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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 T1/2.

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 T1/2.

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 122,124,126,128,130Te(35Cl, 35Cl'), E=70 MeV; measured γ(35Cl)(θ, H) following Coulomb excitation. 122,124,126,128,130Te 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 T1/2, 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 T1/2.

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1223.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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

doi: 10.1103/PhysRevC.14.514
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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

doi: 10.1103/PhysRevC.11.198
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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

doi: 10.1016/0375-9474(73)90509-5
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2680.


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
Citations: PlumX Metrics


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, T1/2.

doi: 10.1103/PhysRevC.3.2198
Citations: PlumX Metrics


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), T1/2, 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
Citations: PlumX Metrics


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 T1/2.

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 T1/2.

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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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
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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
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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

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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.


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