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NSR database version of April 26, 2024.

Search: Author = K.A.Erb

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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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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
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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