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NSR database version of May 24, 2024.

Search: Author = K.A.Erb

Found 32 matches.

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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
Citations: PlumX Metrics


1987OL01      Nucl.Instrum.Methods Phys.Res. A254, 1 (1987)

D.K.Olsen, K.A.Erb, C.M.Jones, W.T.Milner, D.C.Weisser, N.F.Ziegler

Calibration of the HHIRF Tandem Accelerator Energy-Analyzing Magnet

NUCLEAR REACTIONS 12C(16O, α), E=27.3 MeV; measured σ(Eα). Energy analyzing magnet.

doi: 10.1016/0168-9002(87)90474-8
Citations: PlumX Metrics


1986ER10      Phys.Lett. 181B, 52 (1986)

K.A.Erb, I.Y.Lee, W.T.Milner

Evidence for Peak Structure in e+ + Th Interactions

NUCLEAR REACTIONS 181Ta, 232Th(e+, e+e-), E ≤ 1.9 MeV; measured e+, e- spectra; deduced structure. Magnetic spectrometer, coincidence method.

doi: 10.1016/0370-2693(86)91253-0
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1984FU10      Nucl.Phys. A427, 545 (1984)

C.B.Fulmer, G.R.Satchler, K.A.Erb, D.C.Hensley, R.L.Auble, J.R.Ball, F.E.Bertrand, E.E.Gross

Elastic and Inelastic Scattering of 158 MeV 9Be Ions

NUCLEAR REACTIONS 12C, 16O, 26Mg, 27Al, 40Ca, 60Ni, 197Au(9Be, 9Be); 12C, 26Mg, 60Ni(9Be, 9Be'), E=158 MeV; measured σ(θ); deduced optical potential parameters. Distorted wave calculations.

doi: 10.1016/0375-9474(84)90230-6
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1983GR10      Nucl.Phys. A401, 362 (1983)

E.E.Gross, J.R.Beene, K.A.Erb, M.P.Fewell, D.Shapira, M.J.Rhoades-Brown, G.R.Satchler, C.E.Thorn

Elastic and Inelastic Scattering of 120 MeV 18O from 208Pb and the Spin Alignment of the 2+ State of 18O

NUCLEAR REACTIONS 208Pb(18O, 18O), (18O, 18O'), E=120 MeV; measured σ(E(18O), θ), Doppler broadened line shapes. 18O deduced substate population, excited state hexadecapole moment. Enriched target. Coupled-channels analysis.

doi: 10.1016/0375-9474(83)90533-X
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1983KO15      Phys.Rev. C28, 168 (1983)

S.K.Korotky, K.A.Erb, R.L.Phillips, S.J.Willett, D.A.Bromley

Evidence for Nuclear Molecular Orbital Effects in the 13C + 13C → 12C + 14C Transfer Reaction

NUCLEAR REACTIONS 13C(13C, 12C), (13C, 14C), E=16-50 MeV; measured σ(θ, E); deduced evidence for effective Q-value reduction in surface region, collision delay time increase. DWBA analysis, two-pole model. 13C(13C, 13C), E=14.5-71 MeV; measured σ(θ, E); deduced geometrical effect oscillations. Optical model analysis, single pole model.

doi: 10.1103/PhysRevC.28.168
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1983SA20      Phys.Lett. 128B, 147 (1983)

G.R.Satchler, C.B.Fulmer, R.L.Auble, J.B.Ball, F.E.Bertrand, K.A.Erb, E.E.Gross, D.C.Hensley

Refractive Effects in 9Be Scattering and Nuclear Rainbow Ghosts

NUCLEAR REACTIONS 12C, 16O(9Be, 9Be), E=158 MeV; measured σ(θ); deduced optical model parameters, nuclear rainbow, refractive effects. Optical model.

doi: 10.1016/0370-2693(83)90378-7
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1983WI11      Phys.Rev. C28, 1986 (1983)

S.J.Willett, S.K.Korotky, R.L.Phillips, D.A.Bromley, K.A.Erb

Spin Alignment and Phase Angles in 12C + 12C Inelastic Scattering

NUCLEAR REACTIONS, ICPND 12C(12C, 12C'), E=30-65 MeV; measured 12Cγ(θ); deduced σ(E). 12C level deduced magnetic substate alignments, phase angles. Band crossing, diffraction, DWBA, barrier top models.

doi: 10.1103/PhysRevC.28.1986
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1982SH16      Phys.Lett. 114B, 111 (1982)

D.Shapira, R.Novotny, Y.D.Chan, K.A.Erb, J.L.C.Ford, Jr., J.C.Peng, J.D.Moses

Deep-Inelastic Back-Angle Yields and Orbiting in 28Si + 12C

NUCLEAR REACTIONS, ICPND 12C(28Si, 12C), (28Si, 14N), (28Si, 16O), E=99-133 MeV; measured reaction σ, σ(E(12C)), σ(E(14N)), σ(E(16O)); deduced orbiting effect.

doi: 10.1016/0370-2693(82)90126-5
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1981ER02      Phys.Rev. C23, 2781 (1981)

K.A.Erb, D.A.Bromley

Rotational and Vibrational Excitations in Nuclear Molecular Spectra

NUCLEAR REACTIONS 12C(12C, 12C), (12C, X), E(cm) < 13 MeV; analyzed all data. Molecular symmetry model.

doi: 10.1103/PhysRevC.23.2781
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1980ER06      Phys.Rev. C22, 507 (1980)

K.A.Erb, R.R.Betts, S.K.Korotky, M.M.Hindi, P.P.Tung, M.W.Sachs, S.J.Willett, D.A.Bromley

Resonant and Average Behavior of the 12C+12C Total Reaction Cross Section: 5.6≤E(cm)≤10.0 MeV

NUCLEAR REACTIONS 12C(12C, γ), E=11.8-20 MeV; measured σ(E); deduced total reaction σ. 24Mg deduced resonances, J, π, Γ(12C), Γ. Optical model analysis, incoming-wave boundary condition model.

doi: 10.1103/PhysRevC.22.507
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1979ER11      Phys.Rev. C20, 2031 (1979)

K.A.Erb, W.D.Callender, R.K.Sheline

Two-Particle Two-Hole Configurations in 208Bi and the 210Bi-m(p, t)208Bi Reaction

NUCLEAR REACTIONS 210mBi(p, t), E=18.4 MeV; measured σ(θ). 208Bi deduced levels, J, π. Radioactive, enriched target. DWBA analysis, shell model wave functions.

doi: 10.1103/PhysRevC.20.2031
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1979KO19      Phys.Rev. C20, 1014 (1979)

S.K.Korotky, K.A.Erb, S.J.Willett, D.A.Bromley

12C + 12C Coulomb Barrier Resonances: Direct Determination of Resonance Parameters from Elastic Scattering Measurements

NUCLEAR REACTIONS 12C(12C, 12C), E=13.0-14.1 MeV; measured σ(E;θ); deduced phase shift parameters. 24Mg resonances deduced J, Γ(12C). Breit-Wigner analysis.

doi: 10.1103/PhysRevC.20.1014
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1979PH01      Phys.Rev.Lett. 42, 566 (1979)

R.L.Phillips, K.A.Erb, D.A.Bromley, J.Weneser

Origin of Gross Structure in 12C + 12C and 16O + 16O Inelastic Scattering

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=10-40 MeV; 16O(16O, 16O'), E(cm)=15-45 MeV; calculated σ(E). Nonresonant diffraction model.

doi: 10.1103/PhysRevLett.42.566
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1978SH22      Phys.Rev. C18, 2574 (1978)

G.B.Sherwood, K.A.Erb, D.L.Hanson, R.J.Ascuitto, D.A.Bromley, J.J.Kolata

Interference Effects in the Reaction 48Ti(16O, 15N)49V

NUCLEAR REACTIONS 48Ti(16O, 15N), E=50 MeV; measured σ(θ). 48Ti, 49V levels deduced B(E2), (2j+1)C2S. CCBA analysis of inelastic multistep contributions. Particle-core model. Enriched targets.

doi: 10.1103/PhysRevC.18.2574
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1978TU06      Phys.Rev. C18, 1663 (1978)

P.P.Tung, K.A.Erb, M.W.Sachs, G.B.Sherwood, R.J.Ascuitto, D.A.Bromley

Sequential Amplitudes in Heavy-Ion Induced Two-Proton Transfer Reactions

NUCLEAR REACTIONS 90Zr, 88Sr(16O, 16O), (16O, 14C), E=80 MeV; 88Sr, 90Zr(12C, 12C), (12C, 10Be), E=60 MeV; measured σ(θ). Finite range DWBA, CCBA analyses. Enriched targets.

doi: 10.1103/PhysRevC.18.1663
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1977HA28      Phys.Rev. C16, 902 (1977)

D.L.Hanson, K.A.Erb, J.S.Vaagen, R.J.Ascuitto, D.A.Bromley, J.J.Kolata

Quadrupole Transfer Strength Studied Through Heavy-Ion Induced Two-Neutron Transfer between the Shape Transitional Nuclei 190,192Os

NUCLEAR REACTIONS 192Os(12C, 12C), (12C, 14C), E=70 MeV; measured σ(θ); deduced effect of shape transitions on quadrupole transfer strength. CCBA analysis.

doi: 10.1103/PhysRevC.16.902
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1976ER03      Phys.Rev.Lett. 37, 670 (1976)

K.A.Erb, R.R.Betts, D.L.Hanson, M.W.Sachs, R.L.White, P.P.Tung, D.A.Bromley

New Resonances in the Low-Energy 12C-12C Spectrum

NUCLEAR REACTIONS 12C(12C, α), E(cm)=6.5-11 MeV; measured σ(E, Eα, θ). 20Ne deduced levels. 24Mg deduced resonances, Γα.

doi: 10.1103/PhysRevLett.37.670
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1976HA46      Nucl.Phys. A269, 520 (1976)

D.L.Hanson, R.J.Ascuitto, J.S.Vaagen, K.A.Erb, D.A.Bromley, J.J.Kolata, D.J.Pisano

Quadrupole Transfer Strength for Deformed Rare-Earth Nuclei as Studied With Heavy-Ion Induced Two-Nucleon Transfer Reactions

NUCLEAR REACTIONS 154Sm(12C, 14C), E=65 MeV; 182W(12C, 14C), E=70 MeV; measured σ(E(14C), θ); deduced σ(θ) dependence on quadrupole transfer strength in presence of multistep processes. Enriched targets.

doi: 10.1016/0375-9474(76)90697-7
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1975AS01      Phys.Lett. 55B, 289 (1975)

R.J.Ascuitto, J.S.Vaagen, K.A.Erb, D.L.Hanson, D.A.Bromley, J.J.Kolata

Inelastic Nuclear-Coulomb Interference and Direct-Two-Step Interference in Heavy-Ion Induced Two-Nucleon Transfer Reactions on Rare-Earth Nuclei

NUCLEAR REACTIONS 186W(12C, 10Be), E=70 MeV; measured σ(E(10Be), θ).

doi: 10.1016/0370-2693(75)90602-4
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1974ER03      Phys.Rev.Lett. 33, 1102 (1974)

K.A.Erb, D.L.Hanson, R.J.Ascuitto, B.Sorensen, J.S.Vaagen, J.J.Kolata

Observation of Multistep Inelastic Processes in Heavy-Ion-Induced Two-Neutron Transfer Reactions on Rare-Earth Nuclei

NUCLEAR REACTIONS 186W(12C, 14C), E=70 MeV; measured σ(E(14C), θ). 184W levels deduced form factors.

doi: 10.1103/PhysRevLett.33.1102
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1974HA11      Phys.Rev. C9, 929 (1974)

D.L.Hanson, R.G.Stokstad, K.A.Erb, C.Olmer, D.A.Bromley

Compound Nature of the Reaction 12C(14N, 6Li)20Ne

NUCLEAR REACTIONS 12C(14N, 6Li), E(cm)=24, 36, 55 MeV; calculated σ(E(6Li), θ). 12C(14N, 2p), (14N, α), (14N, 7Be), E=12-60 MeV; calculated σ.

doi: 10.1103/PhysRevC.9.929
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1974HA25      Phys.Rev. C9, 1760 (1974)

D.L.Hanson, R.G.Stokstad, K.A.Erb, C.Olmer, M.W.Sachs, D.A.Bromley

Systematics of 'Quasimolecular' Resonances: A Search for Sub-Coulomb Resonant Structure in the Reactions 14N + 14N and 9Be + 12C

NUCLEAR REACTIONS 9Be(12C, α), (12C, p), E(cm)=2.4-6.34 MeV; measured σ(E, Eα, Ep); 14N(14N, α), (14N, p), (14N, d), E(cm)=7-10 MeV; measured σ(E, Eα, Ep, Ed); deduced no resonances.

doi: 10.1103/PhysRevC.9.1760
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1974OL06      Phys.Rev. C10, 1722 (1974)

C.Olmer, R.G.Stokstad, D.L.Hanson, K.A.Erb, M.W.Sachs, D.A.Bromley

Light Particle and Gamma-Ray Production in 12C + 14N Interactions

NUCLEAR REACTIONS 12C(14N, d), (14N, p), (14N, α), E=20, 25 MeV; measured σ(Ed, θ), σ(Ep, θ), σ(Eα, θ); 14N(12C, γ), E=14-33 MeV; measured σ(E, Eγ). 24,25Mg deduced levels, J, π.

doi: 10.1103/PhysRevC.10.1722
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1973ER05      Phys.Rev. C7, 2500 (1973)

K.A.Erb, T.S.Bhatia

Weak-Coupling Structure in 207Bi Studied with the 209Bi(p, t)207Bi and 208Pb(p, t)206Pb Reactions

NUCLEAR REACTIONS 209Bi, 208Pb(p, t), Ep=17.8 MeV; measured σ(Et, θ). 207Bi, 206Pb deduced levels, L. 207Bi deduced particle-core coupling.

doi: 10.1103/PhysRevC.7.2500
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0278.


1973ER08      Phys.Rev. C8, 347 (1973)

K.A.Erb, W.S.Gray

Studies of 205Bi and 207Bi by Proton-Transfer Reactions

NUCLEAR REACTIONS 204,206Pb(3He, d), (α, t), E=45 MeV; measured σ(Ed, θ), σ(Et). 205,207Bi deduced levels, S, L.

doi: 10.1103/PhysRevC.8.347
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1973MA01      Phys.Rev. C7, 651 (1973)

J.V.Maher, K.A.Erb, R.W.Miller

(16O, 15N) Reaction on 2s-1d- and 1f-2p-Shell Nuclei

NUCLEAR REACTIONS 24Mg, 27Al, 28Si, 45Sc, 46,48Ti(16O, 15N), E=42, 48, 53 MeV; measured σ(θ). 28Si, 47,49V, 46Ti levels deduced S.

doi: 10.1103/PhysRevC.7.651
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1972ER04      Phys.Rev.Lett. 29, 1010 (1972)

K.A.Erb, J.E.Holden, I.Y.Lee, J.X.Saladin, T.K.Saylor

Quadrupole and Hexadecapole Deformations in Rare-Earth Nuclei

NUCLEAR REACTIONS 158,160Gd, 162,164Dy, 166,168,170Er(α, α), (α, α'), E=11-13 MeV; measured σ ratios. 158,160Gd, 162,164Dy , 166,168,170Er deduced B(E2), B(E4), β(L).

doi: 10.1103/PhysRevLett.29.1010
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1972MA36      Phys.Rev.Lett. 29, 291 (1972)

J.V.Maher, K.A.Erb, G.H.Wedberg, J.L.Ricci, R.W.Miller

(O16, C12) Studies in the 2s-1d Shell

NUCLEAR REACTIONS 24,26Mg, 27Al, 28Si(16O, 12C), E=42 MeV; measured σ(θ).

doi: 10.1103/PhysRevLett.29.291
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1972SA42      Phys.Lett. 42B, 51 (1972)

T.K.Saylor, J.X.Saladin, I.Y.Lee, K.A.Erb

Electric Hexadecapole Transition Moments in 152,154Sm

NUCLEAR REACTIONS 152,154Sm(α, α'), E=10.5-12 MeV; measured Coulomb excitation probabilities. 152,154Sm deduced B(E2), E4 reduced matrix elements, β(L).

doi: 10.1016/0370-2693(72)90713-7
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1971ER12      Priv.Comm. (1971)

K.A.Erb, W.S.Gray


1969ER05      Priv.Comm. (1971)

K.A.Erb, W.S.Gray


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