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NSR database version of May 8, 2024.

Search: Author = S.S.Hanna

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2002MA43      Nucl.Phys. A704, 98c (2002)

K.Matsuta, T.Minamisono, M.Fukuda, M.Mihara, K.Sato, K.Minamisono, T.Yamaguchi, T.Onishi, T.Miyake, M.Sasaki, M.Tanigaki, T.Ohtsubo, S.Momota, Y.Nojiri, K.Yoshida, A.Ozawa, I.Tanihata, A.Kitagawa, M.Torikoshi, M.Kanazawa, S.Koda, T.Nishio, M.Suda, J.R.Alonso, G.F.Krebs, T.J.M.Symons, S.S.Hanna

Recent Studies on the Nuclear Moments of Light Mirror Nuclei ( T = 1/2, 3/2)

NUCLEAR MOMENTS ⁹C, ¹³O, ²⁷Mg, ²⁷Si; measured β-NMR spectra of oriented nuclei; deduced quadrupole moments.

doi: 10.1016/S0375-9474(02)00770-4
Citations: PlumX Metrics

1999HA24      Nucl.Phys. A649, 271c (1999)

S.S.Hanna

Analog Giant Resonances Excited by (p, n), (n, p), (π^-, γ), (π^±, π⁰), (π⁺, π^-), (d, ²He), (t, ³He) and (³He, ³H) Reactions

NUCLEAR REACTIONS ¹³C(n, p), E=65 MeV; ¹³C(π^-, γ), E not given; ^12,13C(π⁺, π⁰), (π^-, π⁰), E=165 MeV; analyzed data; deduced analog resonance production features.

doi: 10.1016/S0375-9474(99)00071-8
Citations: PlumX Metrics

1999MB13      Hyperfine Interactions 120/121, 673 (1999)

K.Matsuta, T.Onishi, M.Fukuda, T.Minamisono, H.Akai, M.Sasaki, T.Yamaguchi, T.Miyake, K.Sato, K.Minamisono, F.Ohsumi, Y.Muramoto, S.Oui, C.Ha, K.Tanaka, K.Kidera, A.Morishita, A.Kitagawa, M.Torikoshi, M.Kanazawa, T.Nishio, S.Koda, T.Ohtsubo, S.Fukuda, Y.Nojiri, S.Momota, A.Ozawa, K.Yoshida, T.Suzuki, T.Kobayashi, I.Tanihata, S.S.Hanna, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Electromagnetic moments of short lived β emitters ²¹F, ²³Mg, ²⁷Si and ³⁹Ca

NUCLEAR MOMENTS ²¹F, ²³Mg, ²⁷Si, ³⁹Ca; measured asymmetry change as a function of the frequency; deduced magnetic moments, electrical quadrupole coupling constants. Comparison with OXBASH shell model calculations.

doi: 10.1023/A:1017036009679
Citations: PlumX Metrics

1998FR07      Phys.Rev. C57, 3144 (1998)

E.Frlez, D.Pocanic, K.A.Assamagan, J.P.Chen, K.J.Keeter, R.M.Marshall, R.C.Minehart, L.C.Smith, G.E.Dodge, S.S.Hanna, B.H.King, J.N.Knudson

Differential Cross Sections for Pion Charge Exchange on the Proton at 27.5 MeV

NUCLEAR REACTIONS ¹H(π^-, π⁰), E=27.5 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.57.3144
Citations: PlumX Metrics

1998HA24      Nucl.Instrum.Methods Phys.Res. A401, 345 (1998)

S.S.Hanna, C.J.Martoff, D.Pocanic, K.Wang, R.C.Byrd, C.C.Foster, I.J.van Heerden

A Monochromatic Neutron Facility for (n, p) Reactions

NUCLEAR REACTIONS ⁶Li, ¹³C(n, p), E=118 MeV; measured proton spectra.

doi: 10.1016/S0168-9002(97)00985-6
Citations: PlumX Metrics

1996MA58      Phys.Rev. C54, 2767 (1996)

C.J.Martoff, S.S.Hanna, D.Pocanic, K.Wang, W.J.Cummings, R.C.Byrd, C.C.Foster

Reaction ¹³C(n, p)¹³B at 118 MeV

NUCLEAR REACTIONS ¹³C(n, p), E=118 MeV; measured σ(θ), proton spectra; deduced nucleon-nucleon interaction spin-isospin component central part volume integral, (n, p), (p, n) reaction σ universal proportionality energy dependence.

doi: 10.1103/PhysRevC.54.2767
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13951.

1996WA06      Phys.Rev. C53, 1718 (1996)

K.Wang, C.J.Martoff, D.Pocanic, S.S.Hanna, F.P.Brady, J.L.Romero, C.M.Castaneda, J.R.Drummond, B.McEachern, D.S.Sorenson

Reaction ¹³C(n, p)¹³B at 65 MeV

NUCLEAR REACTIONS ¹³C(n, p), E=65 MeV; measured spectra, σ(θ); deduced v(c)(στ). ¹³B levels deduced spin-dipole transition role, possible analog resonance.

doi: 10.1103/PhysRevC.53.1718
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13633.

1994HA41      Nucl.Phys. A577, 173c (1994)

S.S.Hanna

Isospin Splitting in Analog Giant Resonances Excited by Single Pion Charge Exchange Reactions

NUCLEAR REACTIONS ¹²C(π⁺, π⁰), (π^-, π⁰), ¹³C, ⁹Be(π⁺, π⁰), (π^-, π⁰), E=165 MeV; measured σ(θ) vs E(π). ¹³C(π⁺, pπ⁰), E=165 MeV; measured pπ⁰(θ). ¹³B, ⁹Li, ^12,13N, ⁹B deduced levels, isospin.

doi: 10.1016/0375-9474(94)90852-4
Citations: PlumX Metrics

1994KN01      Phys.Rev. C50, 909 (1994)

J.N.Knudson, J.D.Bowman, S.I.Penttila, J.R.Comfort, J.Tinsley, B.G.Ritchie, J.Gorgen, D.Mathis, S.S.Hanna, B.King, D.Pocanic, R.A.Loveman, L.S.Fritz, N.S.Dixon

Neutron Deformation in ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=165 MeV; measured σ(E, θ), oriented, unoriented nuclei; deduced asymmetry vs θ. ¹⁶⁵Ho deduced neutron distribution deformation features.

doi: 10.1103/PhysRevC.50.909
Citations: PlumX Metrics

1994KU19      Phys.Rev. C50, 1771 (1994)

S.E.Kuhn, W.J.Cummings, G.E.Dodge, S.S.Hanna, B.H.King, Y.M.Shin, J.G.Congleton, R.Helmer, R.B.Schubank, N.R.Stevenson, U.Wienands, Y.K.Lee, G.R.Mason, B.E.King, K.S.Chung, J.M.Lee, D.P.Rosenzweig

Multinucleon Effects in Muon Capture on ³He at High Energy Transfer

NUCLEAR REACTIONS ³He(μ^-, p), (μ^-, d), (μ^-, np), E at rest; measured proton, deuteron, np-coin spectra. PWIA with, without breakup channel.

doi: 10.1103/PhysRevC.50.1771
Citations: PlumX Metrics

1994PO01      Phys.Rev.Lett. 72, 1156 (1994)

D.Pocanic, E.Frlez, K.A.Assamagan, J.P.Chen, K.J.Keeter, R.M.Marshall, R.C.Minehart, L.C.Smith, G.E.Dodge, S.S.Hanna, B.H.King, J.N.Knudson

Reaction π⁺p → π⁺π⁰p Near Threshold and Chiral Symmetry Breaking

NUCLEAR REACTIONS ¹H(π⁺, π⁺π⁰), E=190-260 MeV; measured invariant mass spectra, π⁰π⁺-, π⁰p-coin; deduced total σ(E).

doi: 10.1103/PhysRevLett.72.1156
Citations: PlumX Metrics

1992CU01      Phys.Rev.Lett. 68, 293 (1992)

W.J.Cummings, G.E.Dodge, S.S.Hanna, B.H.King, S.E.Kuhn, Y.M.Shin, R.Helmer, R.B.Schubank, N.R.Stevenson, U.Wienands, Y.K.Lee, G.R.Mason, B.E.King, K.S.Chung, J.M.Lee, D.P.Rosenzweig

Energetic Protons and Deuterons Emitted following μ^- Capture by ³He Nuclei

NUCLEAR REACTIONS ³He(μ^-, X), E at rest; measured p-, d-spectra; deduced capture strength, nucleon-nucleon correlations, meson exchange currents role.

doi: 10.1103/PhysRevLett.68.293
Citations: PlumX Metrics

1992KI05      Nucl.Phys. A539, 1 (1992)

S.W.Kikstra, S.S.Hanna, A.G.M.van Hees, Z.Guo, C.van der Leun

Resonant Absorption by the Lowest Two T = (3/2) Levels of ⁹Be

NUCLEAR REACTIONS ⁹Be(γ, X), E=14.38-16.98 MeV; measured σ(Eγ), ⁹Be levels deduced Γγ₀, isospin mixing, giant M1 resonance parameters. Shell model calculations. Monochromatic γ's from ¹¹B(p, γ₀γ₁).

doi: 10.1016/0375-9474(92)90232-9
Citations: PlumX Metrics

1991KN01      Phys.Rev.Lett. 66, 1026 (1991)

J.N.Knudson, J.D.Bowman, S.I.Penttila, J.R.Comfort, B.G.Ritchie, J.Gorgen, D.Mathis, J.Tinsley, S.S.Hanna, B.King, D.Pocanic, R.A.Loveman, L.S.Fritz, N.S.Dixon

Neutron Deformation in ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=165 MeV; measured σ(E(π⁰)), orientation asymmetries. ¹⁶⁵Ho deduced neutral, charge quadrupole deformation ratio. Aligned, unaligned targets.

doi: 10.1103/PhysRevLett.66.1026
Citations: PlumX Metrics

1991MA02      Phys.Rev. C43, 1106 (1991)

C.J.Martoff, W.J.Cummings, D.Pocanic, S.S.Hanna, H.Ullrich, M.Furic, T.Petkovic, T.Kozlowski, J.P.Perroud

Nucleon Pairing in μ^- Capture by ⁴⁰Ca

NUCLEAR REACTIONS Ca(μ^-, p), (μ^-, n), E at rest; measured nucleon spectra; deduced correlated pair capture role.

doi: 10.1103/PhysRevC.43.1106
Citations: PlumX Metrics

1990WU01      Phys.Rev. C41, 1600 (1990)

C.Y.Wu, M.Satteson, K.Wang, D.Cline, H.E.Gove, S.S.Hanna, M.Hass, R.Ibbotson, A.V.Ramayya

Isomers in Iodine Nuclei

NUCLEAR REACTIONS ⁹²Mo(²⁸Si, n3p), E=120 MeV; ¹¹⁶Cd(¹¹B, 5n), (¹¹B, 6n), E=65 MeV; measured Eγ, Iγ, γ(t). ^116,121,122I deduced isomer T_1/2.

doi: 10.1103/PhysRevC.41.1600
Citations: PlumX Metrics

1989WU01      Phys.Rev. C39, 250 (1989)

C.Y.Wu, J.Boyle, D.Cline, E.Dafni, H.E.Gove, M.Satteson, K.Wang, S.S.Hanna, A.V.Ramayya

Successive Decays of Isomers in ⁸¹Sr

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, n4p), E=140 MeV; measured E(γ), I(γ). ⁸¹Sr deduced isomer T_1/2.

doi: 10.1103/PhysRevC.39.250
Citations: PlumX Metrics

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

doi: 10.1103/PhysRevC.37.2881
Citations: PlumX Metrics

1988GA22      Nucl.Instrum.Methods Phys.Res. A271, 483 (1988)

C.S.Galovich, S.S.Hanna, D.L.Clark

Design and Performance of an Electron-Positron Pair Detector

NUCLEAR REACTIONS ⁴⁰Ca, ¹⁶O(p, p'), E=10.2 MeV; measured pair production spectra. 4π acceptance pair spectrometer.

doi: 10.1016/0168-9002(88)90309-9
Citations: PlumX Metrics

1988HA12      J.Phys.(London) G14, Supplement S283 (1988)

S.S.Hanna

Current Developments in Giant Resonances

NUCLEAR REACTIONS ⁶Li(n, p), E=118 MeV; measured σ(Ep), σ(θ=0°). ⁶He level deduced transition characteristics.

doi: 10.1088/0305-4616/14/S/030
Citations: PlumX Metrics

1988HA21      Nucl.Phys. A483, 1 (1988)

J.R.Hall, D.L.Clark, S.J.Freedman, S.S.Hanna

Energy Dependence of the Beta Asymmetry in the Decay of ⁸Li

RADIOACTIVITY ⁸Li(β^-) [from ⁷Li(polarized d, p), E=6 MeV]; measured β-decay asymmetry vs E(β); deduced no second class current evidence. Shell model, conserved vector current hypothesis comparison. Plastic scintillation detectors, enriched target, polarized source.

doi: 10.1016/0375-9474(88)90061-9
Citations: PlumX Metrics

1988KU08      Phys.Rev. C37, 2281 (1988)

P.M.Kurjan, J.R.Calarco, G.A.Fisher, S.S.Hanna

Giant E1 Resonances in ²⁰Ne Observed with the ¹⁹F(p(pol), γ₀γ₁)²⁰Ne Reactions

NUCLEAR REACTIONS, ICPND ¹⁹F(polarized p, γ), E=3-10 MeV; measured γ yield, σ(θγ). ²⁰Ne deduced transition γ multipolarity, GDR features.

doi: 10.1103/PhysRevC.37.2281
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0086.

1988WA13      Phys.Rev. C37, 2301 (1988)

T.R.Wang, W.Haeberli, S.W.Wissink, S.S.Hanna

Electric Quadrupole Strength in ²⁰Ne from the ¹⁹F(p(pol), γ₀)²⁰Ne Reaction

NUCLEAR REACTIONS, ICPND ¹⁹F(polarized p, γ), E=3.5-13.3 MeV; measured σ(θ), analyzing power vs θ, σ(E). ²⁰Ne deduced GQR features.

doi: 10.1103/PhysRevC.37.2301
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2715.

1988WA24      Phys.Rev. C38, 2478 (1988)

K.Wang, C.J.Martoff, D.Pocanic, W.J.Cummings, S.S.Hanna, R.C.Byrd, C.C.Foster

Reaction ⁶Li(n, p)⁶He at 118 MeV

NUCLEAR REACTIONS ⁶Li(n, p), E=118 MeV; measured σ(θ); deduced Gamow-Teller resonance, sum rule. DWBA analyses. Intrinsic germanium detectors, enriched target.

doi: 10.1103/PhysRevC.38.2478
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13152.

1988WI16      Phys.Rev. C37, 2289 (1988)

S.W.Wissink, S.S.Hanna, D.G.Mavis, T.R.Wang

Electric Quadrupole Strength in ¹⁶O from the ¹⁵N(p(pol), γ₀)¹⁶O Reaction

NUCLEAR REACTIONS, ICPND ¹⁵N(polarized p, γ), E=6.25-13.75 MeV; measured γ(θ), analyzing powers, σ(θ), σ(E). ¹⁶O deduced GQR features.

doi: 10.1103/PhysRevC.37.2289
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2714.

1987KN02      Phys.Rev. C35, 1382 (1987)

J.N.Knudson, J.R.Comfort, R.A.Gianelli, B.G.Ritchie, D.Rothenberger, D.Pocanic, S.S.Hanna, J.D.Bowman, H.W.Baer, A.G.Bergmann, P.A.Heusi, F.Irom, C.J.Seftor, S.Hoibraten, R.A.Loveman, S.H.Rokni, H.Crannell, D.I.Sober, W.J.Fickinger, H.Marshak

Excitation of the Isobaric Analog State of ¹⁶⁵Ho Pion Single-Charge Exchange

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=98, 163.2, 228.3 MeV; measured π⁰ yield, θ=4°-6°. ¹²⁰Sn(π⁺, π⁰), E=98-165 MeV; analyzed data; deduced reaction systematics vs mass. ¹⁶⁵Er deduced IAS excitation σ.

doi: 10.1103/PhysRevC.35.1382
Citations: PlumX Metrics

1987NE04      Phys.Rev. C35, 890 (1987)

B.T.Neyer, D.L.Clark, J.S.Dunham, W.A.Seale, J.L.Thornton, R.T.Westervelt, S.S.Hanna, B.A.Brown, B.H.Wildenthal

Lifetime of the Lowest 0⁺, T = 1 State of ²²Na

NUCLEAR REACTIONS ¹⁹F(α, n), E=4.3 MeV; measured Doppler shift, recoil. ²²Na level deduced T_1/2, M1 transition characteristics, analog β-decay Gamow-Teller transition comparison.

doi: 10.1103/PhysRevC.35.890
Citations: PlumX Metrics

1987PO18      Can.J.Phys. 65, 687 (1987)

D.Pocanic, K.Wang, C.J.Martoff, S.S.Hanna, R.C.Byrd, C.C.Foster, D.L.Friesel, J.Rapaport

First (n, p) Measurements with the Indiana University Cyclotron Facility

NUCLEAR REACTIONS ⁶Li(n, p), E=118 MeV; measured σ(Ep), σ(θp).

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13152.

1987ZI01      Nucl.Phys. A462, 205 (1987)

F.Zijderhand, S.W.Kikstra, S.S.Hanna, C.van der Leun

Resonant Absorption and the Isospin Mixing of the Second T = (3/2) State of ⁹Be

NUCLEAR REACTIONS ⁷Li(d, γ), E ≈ 0.36 MeV; measured σ(E(d)); ⁹Be(γ, X), E=16.96-16.99 MeV; measured σ(E). ⁹Be deduced Γ, Γγ, resonance strength, T-mixing. Natural target.

doi: 10.1016/0375-9474(87)90545-8
Citations: PlumX Metrics

1986MA16      Czech.J.Phys. B36, 378 (1986)

C.J.Martoff, D.Pocanic, L.W.Whitlow, S.S.Hanna, H.Ullrich, S.Cierjacks, M.Furic, T.Petkovic, H.J.Weyer

Search for Emission of Nucleons and Nucleon Pairs following Muon Capture in Selected Light Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O, ²⁷Al(μ^-, p), E at rest; measured proton spectra.

doi: 10.1007/BF01597841
Citations: PlumX Metrics

1985HA18      Hyperfine Interactions 21, 59 (1985)

S.S.Hanna, J.W.Hugg

Analysis of the Magnetic Moments of Mirror Nuclei

NUCLEAR STRUCTURE A=1-43; analyzed data; deduced isoscalar sum, isovector difference moments.

doi: 10.1007/BF02061977
Citations: PlumX Metrics

1984CA34      Phys.Lett. 146B, 179 (1984)

J.R.Calarco, J.Arruda-Neto, K.A.Griffioen, S.S.Hanna, D.H.H.Hoffmann, B.Neyer, R.E.Rand, K.Wienhard, M.R.Yearian

Observation of Monopole Strength in the ¹²C(e, e'p₀)¹¹B Reaction

NUCLEAR REACTIONS ¹²C(e, e'p), E=86, 118, 126 MeV; measured σ(E(e'), θ(e'), θp), forward, backward asymmetry. ¹²C deduced possible monopole resonance, EWSR.

doi: 10.1016/0370-2693(84)91012-8
Citations: PlumX Metrics

1984DU07      Nucl.Instrum.Methods 219, 46 (1984)

J.S.Dunham, C.S.Galovich, H.F.Glavish, S.S.Hanna, D.G.Mavis, S.W.Wissink

Polarized Gas Jet Targets

NUCLEAR REACTIONS ¹H(α, α), E=8 MeV; measured target polarization. Polarized gas jet targets.

doi: 10.1016/0167-5087(84)90133-9
Citations: PlumX Metrics

1984PO15      Phys.Rev. C30, 1520 (1984)

D.Pocanic, K.Van Bibber, J.S.Dunham, W.A.Seale, F.Sperisen, S.S.Hanna

Intermediate Structure in the ¹⁶O + ¹⁶O System

NUCLEAR REACTIONS ¹⁶O(¹⁶O, α), E=20-44 MeV; measured σ(θ) vs E; deduced optical model parameters. ³²S deduced intermediate structure, resonance J, π. Statistical, Hauser-Feshbach analyses.

doi: 10.1103/PhysRevC.30.1520
Citations: PlumX Metrics

1983CA14      Phys.Rev. C28, 483 (1983); Erratum Phys.Rev. C29, 672 (1983)

J.R.Calarco, S.S.Hanna, C.C.Chang, E.M.Diener, E.Kuhlmann, G.A.Fisher

Absolute Cross Section for the Reaction ³H(p, γ₀)⁴He and a Review of ⁴He(γ, p₀)³H Measurements

NUCLEAR REACTIONS ³H(p, γ₀), E=8.34, 13.6 MeV; measured σ(θ=90°).

doi: 10.1103/PhysRevC.28.483
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1222.

1983MI08      Phys.Rev. C28, 497 (1983)

D.J.Millener, J.W.Olness, E.K.Warburton, S.S.Hanna

Strong E1 Transitions in ⁹Be, ¹¹Be, and ¹³C

NUCLEAR STRUCTURE ^9,11Be, ¹³C; calculated B(λ). Shell model.

NUCLEAR REACTIONS ⁹Be(t, pγ), E=1.5-3.3 MeV; ³H(⁹Be, pγ), E=10-16 MeV; measured DSA. ¹¹Be level deduced T_1/2.

doi: 10.1103/PhysRevC.28.497
Citations: PlumX Metrics

1982HA12      Phys.Rev. C25, 1179 (1982)

S.S.Hanna, W.Feldman, M.Suffert, D.Kurath

High-Lying 0⁺ and 3^- Levels in ¹²C

NUCLEAR REACTIONS ¹¹B(p, γ), E=0.82-2.83 MeV; measured σ(θ) vs E, γ(θ). ¹²C levels deduced J, π, transition strengths, Γγ. Shell model.

doi: 10.1103/PhysRevC.25.1179
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0048.

1981PO16      Fizika(Zagreb) 13, Suppl.No.1, 35 (1981)

D.Pocanic, K.Van Bibber, W.A.Seale, J.Dunham, J.L.Thornton, S.S.Hanna

Intermediate Structure in the ¹⁶O + ¹⁶O System Observed via the α Exit Channel

NUCLEAR REACTIONS ¹⁶O(¹⁶O, α), E ≈ 20-45 MeV; measured σ(θ, E). ³²S deduced intermediate structure. Correlation, deviation function analysis.

1980CA11      Phys.Lett. 92B, 67 (1980)

J.R.Calarco, P.M.Kurjan, G.A.Fisher, S.S.Hanna

Intermediate Structure in the Giant E1 Resonance in the ¹⁹F(p, γ₀)²⁰Ne Reaction

NUCLEAR REACTIONS ¹⁹F(p, γ), (polarized p, γ), E=3.5-10 MeV; measured σ(E, θ); deduced E1, E2 capture amplitudes, intermediate structure. Doorway resonances model.

doi: 10.1016/0370-2693(80)90305-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0086.

1980LI12      Hyperfine Interactions 8, 3 (1980)

A.Little, H.C.Jain, S.M.Lazarus, T.K.Saylor, B.B.Triplett, S.S.Hanna

Calculation of Hyperfine Interactions Measured by Magnetic Decoupling In Oxygen Ions

NUCLEAR REACTIONS ¹⁹F(p, α), E=0.874, 1.374, 2.026 MeV; ¹⁶O(α, α'), E=17.55 MeV; measured αγ(θ, H), αγ(θ); deduced hyperfine interaction of atomic orbitals.

doi: 10.1007/BF01026853
Citations: PlumX Metrics

1979CH19      Nucl.Phys. A322, 168 (1979)

V.K.C.Cheng, A.Little, H.C.Yuen, S.M.Lazarus, S.S.Hanna

Nuclear Reaction Cross Sections of ¹⁶O + ¹⁶O Obtained by γ-Ray Detection

NUCLEAR REACTIONS ¹⁶O(¹⁶O, X), E(cm)=9.30 MeV; measured σ(E, Eγ, θ); deduced partial, total reaction σ. Ge(Li) detector, natural target.

doi: 10.1016/0375-9474(79)90340-3
Citations: PlumX Metrics

1979KU10      Phys.Rev. C20, 5 (1979)

E.Kuhlmann, J.R.Calarco, V.K.C.Cheng, D.G.Mavis, J.R.Hall, S.S.Hanna

E1 and E2 Strength in ³²S and ³⁴S Observed in α-Capture Reactions

NUCLEAR REACTIONS ²⁸Si(α, γ₀), E=5-16 MeV; ³⁰Si(α, γ₀), E=4-15 MeV; measured σ(E, Eγ, θγ). ^32,34S deduced E1, E2 strengths. Enriched targets.

doi: 10.1103/PhysRevC.20.5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0271.

1979VE02      Phys.Rev. C19, 1705 (1979)

E.Ventura, J.R.Calarco, C.C.Chang, E.M.Diener, D.G.Mavis, S.S.Hanna, G.A.Fisher

Structure in the Giant Resonance Region of ¹⁶O Observed with the Reaction ¹³C(³He, γ)¹⁶O

NUCLEAR REACTIONS ¹³C(³He, γ), E=3.0-8.5 MeV; measured σ(E(³He), Eγ, θ). ¹⁶O deduced resonances, structure in giant resonance region. Enriched ¹³C target.

doi: 10.1103/PhysRevC.19.1705
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1978OC01      Phys.Rev. C17, 892 (1978)

W.J.O'Connell, S.S.Hanna

Giant E1 Resonance in ¹⁶O Observed with the Reaction ¹⁵N(p, γ₀)¹⁶O

NUCLEAR REACTIONS ¹⁵N(p, γ), E=8.6-18.0 MeV; measured σ(E, Eγ, θ). ¹⁶O deduced giant resonance, level properties. ¹⁵N(p, αγ), E=8.6-18.0 MeV; measured yield. 99.3% enriched gas target.

doi: 10.1103/PhysRevC.17.892
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1977CA21      Phys.Rev.Lett. 39, 925 (1977)

J.R.Calarco, S.W.Wissink, M.Sasao, K.Wienhard, S.S.Hanna

Structure in the Giant Dipole Resonance of ¹⁶O: Evidence for a Secondary Doorway State from Polarized-Proton Capture

NUCLEAR REACTIONS ¹⁵N(polarized p, γ); measured σ. ¹⁶O deduced doorway state, parameters in GDR region.

doi: 10.1103/PhysRevLett.39.925
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1977LA01      Phys.Rev. C15, 1043 (1977)

G.Langouche, B.B.Triplett, N.S.Dixon, S.S.Hanna, P.Boolchand

Nuclear Orientation of ¹²⁵Sb in Pd₂MnSb Observed with the Mossbauer Effect of ¹²⁵Te

NUCLEAR MOMENTS ¹²⁵Sb, ^125mTe; measured Mossbauer effect of ¹²⁵Te level; deduced sign of μ. Oriented ¹²⁵Sb, ZnTe absorber.

doi: 10.1103/PhysRevC.15.1043
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1977LA03      Phys.Rev. B15, 2504 (1977)

G.Langouche, B.B.Triplett, N.S.Dixon, Y.Mahmud, S.S.Hanna

Mossbauer Investigation of ¹²⁹I in Te-Thiourea Compounds and the Quadrupole Moment of the First Excited State of ¹²⁵Te

NUCLEAR MOMENTS ¹²⁵Te; measured quadrupole moment for 1st excited state. Mossbauer technique.

doi: 10.1103/PhysRevB.15.2504
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1976FI05      Phys.Rev. C14, 28 (1976)

G.A.Fisher, P.Paul, F.Riess, S.S.Hanna

Giant E1 Resonances in ⁸Be from the Reaction ⁷Li(p, γ)⁸Be

NUCLEAR REACTIONS ⁷Li(p, γ), E=0.8-17.6 MeV; measured σ(E, Eγ, θ). ⁸Be deduced giant resonances, Γγ.

doi: 10.1103/PhysRevC.14.28
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1976HA64      Aust.J.Phys. 29, 511 (1976)

S.S.Hanna

Giant Resonances

1976JA16      Phys.Rev. C14, 2013 (1976)

H.C.Jain, A.Little, S.M.Lazarus, T.K.Saylor, B.B.Triplett, S.S.Hanna

Magnetic Moment of the 3^- Level of ⁴⁰Ca from Magnetic Decoupling in Free Ions

NUCLEAR REACTIONS ⁴⁰Ca(α, α'), E=16.17 MeV; measured (α, α'γ) correlation vs decoupling field H for free ion recoil. ⁴⁰Ca deduced μ. Natural thin targets.

doi: 10.1103/PhysRevC.14.2013
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1976JA20      Hyperfine Interactions 2, 385 (1976)

H.C.Jain, A.Little, B.B.Triplett, S.M.Lazarus, T.K.Saylor, S.S.Hanna

Decoupling of the Hyperfine Interactions in ⁴⁰Ca Ions Recoiling into Vacuum

NUCLEAR REACTIONS ⁴⁰Ca(α, α'γ), E=16.17 MeV; measured α'γ(θ, H). ⁴⁰Ca level deduced g.

doi: 10.1007/BF01021184
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1976LA09      Phys.Rev. C13, 2589 (1976)

G.Langouche, N.S.Dixon, Y.Mahmud, B.B.Triplett, S.S.Hanna, P.Boolchand

Magnetic Moment of the First Excited State of ¹²¹Sb and the Hyperfine Field in Pd₂MnSb

NUCLEAR MOMENTS ¹²¹Sb; measured Mossbauer effect; deduced μ, hyperfine field in Pd₂MnSb.

doi: 10.1103/PhysRevC.13.2589
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1976MI05      Phys.Lett. 61B, 155 (1976)

T.Minamisono, J.W.Hugg, D.G.Mavis, T.K.Saylor, H.F.Glavish, S.S.Hanna

Measurement of the Magnetic Moment of ³⁹Ca by Use of a Polarized Proton Beam and NMR Detection

NUCLEAR MOMENTS ³⁹Ca; measured μ. NMR.

doi: 10.1016/0370-2693(76)90613-4
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1976MI11      Phys.Rev. C14, 376 (1976)

T.Minamisono, J.W.Hugg, J.R.Hall, D.G.Mavis, H.F.Glavish, S.S.Hanna

Measurement of the Magnetic Dipole Moment of β-Emitting ²⁵Al by Use of a Polarized Proton Beam and Nuclear Magnetic Resonance Detection

RADIOACTIVITY ²⁵Al [from ²⁸Si(polp, α)]; measured β(θ), polarization transfer, relaxation time, NMR; deduced μ. Polarized ²⁵Al.

doi: 10.1103/PhysRevC.14.376
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1976MI16      Phys.Rev. C14, 2335 (1976)

T.Minamisono, J.W.Hugg, J.R.Hall, D.G.Mavis, D.L.Clark, S.S.Hanna

Measurement of the Magnetic Dipole Moment of β-Emitting ³¹S by Use of A Polarized Proton Beam and Nuclear Magnetic Resonance Detection

RADIOACTIVITY ³¹S [from ³¹P(polp, n)]; measured β asymmetry, polarization transfer, relaxation time NMR; deduced μ. polarized ³¹S.

doi: 10.1103/PhysRevC.14.2335
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1976MI21      Hyperfine Interactions 2, 315 (1976)

T.Minamisono, J.W.Hugg, D.G.Mavis, T.K.Saylor, S.M.Lazarus, H.F.Glavish, S.S.Hanna

Nuclear Moment Determination of β-Emitting Nuclei by Use of Nuclear Reactions Initiated with Fast Polarized Beams

NUCLEAR MOMENTS ⁸Li; measured nuclear spin I, quadrupole moment. ³⁹Ca; measured μ.

doi: 10.1007/BF01021156
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1976TA13      Phys.Rev. C14, 514 (1976)

S.L.Tabor, B.A.Watson, S.S.Hanna

Interaction Sizes of the Even Neodymium Isotopes from Elastic α Scattering

NUCLEAR REACTIONS ^{142,144,146,148,150}Nd(α, α), E=11-19 MeV; measured σ(E, θ); deduced nuclear interaction size, optical model parameters.

doi: 10.1103/PhysRevC.14.514
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1975BO51      Phys.Lett. 54A, 293 (1975)

P.Boolchand, M.Tenhover, S.Jha, G.Langouche, B.B.Triplett, S.S.Hanna, P.Jena

Magnetic Hyperfine Structure of ¹²⁵Te in Ferromagnetic Pd₂MnSb

NUCLEAR MOMENTS ¹²⁵Te; measured g-factor ratio in Pd₂MnSb. Mossbauer experiment.

doi: 10.1016/0375-9601(75)90264-9
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1975FI08      Nucl.Phys. A251, 1 (1975)

S.Fiarman, S.S.Hanna

Energy Levels of Light Nuclei A = 3

COMPILATION ³H, ³He; compiled, evaluated structure data.

doi: 10.1016/0375-9474(75)90700-9
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1975KU06      Phys.Rev. C11, 1525 (1975)

E.Kuhlmann, E.Ventura, J.R.Calarco, D.G.Mavis, S.S.Hanna

E1 and E2 Strength in ²⁴Mg and ²⁶Mg Observed in α-Capture Reactions

NUCLEAR REACTIONS ²⁰Ne(α, γ), E=2.5-20 MeV; ²²Ne(α, γ), E=4.5-16 MeV; measured σ(E, Eγ, θ(γ)). ^24,26Mg deduced E1, E2 strength. Enriched targets.

doi: 10.1103/PhysRevC.11.1525
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1975MI04      Phys.Rev.Lett. 34, 1465 (1975)

T.Minamisono, J.W.Hugg, D.G.Mavis, T.K.Saylor, S.M.Lazarus, H.F.Glavish, S.S.Hanna

Measurement of the Quadrupole Moment of ⁸Li by Use of a Polarized Deuteron Beam and NMR Detection

RADIOACTIVITY ⁸Li [from ⁷Li(polarized d, p)]; measured β-asymmetry; deduced quadrupole moment.

doi: 10.1103/PhysRevLett.34.1465
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1975TA01      Phys.Rev. C11, 198 (1975)

S.L.Tabor, B.A.Watson, S.S.Hanna

Matter Radii of the Even Tin Isotopes from Elastic α and ¹⁶O Scattering

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(α, α), E=9-17 MeV; ^{116,118,120,122,124}Sn(¹⁶O, ¹⁶O), E=46-59 MeV; measured σ(E, θ); deduced nuclear size. Enriched targets.

doi: 10.1103/PhysRevC.11.198
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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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1974KU12      Phys.Rev. C10, 1593 (1974)

E.Kuhlmann, S.S.Hanna

Analog Transitions in the A = 30 System

NUCLEAR REACTIONS ²⁹Si(p, γ), E=0.7-0.75 MeV; measured σ(E, Eγ, θ). ³⁰P level deduced γ-branching.

doi: 10.1103/PhysRevC.10.1593
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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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1973HA62      Nucl.Phys. A216, 221 (1973)

M.Hasinoff, G.A.Fisher, S.S.Hanna

Isospin Splitting of Giant E1 Excitations in ⁹⁰Zr

NUCLEAR REACTIONS ⁸⁹Y(p, γ), Ep=5.4-17.0 MeV; measured σ(Ep;Eγ, θ(γ)). ⁹⁰Zr deduced giant dipole resonances, analog resonances, resonance parameters, isospin splitting, γ-hindrance, level-width. Natural target.

doi: 10.1016/0375-9474(73)90466-1
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1973RU04      Nucl.Phys. A210, 133 (1973)

P.B.Russell, G.L.Latshaw, S.S.Hanna, G.Kaindl

Change of the Nuclear Charge Radius in Excitation of 2⁺ Levels in Ytterbium Isotopes

NUCLEAR REACTIONS ^{170,172,174,176}Yb(γ, γ), E=84.3, 78.7, 76.5, 82.1 keV, respectively; measured single-line Mossbauer absorption. ^{170,172,174,176}Yb levels deduced isomer shifts, Δ < r2 > . ¹⁷⁰Yb level deduced dispersion term 2Xi.

doi: 10.1016/0375-9474(73)90509-5
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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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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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1972HA62      Nucl.Phys. A195, 78 (1972)

M.Hasinoff, G.A.Fisher, P.Kurjan, S.S.Hanna

Isospin Splitting of Giant E1 Excitations in the N = 82 Nucleus ¹⁴²Nd

NUCLEAR REACTIONS ¹⁴¹Pr(p, γ), Ep=6-17 MeV; measured σ(Ep;Eγ, θ(γ)). ¹⁴²Nd deduced giant dipole resonances, analog resonances, resonance parameters, isospin splitting. Natural targets.

doi: 10.1016/0375-9474(72)90722-1
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1972HA63      Nucl.Phys. A195, 91 (1972)

S.S.Hanna, M.Hass, Z.Shkedi, Y.S.Horowitz

Search for a Possible Jπ = 0⁺, T = 2 Resonance in ⁹Be(tau, γ, γ)¹²C

NUCLEAR REACTIONS ⁹Be(³He, γ), E=1.73-1.76 MeV; measured σ(E;θ=0°). ⁹Be(p, γ), E=1.083 MeV; measured Eγ. ¹⁰B deduced resonance, level-width. ¹²C deduced limit on 0+, T=2 resonance. Natural target.

doi: 10.1016/0375-9474(72)90723-3
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1972KU24      Nucl.Phys. A193, 497 (1972)

H.M.Kuan, G.L.Latshaw, W.J.O'Connell, D.W.Heikkinen, E.G.Adelberger, A.V.Nero, S.S.Hanna

Observation of the Second T = 2 State of ²⁰Ne as a Compound Resonance in the ¹⁹F + p Reactions

NUCLEAR REACTIONS ¹⁹F(p, p), (p, n), (p, α), (p, γ), Ep=5.65-6.20 MeV; measured σ(E, θ). ²⁰Ne second T=2 resonance deduced levels, J, π, T, level-width.

doi: 10.1016/0375-9474(72)90336-3
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1972SU08      Part.Nucl. 4, 175 (1972)

M.Suffert, W.Feldman, S.S.Hanna

Resonance in ¹²C at 18.13 MeV Observed in ¹¹B(p, γ)¹²C*(15.1)

NUCLEAR REACTIONS ¹¹B(p, γ), E < 3 MeV; measured σ(E;Eγ, θ(γγ)). ¹²C deduced resonance, level-width, J, π.

1971BE60      Nucl.Phys. A178, 155 (1971)

Z.Berant, M.B.Goldberg, G.Goldring, S.S.Hanna, H.M.Loebenstein, I.Plesser, M.Popp, J.S.Sokolowski, P.N.Tandon, Y.Wolfson

Hyperfine Interaction Studies of Light Nuclei in Highly Ionized Atoms Recoiling in Vacuum

NUCLEAR REACTIONS ¹⁹F(p, αγ), Ep=0.873 MeV; ¹²C(α, α'γ), Eα=10-17 MeV; ¹⁶O(α, α'γ), Eα=17.9 MeV; ¹⁸O(α, α'γ), Eα=18.0 MeV; ¹⁹F(α, α'γ), Eα=10.6, 12.3 MeV; ²⁴Mg(α, α'γ), Eα=11.4 MeV; ¹²C(¹⁶O, αγ), E(¹⁶O)=28.0-30.5 MeV; ¹²C(¹⁸O, ¹⁸O'γ), E(¹⁸O)=33-35 MeV; measured σ(θ(γ)), recoils in vacuum, metals; deduced ionic fields. Natural, enriched targets.

doi: 10.1016/0375-9474(71)90195-3
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1971HA25      Phys.Rev. C3, 2198 (1971)

S.S.Hanna, K.Nagatani, W.R.Harris, J.W.Olness

Lifetime of the First Excited State of ¹¹Be

NUCLEAR REACTIONS ⁹Be(t, pγ), E=3.5 MeV; measured Doppler shift attenuation. ¹¹Be deduced level, T_1/2.

doi: 10.1103/PhysRevC.3.2198
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1970KU09      Nucl.Phys. A151, 129 (1970)

H.M.Kuan, M.Hasinoff, W.J.O'Connell, S.S.Hanna

The Giant Dipole Resonances in ¹¹C and ¹⁵O Observed with the Reactions ¹⁰B(p, γ)¹¹C and ¹⁴N(p, γ)¹⁵O

NUCLEAR REACTIONS ¹⁰B(p, γ), E=2.6-17 MeV; ¹⁴N(p, γ), E=2.2-19 MeV; measured σ(E;Eγ, θ(γ)). ¹¹C, ¹⁵O deduced resonances, J, γ, level-width, giant dipole resonances. Enriched ¹⁰B target.

doi: 10.1016/0375-9474(70)90973-5
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1970RU04      Phys.Lett. 32B, 35 (1970)

P.B.Russell, G.D.Sprouse, G.L.Latshaw, S.S.Hanna, G.M.Kalvius

Isomer Shift of the 2⁺ State in ¹⁶⁰Gd and ¹⁵⁸Gd from Recoil Implantation Mossbauer Studies

NUCLEAR REACTIONS ^158,160Gd(γ, γ), E=79.5, 75.3 keV; measured Mossbauer effect; deduced isomer shift. ^158,160Gd deduced change in nuclear charge radius upon excitation.

doi: 10.1016/0370-2693(70)90329-1
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1969HA41      Phys.Letters 30B, 337 (1969)

M.Hasinoff, G.A.Fisher, H.M.Kuan, S.S.Hanna

Isospin Splitting of E1 Resonances in ⁸⁸Sr and ⁹⁰Zr

NUCLEAR REACTIONS ⁸⁷Rb(p, γ), E = 4-15 MeV; ⁸⁷Rb(p, p), E = 5-12 MeV; measured σ(E;Eγ), σ(E). ⁸⁸Sr deduced resonances, level-width, isospin splitting. ⁸⁹Y(p, γ), E = 7-14 MeV; ⁸⁹Y(p, p), E = 10-14 MeV; measured σ(E;Eγ, θ(γ)), σ(E). ⁹⁰Zr deduced resonances, level-width, isospin splitting.

doi: 10.1016/0370-2693(69)90498-5
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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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1969SP05      Nucl.Phys. A137, 658 (1969)

G.D.Sprouse, S.S.Hanna

Lifetimes and Magnetic Moments of Levels in ⁵⁷Fe

NUCLEAR REACTIONS ^56,57Fe(¹⁶O, ¹⁶O'γ), E=14-35 MeV; ⁵⁷Fe(α, α'γ), E=3.15 MeV; measured σ(Eγ, θ, H), DSA. ^56,57Fe levels deduced B(E2), T_1/2, δ. ⁵⁷Fe level deduced g. Natural, enriched targets.

doi: 10.1016/0375-9474(69)90100-6
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1968DI04      Phys.Rev. 168, 1169 (1968)

F.S.Dietrich, M.Suffert, A.V.Nero, S.S.Hanna

Gamma Decay of the Lowest T = 3/2 State of ¹³N

NUCLEAR STRUCTURE ¹²C, ¹³N; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.168.1169
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1968FI09      Phys.Rev. 176, 1130(1968)

T.R.Fisher, S.S.Hanna, D.C.Healey, P.Paul

Lifetimes of Levels in A = 10 Nuclei

NUCLEAR REACTIONS ⁹Be(d, p), (d, n), E=1.7 MeV; ¹⁰B(p, n), (p, p'), E=2-9.5 MeV; measured Doppler-shift attenuation. ¹⁰Be, ¹⁰B, ¹⁰C levels deduced T_1/2.

doi: 10.1103/PhysRev.176.1130
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1968RI16      Phys.Rev. 176, 1140(1968)

F.Riess, P.Paul, J.B.Thomas, S.S.Hanna

Lifetimes of Levels in ¹²C, ¹³C, and ¹³N

NUCLEAR REACTIONS ¹³C(p, p'), E=4.1, 4.125, 4.55 MeV; ¹²C(d, p), E=1.79, 2.715, 3.60 MeV; ¹²C(p, γ), E approx. 0.459 MeV; ¹⁰B(α, p), E=2.9 MeV; measured Doppler - shift attenuation. ^12,13C, ¹³N levels, deduced T_1/2.

doi: 10.1103/PhysRev.176.1140
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1967BL23      Phys.Letters 25B, 405 (1967)

J.L.Black, W.J.O'Connell, S.S.Hanna, G.L.Latshaw

Inverse Photonuclear Process in ¹⁶O

NUCLEAR STRUCTURE ¹⁶O, ¹⁵N; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90159-1
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1967HA40      Contrib.Intern.Conf.Nucl.Struct., Tokyo, p.198 (1967)

S.S.Hanna, G.M.Kalvius, G.D.Sprouse

Magnetic Moments, Polarizations, and Lifetimes by Recoil Implantation

NUCLEAR STRUCTURE ⁵⁷Fe; measured not abstracted; deduced nuclear properties.

1967KU02      Phys.Letters 24B, 566 (1967)

H.M.Kuan, S.S.Hanna

T = 3/2 States in ¹³N Observed in the Reaction ¹²C(p, p)¹²C

NUCLEAR STRUCTURE ¹³N, ¹²C; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90390-5
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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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1967PA01      Phys.Letters 24B, 51 (1967)

P.Paul, T.R.Fisher, S.S.Hanna

Transition Rates of Analog Levels in A = 10 Nuclei

NUCLEAR STRUCTURE ¹⁰B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90337-1
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1967RI09      Phys.Rev.Letters 19, 367 (1967)

F.Riess, W.J.O'Connell, D.W.Heikkinen, H.M.Kuan, S.S.Hanna

Observation of T = 2 Level in ²⁴Mg as a Compound-Nucleus Resonance

NUCLEAR STRUCTURE ²⁴Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.19.367
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1966FI01      Phys.Rev.Letters 16, 850 (1966)

T.R.Fisher, S.S.Hanna, P.Paul

Transition Rates in B¹⁰ and the β Decay of C¹⁰

NUCLEAR STRUCTURE ⁹Be, ¹⁰B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.16.850
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1966PA11      Phys.Rev. 147, 774 (1966)

P.Paul, J.B.Thomas, S.S.Hanna

Lifetimes of the First Excited States of Li⁷ and Be⁷

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

doi: 10.1103/PhysRev.147.774
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1966SE03      Phys.Rev. 145, 736 (1966)

R.E.Segel, P.P.Singh, S.S.Hanna, M.A.Grace

Gamma Rays from B¹⁰+p; Decay Schemes and Excitation Functions

NUCLEAR STRUCTURE ¹⁰C, ¹⁰B, ⁷Be; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.145.736
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1965HA34      Phys.Rev. 139, A722 (1965)

S.S.Hanna, R.S.Preston

Mossbauer Cross Section of Fe⁵⁷ in Iron

NUCLEAR REACTIONS ⁵⁷Fe(γ, γ), E=14.4 keV; measured Mossbauer effect in iron.

1965SE06      Phys.Rev. 139, B818 (1965)

R.E.Segel, S.S.Hanna, R.G.Allas

States in C¹² Between 16.4 and 19.6 MeV

NUCLEAR STRUCTURE ¹²C, ¹¹B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B818
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0332.

1965SI11      Nucl.Phys. 65, 577(1965)

P.P.Singh, R.E.Segel, L.Meyer-Schutzmeister, S.S.Hanna, R.G.Allas

Giant Resonances and Fine Structure in Si²⁸ from the Al²⁷(p, γ)Si²⁸ Reaction

NUCLEAR REACTIONS ²⁷Al(p, γ), E=4-12.5 MeV; measured σ(E; Eγ, θ). ²⁸Si deduced mean level width. Natural target.

doi: 10.1016/0029-5582(65)90326-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1485.

1965SP06      Nucl.Phys. 74, 177 (1965)

G.D.Sprouse, S.S.Hanna

Gamma Ray Transitions in ⁵⁷Fe

RADIOACTIVITY ⁵⁷Co; measured Eγ, Iγ; deduced log ft. ^56,58Co; measured Eγ. ⁵⁷Fe(α, α'γ), E = 3.3 MeV; measured Eγ, Iγ. Enriched target.

doi: 10.1016/0029-5582(65)90257-9
Citations: PlumX Metrics

1964AL20      Nucl. Phys. 58, 122 (1964)

R.G.Allas, S.S.Hanna, L.Meyer-Schutzmeister, R.E.Segel

Radiative Capture of Protons by B¹¹ and the Giant Dipole Resonance in C¹²

NUCLEAR REACTIONS ¹¹B(p, γ), Ep=4-14 MeV; measured σ(E, θ), Eγ. Enriched target.

doi: 10.1016/0029-5582(64)90527-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0344.

1964HA39      Bull.Am.Phys.Soc. 9, No.7, 719, K10 (1964)

S.S.Hanna, G.D.Sprouse

Transitions in Ta¹⁸¹ from the Decay of W¹⁸¹

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

1964HE21      Rev.Mod.Phys. 36, 407 (1964)

J.Heberle, M.Schulhof, S.S.Hanna

Mossbauer Effect in Fe⁵⁷ and Sn¹¹⁹ Metals in Large External Magnetic Fields

NUCLEAR STRUCTURE ¹¹⁹Sn; measured not abstracted; deduced nuclear properties.