Amann, K.A.Snover

Symmetry Energy for Collective Dipole Excitation

NUCLEAR REACTIONS 48Ca(p, γ), E=4-18 MeV; 63Cu(p, γ), E=2-18 MeV; measured σ(E;Eγ). 49Sc, 64Zn deduced giant dipole resonance structure, separation energies of T+1, T components.

doi: 10.1103/PhysRevLett.27.1013
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1971SN01      Phys.Rev. C4, 398 (1971)

K.A.Snover, J.M.McDonald, D.B.Fossan, E.K.Warburton

Gamma-Ray Decay of the Low-Lying Levels of Cl34

NUCLEAR REACTIONS 32S(3He, pγ), E=6.8 MeV; measured Eγ, Iγ, Doppler shift attenuation. 31P(α, nγ), E=8-11 MeV; measured recoil distance. 34Cl deduced levels, T1/2, γ-branching.

doi: 10.1103/PhysRevC.4.398
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1971SN03      Phys.Lett. 37B, 29 (1971)

K.A.Snover, J.F.Amann, W.Hering, P.Paul

Proton Radiative Capture into 209Bi Through Giant Resonances and Analog Resonances

NUCLEAR REACTIONS 208Pb(p, γ), E=8-18 MeV; calculated σ(E;Eγ). 209Bi deduced giant dipole/analog resonance interference, E1 strengths.

doi: 10.1016/0370-2693(71)90561-2
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1970GO04      Phys.Rev. C1, 123 (1970)

D.R.Goosman, E.G.Adelberger, K.A.Snover

T = 3/2 Levels in 11B from the 10Be(p, γ0)11B Reaction

NUCLEAR REACTIONS 10Be(p, γ), E=0.6-6.3 MeV; measured σ(E;Eγ, θ(γ)). 11B deduced isobaric analog resonances, J, π, level-width.

doi: 10.1103/PhysRevC.1.123
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1969SN01      Phys.Rev.Letters 22, 239(1969)

K.A.Snover, D.W.Heikkinen, F.Riess, H.M.Kuan, S.S.Hanna

Lowest T = 2 Level in 28Si Observed as a Highly Forbidden Compound-Nucleus Resonance

NUCLEAR REACTIONS 24Mg(α, γ), (α, α'), E=6.09-6.13 MeV; measured σ(E;Eγ), σ(E;Eα', θ). 28Si deduced resonances, level-width.

doi: 10.1103/PhysRevLett.22.239
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1968PA09      Phys.Rev. 173, 919 (1968)

P.Paul, D.Kohler, K.A.Snover

Magnetic Dipole Transitions and Isospin in Be8

NUCLEAR STRUCTURE 8Be, 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.173.919
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1967KU06      Phys.Letters 25B, 217 (1967)

H.M.Kuan, D.W.Heikkinen, K.A.Snover, F.Riess, S.S.Hanna

Observation of T = 2 Level in 20Ne as a Compound Nucleus Resonance

NUCLEAR STRUCTURE 20Ne, 19F; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90043-3
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