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NSR database version of April 11, 2024.

Search: Author = P.H.Stelson

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1993BR11      Phys.Rev. C48, 1147 (1993)

M.E.Brandan, J.R.Alfaro, A.Menchaca-Rocha, J.Gomez del Campo, G.R.Satchler, P.H.Stelson, H.J.Kim, D.Shapira

Elastic Scattering of 58Ni + 27Al at Near-Barrier Energies

NUCLEAR REACTIONS 27Al(58Ni, 58Ni), E=155-220 MeV; measured σ(E, θ); deduced optical model parameters, potential volume integrals. Phenomenological folding model, dispersion relations analyses.

doi: 10.1103/PhysRevC.48.1147
Citations: PlumX Metrics


1993SH06      Phys.Rev. C47, 1666 (1993)

D.Shapira, P.H.Stelson

Role of Neutron Flow in the Enhancement of Heavy Ion Fusion at Energies Below the Coulomb Barrier and the Systematics of Threshold Barriers

NUCLEAR REACTIONS 89,90Zr(51Ti, X), E(cm) ≈ 98-120 MeV; calculated sub-barrier fusion σ(E); deduced neutron flow features. Many other target + projectile systems included.

doi: 10.1103/PhysRevC.47.1666
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1991KI01      Phys.Rev. C43, 1231 (1991)

H.J.Kim, J.Gomez del Campo, D.Shapira, P.H.Stelson, D.Napoli

Multinucleon-Transfer Reactions for the 50Ti + 93Nb System at Sub- and Near-Barrier Energies

NUCLEAR REACTIONS 50Ti(93Nb, X), E=283.1-306.9 MeV; measured fragment energy, charge spectra, σ(fragment θ); deduced multi-nucleon transfer probabilities.

doi: 10.1103/PhysRevC.43.1231
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1991RO01      Phys.Lett. 254B, 25 (1991)

N.Rowley, G.R.Satchler, P.H.Stelson

On the ' Distribution of Barriers ' Interpretation of Heavy-Ion Fusion

NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 55-65 MeV; analyzed data; deduced potential barriers distribution features.

doi: 10.1016/0370-2693(91)90389-8
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1990ST04      Phys.Rev. C41, 1584 (1990)

P.H.Stelson, H.J.Kim, M.Beckerman, D.Shapira, R.L.Robinson

Fusion Cross Sections for 46,50Ti + 90Zr, 93Nb and Some Systematics of Heavy-Ion Fusion at Barrier and Subbarrier Energies

NUCLEAR REACTIONS, ICPND 90Zr, 93Nb(46Ti, X), (50Ti, X), E(cm)=100.29-117.6 MeV; measured σ(fragment θ). 58,64Ni(32S, X), (28Si, X), E(cm)=56-62 MeV; 93Nb, 100Mo(32S, X), (36S, X), E(cm)=71-91 MeV; 184W(16O, X), E(cm) ≈ 60-100 MeV; calculated fusion σ(E).

doi: 10.1103/PhysRevC.41.1584
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1988AH01      Phys.Rev. C37, 1836 (1988)

A.Ahmad, G.Bomar, H.Crowell, J.H.Hamilton, H.Kawakami, C.F.Maguire, W.G.Nettles, R.B.Piercey, A.V.Ramayya, R.Soundranayagam, R.M.Ronningen, O.Scholten, P.H.Stelson

Coulomb Excitation of 144, 146, 148, 150Nd

NUCLEAR REACTIONS 144,146,148,150Nd(α, α'), E=10.5, 11 MeV; measured σ(Eα) following Coulomb excitation. 144,146,148,150Nd deduced B(E2), B(E3), hexadecapole transition matrix element. Enriched targets.

doi: 10.1103/PhysRevC.37.1836
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1988BE41      Phys.Scr. 38, 657 (1988)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson, G.A.Leander, C.W.Reich

Coulomb Excitation of States in 229Th

NUCLEAR REACTIONS 229Th(α, α), (α, α'), E=17 MeV; measured σ(Eα), σ(Eα') following Coulomb excitation. 229Th levels deduced excitation probability, B(E2), intrinsic quadrupole, hexadecapole moments, J, π, K, Nilsson assignments.

doi: 10.1088/0031-8949/38/5/004
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1988HA26      Phys.Rev. C38, 572 (1988)

B.A.Harmon, D.Shapira, P.H.Stelson, B.L.Burks, K.A.Erb, B.Shivakumar, K.Teh, S.T.Thornton

Effect of Entrance Channel Asymmetry of Fusion Reactions Leading to Compound Nuclei with A = 40, 42

NUCLEAR REACTIONS 12C(28Si, X), E=6.4, 7.8, 9.4 MeV/nucleon; 12C(30Si, X), E=5.2, 5.7, 6.4, 7.5, 8.3 MeV/nucleon; measured fusion σ; deduced entrance channel asymmetry role.

doi: 10.1103/PhysRevC.38.572
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1988KI09      Phys.Rev. C38, 2081 (1988)

H.J.Kim, J.Gomez del Campo, M.M.Hindi, D.Shapira, P.H.Stelson

Transfer Reactions for the 50Ti + 90Zr System below the Coulomb Barrier

NUCLEAR REACTIONS 50Ti(90Zr, X), E=274-303 MeV; measured quasielastic σ(θ); deduced (90Zr, 49Ti), (90Zr, 51V) reaction probabilities.

doi: 10.1103/PhysRevC.38.2081
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1988SH03      Phys.Rev. C37, 652 (1988)

B.Shivakumar, D.Shapira, P.H.Stelson, S.Ayik, B.A.Harmon, K.Teh, D.A.Bromley

28Si + 14N Orbiting Interaction

NUCLEAR REACTIONS 14N(28Si, 14N), E=100 MeV; 14N(28Si, 16O), E=140 MeV; 14N(28Si, 12C), E=100-170 MeV; measured ejectile yields. 28Si(14N, X), E=100-170 MeV; measured orbiting σ(E) for X=10,11B, 11,12,13C, 13,14,15N, 15,16,17O, 17,18,19F, 19,20,21Ne; deduced critical angular momentum.

doi: 10.1103/PhysRevC.37.652
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1988SI01      Phys.Rev. C37, 158 (1988)

J.D.Silk, H.D.Holmgren, D.L.Hendrie, T.J.M.Symons, G.D.Westfall, P.H.Stelson, S.Raman, R.L.Auble, J.R.Wu, K.Van Bibber

Fragmentation of 16O Projectiles at 100 MeV per Nucleon

NUCLEAR REACTIONS 27Al(16O, 12CX), E=100 MeV/nucleon; measured invariant σ vs rapidity. 27Al(16O, X), E=100 MeV/nucleon; measured σ(fragment θ), σ vs fragment mass for X=7,9,10Be, 10,11,12B, 10,11,12,13,14C, 13,14,15N; deduced reaction mechanism.

doi: 10.1103/PhysRevC.37.158
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1988ST08      Phys.Lett. 205B, 190 (1988)

P.H.Stelson

Neutron Flow between Nuclei as the Principal Enhancement Mechanism in Heavy-Ion Subbarier Fusion

NUCLEAR REACTIONS 58Ni(58Ni, X), E ≈ 93-110 MeV; 64Ni(64Ni, X), E(cm) ≈ 90-110 MeV; calculated fusion σ(E); deduced barrier distribution, neutron flow role.

doi: 10.1016/0370-2693(88)91647-4
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1987GO01      Phys.Rev. C35, 137 (1987)

J.Gomez del Campo, D.E.DiGregorio, J.A.Biggerstaff, Y.D.Chan, D.C.Hensley, P.H.Stelson, D.Shapira, M.E.Ortiz

Correlations between α Particles and Evaporation Residues for the 14N + 12C Reaction at E(14N) = 180 MeV

NUCLEAR REACTIONS 12C(14N, xα), E=180 MeV; measured α(evaporation residues)(θ); deduced equilibrium, nonequilibrium effects. ΔE-E solid state detectors.

doi: 10.1103/PhysRevC.35.137
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1987RA01      At.Data Nucl.Data Tables 36, 1 (1987)

S.Raman, C.H.Malarkey, W.T.Milner, C.W.Nestor, Jr., P.H.Stelson

Transition Probability, B(E2), from the Ground to the First-Excited 2+ State of Even-Even Nuclides

COMPILATION A=6-254; compiled, evaluated 2+ level energies, B(E2), T1/2, β2, β22(sp), EWSR, intrinsic quadrupole moments.

doi: 10.1016/0092-640X(87)90016-7
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1986SC30      Phys.Rev. C34, 1962 (1986)

O.Scholten, R.M.Ronningen, A.Y.Ahmed, G.O.Bomar, H.L.Crowell, J.H.Hamilton, H.Kawakami, C.F.Maguire, W.G.Nettles, R.B.Piercey, A.V.Ramayya, R.Soundranayagam, P.H.Stelson

Mass Dependence of Effective Charges in the Interacting-Boson Model

NUCLEAR REACTIONS 144,146,148,150Nd(α, α'), E not given; measured Coulomb excitation. 144,146,148,150Nd levels deduced B(E2). Magnetic spectrometer. Interacting boson model.

NUCLEAR STRUCTURE 142,144,146,148,150Nd; calculated B(E2), effective charges. Interacting boson model.

doi: 10.1103/PhysRevC.34.1962
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1986SH25      Phys.Rev.Lett. 57, 1211 (1986)

B.Shivakumar, D.Shapira, P.H.Stelson, M.Beckerman, B.A.Harmon, K.Teh, D.A.Bromley

Equilibration in Orbiting Reactions

NUCLEAR REACTIONS 14N(28Si, 14N), E=100-170 MeV; measured ejectile yield at θ=15°, absolute orbiting σ(E). 14N(28Si, 12C), (28Si, 16O), E=100-170 MeV; measured absolute orbiting σ(E); deduced charge, mass equilibration.

doi: 10.1103/PhysRevLett.57.1211
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1985SH30      Nucl.Instrum.Methods Phys.Res. B10/11, 436 (1985)

D.Shapira, J.Gomez del Campo, J.L.C.Ford, Jr., B.Shivakumar, P.H.Stelson, B.A.Harmon, R.L.Parks, S.T.Thornton

Nuclear Physics Experiments with the ORNL-HHIRF Supersonic Gas Jet Target

NUCLEAR REACTIONS 14N(28Si, X), E=150 MeV; measured fragment spectra; deduced orbiting process products mass, charge distribution features.

doi: 10.1016/0168-583X(85)90285-X
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1984GO05      Phys.Rev. C29, 1722 (1984)

J.Gomez del Campo, J.A.Biggerstaff, R.A.Dayras, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad

Comparison of Fusion Cross Sections for the 10B + 16O and 12C + 14N Systems

NUCLEAR REACTIONS, ICPND 12C(14N, X), E=158, 248 MeV; 10B(16O, X), E=203.6 MeV; measured σ(fragment θ, E) for fragment Z=3, 10, fusion, reaction, direct σ(E), fragment velocity spectra. 16O(10B, X), E=42-169.7 MeV; measured fusion, reaction σ(E). 10B(16O, X), E=203.6 MeV; measured evaporation residue σ(θ). 12C(14N, X), E=182 MeV; measured evaporation residue relative yield. Monte Carlo Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.29.1722
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1983AU06      Phys.Rev. C28, 1552 (1983)

R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, C.Y.Wong, D.L.Hendrie, H.D.Holmgren, J.D.Silk

Light Ion Emission from Reactions Induced by 0.8-2.4 GeV 16O Projectiles

NUCLEAR REACTIONS Ni(16O, X), E=0.8, 1.6, 2.4 GeV; Au(16O, X), E=1.6, 2.4 GeV; Al, Sn(16O, X), E=1.6 GeV; measured σ(E, θ) for X=p, d, t, 3He, 4He; deduced model parameters.

doi: 10.1103/PhysRevC.28.1552
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1983RA21      Phys.Rev. C28, 602 (1983); Erratum Phys.Rev. C29, 344 (1984)

S.Raman, B.Fogelberg, J.A.Harvey, R.L.Macklin, P.H.Stelson, A.Schroder, K.-L.Kratz

Overlapping β Decay and Resonance Neutron Spectroscopy of Levels in 87Kr

NUCLEAR REACTIONS 86Kr(n, n), (n, X), E=1-400 keV; measured σ(E), transmission. 86Kr(n, γ), E=1-90 keV; measured σ(capture) vs E. 87Kr deduced resonances, L, J, π, Γγ, (gΓγ), (gΓn), (gΓnΓγ/Γ), neutron strength function, Maxwellian < σ >. Enriched target. Multi-level R-matrix analysis.

RADIOACTIVITY 87Br(β-), (β-n) [from 235U(n, F)]; measured Eγ, Iγ, γγ-coin, β-delayed En; deduced J, π, log ft, Gamow-Teller matrix elements. 87Kr deduced levels, β-branching, J, π.

doi: 10.1103/PhysRevC.28.602
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12837.


1983SH25      Phys.Rev. C28, 1148 (1983)

D.Shapira, D.DiGregorio, J.Gomez del Campo, R.A.Dayras, J.L.C.Ford, Jr., A.H.Snell, P.H.Stelson, R.G.Stokstad, F.Pougheon

Fusion and Peripheral Processes in the Collisions of 20Ne + 20Ne and 20Ne + 16O

NUCLEAR REACTIONS, ICPND 20Ne, 16O(20Ne, 20Ne), (20Ne, X), E=80-160 MeV; measured elastic σ, σ(fragment θ, E), σ(θ) for Z=6, 7, 8, 9, fusion σ(E), reaction σ, deep inelastic σ; deduced fusion potential parameters, entrance channel effects. Monte Carlo simulation.

doi: 10.1103/PhysRevC.28.1148
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1982AU07      Phys.Rev.Lett. 49, 441 (1982)

R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, D.L.Hendrie, H.D.Holmgren, J.D.Silk, H.Breuer

Target-A Dependence of Light-Ion Emission from Reactions Induced by 100-MeV/u 16O

NUCLEAR REACTIONS Al, Ni, Sn, Au(16O, p), (16O, d), (16O, t), (16O, 3He), (16O, α), E=100 MeV/nucleon; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, E(3He)), σ(θ, Eα), inclusive reactions; deduced reaction mechanism, moving source parameters, target mass effects.

doi: 10.1103/PhysRevLett.49.441
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1982BE12      Phys.Rev. C25, 1637 (1982)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson

Coulomb Excitation of Ground Band Rotational States in 249Bk

NUCLEAR REACTIONS 249Bk(α, α), (α, α'), E=17.06 MeV; measured σ(Eα, θ=150°). 249Bk levels deduced B(E2), B(M1), quadrupole moment, μ. Enriched target.

doi: 10.1103/PhysRevC.25.1637
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1981BE54      Phys.Rev. C24, 2723 (1981)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson

Coulomb Excitation of Rotational States and Ground-State Quadrupole Moment for 243Am

NUCLEAR REACTIONS 243Am(α, α'), E=17 MeV; measured σ(Eα', θ=150°), Coulomb excitation. 243Am levels deduced B(E2), B(E4), quadrupole moment. Enriched target.

doi: 10.1103/PhysRevC.24.2723
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1980SH10      Phys.Rev. C21, 1824 (1980)

D.Shapira, J.L.C.Ford, Jr., J.Gomez del Campo, P.H.Stelson

Backward Angle Cross Sections for 27Al + 16O Reaction Products

NUCLEAR REACTIONS 16O(27Al, X), E=105, 145 MeV; measured σ(θ); deduced evaporation residue, damped event σ.

doi: 10.1103/PhysRevC.21.1824
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1979FU04      Phys.Rev. C20, 670 (1979)

C.B.Fulmer, R.M.Wieland, D.C.Hensley, S.Raman, G.R.Satchler, A.H.Snell, P.H.Stelson, R.G.Stokstad

12C + 12C Transfer Reactions at 93.8 MeV

NUCLEAR REACTIONS 12C(12C, 11C), (12C, 11B), (12C, 10B), E=93.8 MeV; measured σ(θ). 13C, 13N levels deduced S. DWBA analysis.

doi: 10.1103/PhysRevC.20.670
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1979GO09      Phys.Rev.Lett. 43, 26 (1979)

J.Gomez del Campo, R.A.Dayras, J.A.Biggerstaff, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad

Comparison of Fusion Cross Sections for 10B + 16O → 26Al and 12C + 14N → 26Al

NUCLEAR REACTIONS 10B(16O, X), E(cm)=15-80 MeV; measured σ(fusion, E), σ(direct, E).

doi: 10.1103/PhysRevLett.43.26
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1979GO11      Phys.Rev. C19, 2170 (1979)

J.Gomez del Campo, R.G.Stokstad, J.A.Biggerstaff, R.A.Dayras, A.H.Snell, P.H.Stelson

Fusion and Peripheral Reactions of 12C + 14N at Energies up to 13 MeV/A

NUCLEAR REACTIONS 12C(14N, X), E=34.1-178.1 MeV; measured σ(θ) of evaporation residues; deduced fusion, direct, total σ. Hauser-Feshbach, optical model calculations.

doi: 10.1103/PhysRevC.19.2170
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1979MC04      Phys.Rev. C20, 2093 (1979)

F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, D.Shapira, P.H.Stelson

Coulomb Excitation of 183W

NUCLEAR REACTIONS 183W(α, α'γ), E=15 MeV; 183W(α, α'), E=13 MeV; measured Eγ, Iγ, γ(θ), σ(Eα'; θ). 183W levels deduced B(E2), B(M1), J, π, δ. Enriched targets.

doi: 10.1103/PhysRevC.20.2093
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1979SH22      Nucl.Instrum.Methods 163, 325 (1979)

D.Shapira, R.Dayras, J.L.C.Ford, Jr., J.Gomez del Campo, A.H.Snell, P.H.Stelson, R.G.Stokstad

A Gas Cell Target for Studying Fusion and Damped Collisions of Light Nuclei

NUCLEAR REACTIONS 20Ne(20Ne, X), E(cm)=83 MeV; measured fusion σ(θ). 16O(20Ne, X), E=131 MeV; measured evaporation residue energy for 12C, 14N, 16O, 19F, 20Ne, 23Na, 24Mg, 27Al, 28Si, 31P, 32S.

doi: 10.1016/0029-554X(79)90115-0
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1979ST10      Phys.Rev. C20, 655 (1979)

R.G.Stokstad, R.M.Wieland, G.R.Satchler, C.B.Fulmer, D.C.Hensley, S.Raman, L.D.Rickertsen, A.H.Snell, P.H.Stelson

Elastic and Inelastic Scattering of 12C by 12C from E = 35-63 MeV

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E(cm)=35-63 MeV; measured σ(E, θ). Optical model, DWBA, coupled-channels analysis.

doi: 10.1103/PhysRevC.20.655
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1978MC02      Nucl.Phys. A297, 51 (1978)

F.K.McGowan, W.T.Milner, R.L.Robinson, P.H.Stelson, Z.W.Grabowski

Coulomb Excitation of Vibrational-Like States in 166-170Er

NUCLEAR REACTIONS 166,168,170Er(α, α'γ), E=14 MeV; measured Iγ, Eγ, γ(θ). 166,168,170Er levels deduced B(E2), B(M1), B(E3), J, π, δ. Enriched targets.

doi: 10.1016/0375-9474(78)90198-7
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1977DA12      Nucl.Phys. A284, 484 (1977)

W.K.Dagenhart, P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner, S.Raman, W.K.Tuttle III

Coulomb Excitation of 115Sn

NUCLEAR REACTIONS 115Sn(α, α'γ), (α, α'), E=7.0-10.6 MeV; 115Sn(16O, 16O'γ), E=45 MeV; measured Eγ, Iγ, Iγ(θ), Doppler broadening, Eα'. 115Sn deduced levels, J, π, B(E2), B(M1), T1/2. Enriched targets.

doi: 10.1016/0375-9474(77)90398-0
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1977MA13      Nucl.Data Sheets 21, 1 (1977)

M.J.Martin, P.H.Stelson

Nuclear Data Sheets for A = 184

COMPILATION 184Hf, 184Ta, 184W, 184Re, 184Os, 184Ir, 184Pt, 184Au, 184Hg, 184Tl; compiled, evaluated structure data.

doi: 10.1016/S0090-3752(77)80091-4
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1977MC11      Nucl.Phys. A289, 253 (1977)

F.K.McGowan, W.T.Milner, R.O.Sayer, R.L.Robinson, P.H.Stelson

Coulomb Excitation of 182,184,186W and 166Er with 4He and 16O Ions

NUCLEAR REACTIONS 182,184,186W(α, α'γ), E=15 MeV; 186W(16O, 16O'γ), E=42 MeV; 166Er(α, α'γ), E=13.5 MeV; 166Er(16O, 16O'γ), E=42 MeV; measured Iγ, Eγ, γ(θ), αγ-coin, 16Oγ-coin. 182W levels deduced J. 184W levels deduced B(EL), J. 186W levels deduced B(EL), J, quadrupole moment. 166Er deduced quadrupole moment. Enriched, natural targets.

doi: 10.1016/0375-9474(77)90532-2
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1977RO08      Phys.Rev. C15, 1671 (1977)

R.M.Ronningen, J.H.Hamilton, A.V.Ramayya, L.Varnell, G.Garcia-Bermudez, J.Lange, W.Lourens, L.L.Riedinger, R.L.Robinson, P.H.Stelson, J.L.C.Ford, Jr.

Reduced Transition Probabilities of Vibrational States in 154-160Gd and 176-180Hf

NUCLEAR REACTIONS 154,156,158,160Gd, 176,178,180Hf(α, α'), E=11-17 MeV; measured σ(E, Eα', θ), Coulomb excitation. 154,156,158,160Gd, 176,178,180Hf levels deduced B(λ), M(λ). Enriched targets.

doi: 10.1103/PhysRevC.15.1671
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1977RO16      Phys.Rev. C16, 571 (1977)

R.M.Ronningen, R.B.Piercey, A.V.Ramayya, J.H.Hamilton, S.Raman, P.H.Stelson, W.K.Dagenhart

Coulomb Excitation of 2+ and 3- States in 192Pt and 194Pt

NUCLEAR REACTIONS 192,194Pt(α, α'), E=14.9 MeV; measured Coulomb excitation. 192,194Pt levels deduced B(E2), B(E3). Enriched targets.

doi: 10.1103/PhysRevC.16.571
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1977RO26      Phys.Rev. C16, 2208 (1977)

R.M.Ronningen, J.H.Hamilton, L.Varnell, J.Lange, A.V.Ramayya, G.Garcia-Bermudez, W.Lourens, L.L.Riedinger, F.K.McGowan, P.H.Stelson, R.L.Robinson, J.L.C.Ford, Jr.

E2 and E4 Reduced Matrix Elements of 154,156,158,160Gd and 176,178,180Hf

NUCLEAR REACTIONS 154,156,158,160Gd, 176,178,180Hf(α, α'), E=11.5-14 MeV; measured Coulomb excitation σ(E). 154,156,158,160Gd, 176,178,180Hf levels deduced β2, β4.

doi: 10.1103/PhysRevC.16.2208
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1977ST25      Phys.Lett. 70B, 289 (1977)

R.G.Stokstad, R.A.Dayras, J.Gomez del Campo, P.H.Stelson, C.Olmer, M.S.Zisman

Measurements of the Fusion of 12C + 14N and the Liquid-Drop Limit for 26Al

NUCLEAR REACTIONS 12C(14N, X), E=248 MeV; measured fusion σ.

doi: 10.1016/0370-2693(77)90660-8
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1976GO07      Nucl.Phys. A262, 125 (1976)

J.Gomez del Campo, M.E.Ortiz, A.Dacal, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, S.T.Thornton

Study of the Coherence Widths Γ in 28Si Measured by the 12C(16O, α) Reaction

NUCLEAR REACTIONS 12C(16O, α), E=40-46 MeV; measured σ(E) for θ=7°. 24Mg levels deduced Γ. 28Si deduced coherence widths. Hauser-Feshbach calculations, fluctuation analysis.

doi: 10.1016/0375-9474(76)90444-9
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1976GU05      Phys.Rev. C13, 691 (1976)

D.E.Gustafson, S.T.Thornton, T.C.Schweizer, J.L.C.Ford, Jr., P.D.Miller, R.L.Robinson, P.H.Stelson

High-Spin States of the Kπ = 3/2+ and 1/2+ Bands of 23Na

NUCLEAR REACTIONS 12C(15N, α), E=36-39.2 MeV; measured σ(E, Eα, θ). 23Na deduced levels, J, π, K. Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.13.691
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1976GU10      Nucl.Phys. A262, 96 (1976)

D.E.Gustafson, J.Gomez del Campo, R.L.Robinson, P.H.Stelson, P.D.Miller, J.K.Bair

High-Spin States of 26Mg Populated in the 12C(18O, α) Reaction

NUCLEAR REACTIONS 12C(18O, α), E=43.2-45.9 MeV; measured σ(E) at θlab=7°. 26Mg deduced levels, K, J, π. Hauser-Feshbach calculations, suggested J, π values.

doi: 10.1016/0375-9474(76)90442-5
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1976RO15      Phys.Rev. C14, 2126 (1976)

R.L.Robinson, J.K.Bair, C.H.Johnson, P.H.Stelson, W.B.Dress, C.M.Jones

Cross Sections for the Ni, Cu, Zn(16,18O, xn) Reactions Near the Coulomb Barrier

NUCLEAR REACTIONS 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn(16O, xn), (18O, xn), E=36-55 MeV; measured total σ(E).

doi: 10.1103/PhysRevC.14.2126
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1976ST07      Phys.Rev.Lett. 36, 1529 (1976)

R.G.Stokstad, J.Gomez del Campo, J.A.Biggerstaff, A.H.Snell, P.H.Stelson

Fusion of 14N + 12C at Energies up to 178 MeV

NUCLEAR REACTIONS 12C(14N, X), E=43-178 MeV; measured fusion σ(E).

doi: 10.1103/PhysRevLett.36.1529
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1976TU02      Phys.Rev. C13, 1036 (1976)

W.K.Tuttle III, P.H.Stelson, R.L.Robinson, W.T.Milner, F.K.McGowan, S.Raman, W.K.Dagenhart

Coulomb Excitation of 113,115In

NUCLEAR REACTIONS 113,115In(α, α'γ), E=9.4, 10, 10.6 MeV; 113,115In(16O, 16O'γ), E=42, 45 MeV; measured Coulomb excitation, DSA, Eγ, Iγ, γ(θ). 113,115In deduced levels, J, π, T1/2, B(E2), B(M1).

doi: 10.1103/PhysRevC.13.1036
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1975GO25      Phys.Rev. C12, 1247 (1975)

J.Gomez del Campo, D.E.Gustafson, R.L.Robinson, P.H.Stelson, P.D.Miller, J.K.Bair, J.B.McGrory

Population of High-Spin States in 23Na Through the 11B(16O, α) Reaction

NUCLEAR REACTIONS 11B(16O, α), E=41.6-45.4 MeV; measured σ(E, Eα, θ). 23Na deduced levels, J, π.

doi: 10.1103/PhysRevC.12.1247
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1975LE22      Phys.Rev. C12, 1483 (1975)

I.Y.Lee, J.X.Saladin, J.Holden, J.O'Brien, C.Baktash, C.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle

Deformation Parameters of the Charge Distribution and the Optical Potential for Some Nuclei in and Near the Rare Earth Region

NUCLEAR REACTIONS 154Sm(α, α'), E=11-19 MeV; 166Er(α, α'), E=12.5-19.5 MeV; 182W(α, α'), E=13-21 MeV; measured σ(Eα'). 168Er(α, α'), E=13-19 MeV; 184W(α, α'), E=12.5-19 MeV; 186W(α, α'), E=13.25-19 MeV; measured σ(Eα', θ). 154Sm, 166,168Er, 182,184,186W deduced M(E2), M(E4), charge deformations, optical potential deformations.

doi: 10.1103/PhysRevC.12.1483
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1974FO11      Nucl.Phys. A226, 189 (1974)

J.L.C.Ford, Jr., J.Gomez del Campo, R.L.Robinson, P.H.Stelson, S.T.Thornton

States in 24Mg Populated by the 10B(16O, d)24Mg and 12C(16O, α)24Mg Reactions

NUCLEAR REACTIONS 10B(16O, d), E=44-46 MeV; 12C(16O, α), E=40-46 MeV; measured σ(E). 24Mg deduced levels, J.

doi: 10.1016/0375-9474(74)90401-1
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1974FO15      Z.Phys. 269, 147 (1974)

J.L.C.Ford, Jr., J.Gomez del Campo, R.L.Robinson, P.H.Stelson, S.T.Thornton

Measurements and Hauser-Feshbach Analysis of the 10B(16O, 6Li)20Ne Reaction

NUCLEAR REACTIONS 10B(16O, 6Li), E=44.4-46 MeV; measured σ(E, E(6Li)). 20Ne deduced levels. Hauser-Feshbach calculations.

doi: 10.1007/BF01669056
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1974GO10      Phys.Rev. C9, 1258 (1974)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, S.T.Thornton

Study of the 10B(16O, α)22Na Reaction

NUCLEAR REACTIONS 10B(16O, α), E(16O)=40-46 MeV, measured σ(E) for θ(lab)=7°; E(16O)=46 MeV, measured σ(θ). 22Na deduced levels. Fluctuation analysis. Hauser-Feshbach calculations, suggested J values. Enriched targets.

doi: 10.1103/PhysRevC.9.1258
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1974HA44      Phys.Lett. 51B, 341 (1974)

M.L.Halbert, C.B.Fulmer, S.Raman, M.J.Saltmarsh, A.H.Snell, P.H.Stelson

Elastic Scattering of 16O by 16O

NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=35-88 MeV; measured σ(E, θ).

doi: 10.1016/0370-2693(74)90223-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1531.


1974MC15      Phys.Rev. C10, 1146 (1974)

F.K.McGowan, C.E.Bemis, Jr., W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson

Coulomb Excitation of Vibrational-Like States in the Even-A Actinide Nuclei

NUCLEAR REACTIONS 230,232Th, 236,238U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα'). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm levels deduced B(E2), B(E3). Enriched targets.

doi: 10.1103/PhysRevC.10.1146
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1974RI12      Phys.Rev.Lett. 33, 1346 (1974)

L.L.Riedinger, G.J.Smith, P.H.Stelson, E.Eichler, G.B.Hagemann, D.C.Hensley, N.R.Johnson, R.L.Robinson, R.O.Sayer

Dominance of the i13/2 Neutron in Yb Backbending

NUCLEAR REACTIONS 148Nd(22Ne, 5nγ), E=109 MeV; measured Eγ, γγ-coin. 156Gd(12C, 3nγ), E=58 MeV; measured Eγ, γ(θ). 165Yb deduced levels, J, π, decoupled rotational bands.

doi: 10.1103/PhysRevLett.33.1346
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1973BE40      Phys.Rev. C8, 1934 (1973)

C.E.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle

Interference between Direct Nuclear Reactions and Coulomb Excitation with Alpha Particles on 154Sm, 166Er, and 182W

NUCLEAR REACTIONS 154Sm, 166Er, 182W(α, α), (α, α'), E=11-21 MeV; measured σ(E;Eα'). 154Sm, 166Er levels deduced E2, E4 matrix elements.

doi: 10.1103/PhysRevC.8.1934
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1973BE44      Phys.Rev. C8, 1466 (1973)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, P.H.Stelson, R.L.Robinson

E2 and E4 Transition Moments and Equilibrium Deformations in the Actinide Nuclei

NUCLEAR REACTIONS 230,232Th, 236U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-19 MeV; 238U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα', θ). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm deduced B(E2), B(E4), β.

doi: 10.1103/PhysRevC.8.1466
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1973GO32      Phys.Lett. 46B, 180 (1973)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, J.B.McGrory, S.T.Thornton

Population of High Spin States in 22Na by Means of the 10B(16O, α) Reaction

NUCLEAR REACTIONS 10B(16O, α), E=46 MeV; measured σ(Eα, θ). 22Na deduced levels of high J.

doi: 10.1016/0370-2693(73)90677-1
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1973RA17      Nucl.Phys. A206, 343 (1973)

S.Raman, P.H.Stelson, G.G.Slaughter, J.A.Harvey, T.A.Walkiewicz, G.J.Lutz, L.G.Multhauf, K.G.Tirsell

Gamma Transitions between Low-Lying Levels in 119Sn

RADIOACTIVITY 119In [from 120Sn(γ, p), 119Sn(n, p), 122Sn(n, α) (β) 119In]; measured T1/2, Eγ, Iγ. 119Sn deduced levels.

NUCLEAR REACTIONS 118Sn(n, γ), En=th, 46-5000 eV; measured Eγ, Iγ. 119Sn(α, α'γ), Eα=10 MeV; measured Eγ, Iγ. 119Sn deduced levels. Enriched targets, Ge(Li) detector.

doi: 10.1016/0375-9474(73)90538-1
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1973ST10      Priv.Comm. (June 1973); See Also 73Ri04, 73St09

P.H.Stelson


1973ST14      Phys.Rev. C8, 368 (1973)

P.H.Stelson, S.Raman, J.A.McNabb, R.W.Lide, C.R.Bingham

Search for a Zero-Phonon Gamma-Ray Transition in 108Pd and 134Ba

RADIOACTIVITY 108mAg, 134Cs; measured Iγ. 108Pd, 134Ba deduced upper limit on intensity of zero phonon γ-transition.

doi: 10.1103/PhysRevC.8.368
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1972FO02      Nucl.Instrum.Methods 98, 199 (1972)

J.L.C.Ford, Jr., P.H.Stelson, R.L.Robinson

A Position Sensitive Proportional Detector for a Magnetic Spectrograph

NUCLEAR REACTIONS 246Cm(α, α'), E=17 MeV; measured σ(Eα'). 246Cm deduced B(E2). 238U(α, α'), E=15 MeV; measured σ(Eα'). 238U deduced levels.

doi: 10.1016/0029-554X(72)90098-5
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1972RA14      Nucl.Phys. A184, 138 (1972)

S.Raman, R.L.Auble, W.T.Milner, J.B.Ball, F.K.McGowan, P.H.Stelson, R.L.Robinson

Nuclear Spectroscopy of 50Cr

RADIOACTIVITY 50Mn; measured T1/2, Eγ, Iγ.

NUCLEAR REACTIONS 50Cr(p, p'γ), E=8.4 MeV; measured Eγ, Iγ. 52Cr(p, t), E=31.4 MeV; measured σ(Et, θ). 50Cr(35Cl, 35Cl'γ), E=54 MeV; measured B(E2), Doppler shift attenuation. 50Cr deduced levels, J, π, γ-branching, T1/2.

doi: 10.1016/0375-9474(72)90449-6
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1972RO27      Nucl.Phys. A193, 14 (1972)

R.L.Robinson, F.K.McGowan, W.T.Milner, P.H.Stelson

Coulomb Excitation of 81Br

NUCLEAR REACTIONS 81Br(α, α'γ), E=2.5-8.2 MeV; 81Br(16O, 16O'γ), E=33 MeV; measured σ(E;Eγ, θ(γ), θ(γγ)), Iγ, Doppler broadening. 81Br deduced levels, J, π, B(E2), B(M1), T1/2.

doi: 10.1016/0375-9474(72)90231-X
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1972ST16      Nucl.Phys. A190, 197 (1972)

P.H.Stelson, W.T.Milner, F.K.McGowan, R.L.Robinson, S.Raman

Coulomb Excitation of 117,119Sn

NUCLEAR REACTIONS 117,119Sn(α, α'γ), 117,119Sn(16O, 16O'γ)Eα=10, 10.5, 11 MeV;E(16O)=45 MeV; measured Eγ, Iγ, Iγ(θ), Doppler broadening. 117,119Sn deduced levels, J, π, B(E2), B(M1), T1/2. Enriched targets.

doi: 10.1016/0375-9474(72)90137-6
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1972ST23      Priv.Comm. (August 1972)

P.H.Stelson


1972ST39      Nucl.Instrum.Methods 98, 481 (1972)

P.H.Stelson, J.K.Dickens, S.Raman, R.C.Trammell

Deterioration of Large Ge(Li) Diodes Caused by Fast Neutrons

doi: 10.1016/0029-554X(72)90232-7
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1971FO17      Phys.Rev.Lett. 27, 1232 (1971)

J.L.C.Ford, Jr., P.H.Stelson, C.E.Bemis, Jr., F.K.McGowan, R.L.Robinson, W.T.Milner

Precise Coulomb Excitation B(E2) Values for First 2+ States of the Actinide Nuclei

NUCLEAR REACTIONS 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf(α, α'), E=17, 18 MeV; measured B(E2). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf deduced B(E2). 252Cf deduced level.

doi: 10.1103/PhysRevLett.27.1232
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1971HA17      Nucl.Phys. A172, 139 (1971)

J.H.Hamilton, S.M.Brahmavar, J.B.Gupta, R.W.Lide, P.H.Stelson

Search for Weak Transitions in the Decay of 108mAg

RADIOACTIVITY 108mAg [from 107Ag(n, γ)]; measured Eγ, Iγ; deduced isomeric branching. Ge(Li) detectors. Sources produced 1950'S, 1960'S.

doi: 10.1016/0375-9474(71)90121-7
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1971MC14      Ann.Phys.(N.Y.) 63, 549 (1971)

F.K.McGowan, W.T.Milner, R.L.Robinson, P.H.Stelson

Coulomb Excitation of 197Au and a Core-Excitation Analysis

NUCLEAR REACTIONS 197Au(α, α'γ), E=9.94-14 MeV; 197Au(16O, 16O'γ), E=42-45 MeV; measured σ(E;Eγ, θ(γ)), γγ-coin. 197Au levels deduced B(E2), B(M1), γ-mixing, g. Coulomb excitation;core-excitation analysis.

doi: 10.1016/0003-4916(71)90028-5
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1971MC21      Phys.Rev.Lett. 27, 1741 (1971)

F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson

Equilibrium Quadrupole and Hexadecapole Deformations in 230Th and 238U

NUCLEAR REACTIONS 230Th, 238U(α, α), (α, α'), E=17, 18 MeV; measured σ(Eα'). 230Th, 238U deduced B(EL), equilibrium deformation parameters.

doi: 10.1103/PhysRevLett.27.1741
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1971MI08      Nucl.Phys. A177, 1 (1971)

W.T.Milner, F.K.McGowan, R.L.Robinson, P.H.Stelson, R.O.Sayer

Coulomb Excitation of 182,184,186W, 186,188,190,192Os and 192,194,196,198Pt with Protons, 4He and 16O Ions

NUCLEAR REACTIONS 182,184,186W(p, p'γ), E=5 MeV;182,184,186W(α, α'γ), E=14, 15 MeV; 182,184,186W(16O, 16O'γ), E=45.5 MeV; 188,190,192Os(p, p'γ), E=4.56-5.08 MeV; 186Os(α, α'γ), E=3-5 MeV; 188,190,192Os(α, α'γ), E=15 MeV; 186,188,190,192Os(16O, 16O'γ), E=42, 45.1, 45.5 MeV; 192,194,196,198Pt(p, p'γ), E=4.5 MeV; 192,194,196,198Pt(16O, 16O'γ), E=43.75 MeV; measured Iγ, Eγ, (16O)(γ)-coin, 182,184,186W, 186,188,190,192Os, 192,196,194,198Pt deduced B(E2), B(M1), J. Enriched, natural targets.

doi: 10.1016/0375-9474(71)90161-8
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1971RO09      Nucl.Phys. A166, 141 (1971)

R.L.Robinson, W.T.Milner, F.K.McGowan, P.H.Stelson, M.A.Ludington

E2/M1 Admixture of the 2'→2 Transition in 108Pd

NUCLEAR REACTIONS 108Pd(α, α'γγ), Eα=10.1 MeV; measured γγ(θ). 108Pd transition deduced γ-mixing, B(E2), B(M1). Enriched target.

doi: 10.1016/0375-9474(71)90418-0
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1971ST15      Priv.Comm. (July 1971)

P.H.Stelson


1970BA64      Phys.Rev. C2, 2154 (1970)

W.T.Bass, P.H.Stelson

Levels of 61Cu, 64Cu, 67Ga, and 68Ga Excited by the (p, n) Reaction

NUCLEAR REACTIONS 61,64Ni, 67,68Zn(p, n), E=2.9-6.3 MeV; measured σ(E;En). 61Cu deduced levels. 64Cu, 67,68Ga deduced levels, J, π.

doi: 10.1103/PhysRevC.2.2154
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1970FO01      Nucl.Phys. A142, 525 (1970)

J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, T.Tamura, C.-Y.Wong

Elastic and Inelastic Proton Scattering from 109Ag

NUCLEAR REACTIONS 109Ag(p, p'), E=13 MeV; measured σ(θ). 109Ag deduced levels, deformation parameters. Enriched target.

doi: 10.1016/0375-9474(70)90810-9
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1970RA13      Nucl.Phys. A147, 1 (1970)

M.N.Rao, P.H.Stelson, R.L.Robinson, J.L.C.Ford, Jr.

Elastic and Inelastic Proton Scattering from 124Te

NUCLEAR REACTIONS 124Te(p, p), (p, p'), E = 12 MeV; measured σ(Ep, θ), σ(Ep', θ). 124Te deduced levels, deformation parameters β(L). Enriched target. DWBA, coupled-channel calculations.

doi: 10.1016/0375-9474(70)90504-X
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1970RO14      Nucl.Phys. A150, 225 (1970)

R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner

Coulomb Excitation of 107,109Ag

NUCLEAR REACTIONS 107,109Ag(α, α'γ), E=10.0, 10.7 MeV; 107,109Ag(16O, 16O'γ), E=45.5 MeV; measured σ(Eγ, θ(γ)), γγ-triple correlation, Doppler broadening. 107,109Ag deduced levels, B(E2), B(M1), B(E1), T1/2, J, π, γ-mixing, γ-branching.

doi: 10.1016/0375-9474(70)90946-2
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1970SA09      Phys.Rev. C1, 1525 (1970)

R.O.Sayer, P.H.Stelson, F.K.McGowan, W.T.Milner, R.L.Robinson

Multiple Coulomb Excitation of 152Sm, 166Er, and 172,174,176Yb

NUCLEAR REACTIONS 152Sm, 166Er, 172,174,176Yb(α, α'γ), E=7, 8, 9, 10 MeV; 152Sm, 166Er, 172,174,176Yb(16O, 16O'γ), E=25-52 MeV; measured σ(E;Eα', Eγ), σ(E;E(16O'), Eγ). 152Sm, 166Er, 172,174,176Yb levels deduced B(E2).

doi: 10.1103/PhysRevC.1.1525
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1970ST05      Nucl.Phys. A144, 254 (1970)

P.H.Stelson, R.W.Lide, C.R.Bingham

Decay of the γ-Vibrational Band in 250Cf

RADIOACTIVITY 250Bk[from 254Es source]; measured Eγ, Iγ. 250Cf deduced levels, B(E2) ratios, γ-mixing. Ge(Li) detector.

doi: 10.1016/0375-9474(70)90358-1
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1970ST20      Phys.Rev. C2, 2015 (1970)

P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner

Static Quadrupole Moment of the First 2+ States of the Even Tin Nuclei

NUCLEAR REACTIONS 112,116,118,120,122,124Sn(α, α'γ), E=10 MeV; 112,114,116,118,120,122,124Sn(16O, 16O'γ), E=46 MeV; measured σ(Eα', Eγ), σ(E(16O'), Eγ). 112,116,118,120,122,124Sn levels deduced quadrupole moment, B(E2).

doi: 10.1103/PhysRevC.2.2015
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1970TA01      Phys.Rev. C2, 160 (1970)

S.Tanaka, P.H.Stelson, W.T.Bass, J.Lin

Levels in 53Mn, 58Co, 63Zn, and 70Ga from the (p, n) Reaction

NUCLEAR REACTIONS 53Cr, 58Fe, 63Cu, 70Zn(p, n), E=2.74-6.35 MeV; measured σ(E;En). 53Mn, 58Co, 63Zn, 70Ga deduced levels.

doi: 10.1103/PhysRevC.2.160
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1969MI07      Nucl.Phys. A129, 687 (1969)

W.T.Milner, F.K.McGowan, P.H.Stelson, R.L.Robinson, R.O.Sayer

Coulomb Excitation of the Even-A Cadmium Nuclei

NUCLEAR REACTIONS 106,108,110,112,114,116Cd(p, p'γ), E=2.7, 3.0 MeV; 106,108,110,112,114,116Cd(α, α'γ), E=9-11 MeV; 106,108Cd(16O, 16O'γ), E=42-49 MeV; measured Iγ, Eγ, γγ-coin, γ(θ). 106,108,110,112,114,116Cd deduced levels, B(E2), B(M1), J. Enriched targets.

doi: 10.1016/0375-9474(69)90710-6
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1969RO03      Nucl.Phys. A123, 193 (1969)

R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer

Gamma-Gamma Angular Correlations Following Coulomb Excitation

NUCLEAR REACTIONS 107,109Ag, 110Pd, 117Sn(α, α'γ), E=9.5-10 MeV; 190,192Os(p, p'γ), E=4.5 MeV; measured γγ(θ). 107,109Ag, 110Pd, 117Sn, 190,192Os deduced levels, J, γ-mixing ratio. Enriched target.

doi: 10.1016/0375-9474(69)90899-9
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1969RO05      Nucl.Phys. A124, 553 (1969)

R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer

Coulomb Excitation of 106,108,110Pd

NUCLEAR REACTIONS 106,108,110Pd(α, α'γ), E=9-10 MeV; 106,108,110Pd(16O, 16O'γ), E=42-49 MeV, measured Iγ, Eγ, γγ-coin., γ(θ). 106,108,110Pd deduced levels B(E2), B(M1), T1/2, J, π. Enriched targets.

doi: 10.1016/0375-9474(69)90650-2
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1969RO30      Phys.Rev. 187, 1609 (1969)

R.L.Robinson, J.L.C.Ford, Jr., P.H.Stelson, T.Tamura, C.Y.Wong

Elastic and Inelastic Proton Scattering from 110Pd

NUCLEAR REACTIONS 110Pd(p, p), (p, p'), E=13 MeV; measured σ(Ep', θ). 110Pd deduced levels, J, π, β(L).

doi: 10.1103/PhysRev.187.1609
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1968EI02      Nucl.Phys. A120, 622 (1968)

E.Eichler, P.H.Stelson, J.K.Dickens

A New Measurement of the Half-Life of the 72Ge 0+ State

NUCLEAR REACTIONS 19F, 72Ge(n, n') E=4.75 MeV; measured nX-delay. 19F, 72Ge level deduced T1/2. Natural target.

doi: 10.1016/0375-9474(68)90468-5
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1968MC08      Nucl.Phys. A113, 529 (1968)

F.K.McGowan, R.L.Robinson, P.H.Stelson, W.T.Milner

Coulomb Excitation of States in the Even-Mass Ruthenium Nuclei with 16O and 4He Ions

NUCLEAR REACTIONS 98,100,102,104Ru(16O, 16O'γ), E=42-49 MeV; 98,100,102,104Ru(α, α'γ), E=10 MeV; measured σ(Eγ, θ), γγ-coin; deduced B(E2), B(M1), J. Enriched targets.

doi: 10.1016/0375-9474(68)90161-9
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1968ST05      Nucl.Phys. A111, 331 (1968)

P.H.Stelson

Decay of 65Zn

RADIOACTIVITY 65Zn; measured Iγ, γγ-coin. 65Cu level deduced branching. Ge(Li) detector.

doi: 10.1016/0375-9474(68)90126-7
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1968ST07      Priv.Comm. (1968)

P.H.Stelson

NUCLEAR STRUCTURE 65Cu; measured not abstracted; deduced nuclear properties.


1968ST14      Phys.Rev. 170, 1172 (1968)

P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner, R.O.Sayer

Coulomb Excitation of the Even Tin Nuclei

NUCLEAR STRUCTURE 112Sn, 118Sn, 116Sn, 120Sn, 122Sn, 124Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.170.1172
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1968ST18      Nucl.Phys. A119, 14 (1968)

P.H.Stelson, J.L.C.Ford, Jr., R.L.Robinson, C.Y.Wong, T.Tamura

Elastic and Inelastic Proton Scattering from 112,114Cd

NUCLEAR REACTIONS 112,114Cd(p, p), (p, p'), E=13 MeV; measured σ(Ep, θ), σ(Ep', θ). 112,114Cd deduced levels, deformation parameters β(L). Enriched targets. DWBA, coupled-channel calculations.

doi: 10.1016/0375-9474(68)90802-6
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1967FO08      Phys.Rev. 158, 1194 (1967)

J.L.C.Ford, Jr., C.-Y.Wong, T.Tamura, R.L.Robinson, P.H.Stelson

Elastic and Inelastic Proton Scattering from 107Ag and the Phonon-Core Model

NUCLEAR STRUCTURE 107Ag; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.158.1194
Citations: PlumX Metrics


1967MA18      Priv.Comm. (1967)

A.Marusak, P.H.Stelson

NUCLEAR STRUCTURE 59Cu; measured not abstracted; deduced nuclear properties.


1967RO03      Nucl.Phys. A96, 6 (1967)

R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner

Low-Lying Levels of 79Br

RADIOACTIVITY 79Kr [from 79Br(p, n), 78Kr(n, γ)]; measured Eγ, Iγ, γγ coin. 79Br deduced levels, B(E2), B(M1), T1/2, J, π, log ft. 79Br(α, α'γ), E = 2.5-7 MeV; 79Br(16O, 16O'γ), E = 36 MeV; measured Eγ, Iγ, γγ coin, γ(θ). Enriched target.

doi: 10.1016/0375-9474(67)90690-2
Citations: PlumX Metrics


1967RO14      Nucl.Phys. A104, 401 (1967)

R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner

Coulomb Excitation of 75As

NUCLEAR REACTIONS 75As(α, α'γ), E=3.5-8.1 MeV; 75As(16O, 16O'γ), E=36-38 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 75As deduced levels, B(E2), B(M1), T1/2, J, π.

doi: 10.1016/0375-9474(67)90564-7
Citations: PlumX Metrics


1967ST05      Phys.Rev. 157, 1098 (1967)

P.H.Stelson

Decay of 124Sb to 124Te

NUCLEAR STRUCTURE 124Sb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.157.1098
Citations: PlumX Metrics


1967ST11      Priv.Comm. (1967)

P.H.Stelson

NUCLEAR STRUCTURE 59Co; measured not abstracted; deduced nuclear properties.


1967ST15      Priv.Comm. (1967)

P.H.Stelson

NUCLEAR STRUCTURE 65Zn; measured not abstracted; deduced nuclear properties.


1967ST18      Priv.Comm. (1967)

P.H.Stelson

NUCLEAR STRUCTURE 59Ni; measured not abstracted; deduced nuclear properties.


1967ST19      Priv.Comm. (1967)

P.H.Stelson, J.K.Dickens, F.G.Perey

NUCLEAR STRUCTURE 59Ni; measured not abstracted; deduced nuclear properties.


1966BI15      ORNL-TM-1665, p.3 (1966)

J.A.Biggerstaff, Y.Cassagnou, W.E.Kinney, M.V.Harlow, Jr., J.M.McConnell, F.G.Perey, P.H.Stelson

Neutron Inelastic Scattering Program

NUCLEAR STRUCTURE 59Ni, 59Cu, 59Co, 51V, 28Si, 60Cu, 65Zn, 56Fe, 53Mn, 51Cr, 55Fe, 40Ca, 39K, 12C, 89Y, 27Al, 23Na; measured not abstracted; deduced nuclear properties.


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