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NSR database version of March 2, 2024.

Search: Author = E.Rost

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1994RO09      Phys.Rev. C50, 1729 (1994)


Subthreshold Response Function in the Δ-Resonance Region

NUCLEAR REACTIONS 16O(e, e'X), E not given; calculated transverse response function; deduced kinematics, Δ mass, width dependences.

doi: 10.1103/PhysRevC.50.1729
Citations: PlumX Metrics

1993RO13      Phys.Rev. C47, 2250 (1993)

E.Rost, C.E.Price, J.R.Shepard

Transverse Response Functions in the Δ-Resonance Region

NUCLEAR REACTIONS 12C, 40Ca, 56Fe(e, e'), E not given; calculated transverse response functions. Relativistic Hartree approximation, Δ-resonance.

doi: 10.1103/PhysRevC.47.2250
Citations: PlumX Metrics

1992PR01      Phys.Rev. C45, 1089 (1992)

C.E.Price, E.Rost, J.R.Shepard, J.A.McNeil

Toward a Consistent Random Phase Approximation Based on the Relativistic Hartree Approximation

NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, isoscalar transitions. RPA, relativistic Hartree approximation.

NUCLEAR REACTIONS 16O, 12C, 40Ca(e, e'), E not given; calculated longitudinal form factor. RPA, relativistic Hartree approximation.

doi: 10.1103/PhysRevC.45.1089
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1991KI08      Phys.Rev. C44, 1077 (1991)

J.D.King, D.Frekers, R.Abegg, R.E.Azuma, L.Buchmann, C.Chan, T.E.Drake, R.Helmer, K.P.Jackson, L.Lee, C.A.Miller, E.Rost, R.Sawafta, R.Schubank, S.S.M.Wong, S.Yen, X.Q.Zhu

Excitation of the 10.957 MeV 0-; T = 0 State in 16O by 400 MeV Protons

NUCLEAR REACTIONS 16O(polarized p, p'), E=400 MeV; measured σ(θ), analyzing power vs θ; deduced reaction mechanism.

doi: 10.1103/PhysRevC.44.1077
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1991OD03      Phys.Rev. C44, 2426 (1991)

J.M.O'Donnell, H.T.Fortune, E.Rost

0+ and 2+ Strengths in Pion Double Charge Exchange to Double Giant-Dipole Resonances

NUCLEAR REACTIONS 40Ca(π+, π-), E=165-300 MeV; calculated σ(θ). 40Ca deduced β. Coupled-channels optical model.

doi: 10.1103/PhysRevC.44.2426
Citations: PlumX Metrics

1990PI06      Phys.Rev. C41, 2277 (1990)

J.Piekarewicz, E.Rost, J.R.Shepard

Correlation Observables in (p, p'γ) Reactions

NUCLEAR REACTIONS 12C(polarized p, p'γ), E=400 MeV; calculated σ(θp, θγ), analyzing powers vs θ. Relativistic impulse approximation.

doi: 10.1103/PhysRevC.41.2277
Citations: PlumX Metrics

1989MC05      Phys.Rev. C40, 399 (1989)

J.A.McNeil, R.J.Furnstahl, E.Rost, J.R.Shepard

Finite Nucleus Dirac Mean Field Theory and Random Phase Approximation using Finite B Splines

NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, isoscalar longitudinal form factors. Finite nucleus Dirac mean field theory.

doi: 10.1103/PhysRevC.40.399
Citations: PlumX Metrics

1989RO13      Phys.Rev. C40, 1736 (1989)

E.Rost, J.R.Shepard

Dirac Random-Phase-Approximation Analysis of the Inelastic Scattering of 500 MeV Protons from 40Ca

NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=500 MeV; calculated σ(θ), analyzing power, spin transfer observables vs θ. Dirac RPA.

doi: 10.1103/PhysRevC.40.1736
Citations: PlumX Metrics

1989SH27      Phys.Rev. C40, 2320 (1989)

J.R.Shepard, E.Rost, J.A.McNeil

Nonspectral Dirac Random-Phase Approximation for Finite Nuclei

NUCLEAR REACTIONS 12C, 16O, 48,40Ca(e, e'), E not given; calculated form factors. Nonspectral Dirac RPA.

NUCLEAR STRUCTURE 16O; calculated lowest 1-, T=0 level B(E1). RPA.

doi: 10.1103/PhysRevC.40.2320
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1988HI09      Phys.Rev. C38, 229 (1988)

K.H.Hicks, R.G.Jeppesen, C.C.K.Lin, R.Abegg, K.P.Jackson, O.Hausser, J.Lisantti, C.A.Miller, E.Rost, R.Sawafta, M.C.Vetterli, S.Yen

Inelastic Proton Scattering at 200 to 400 MeV for 24Mg and 28Si in a Microscopic Framework

NUCLEAR REACTIONS 12C, 24Mg, 28Si(polarized p, p'), E=200-400 MeV; measured σ(θ), A(θ) vs E; deduced model validity. Relativistic, nonrelativistic DWIA.

doi: 10.1103/PhysRevC.38.229
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1426.

1988KU27      J.Phys.(London) G14, L253 (1988)

P.D.Kunz, E.Rost

Relativistic Suppression Factors in (p, d) Reaction Calculations

NUCLEAR REACTIONS 40Ca(p, d), E=120 MeV; calculated Darwin, pseudovector suppression factors vs radius. Relativistic approach.

doi: 10.1088/0305-4616/14/3/002
Citations: PlumX Metrics

1988MC03      Phys.Rev.Lett. 61, 814 (1988)

J.P.McDermott, E.Rost, J.R.Shepard, C.Y.Cheung

Relativistic (γ, p) Calculations at Intermediate Energies

NUCLEAR REACTIONS 16O(γ, p), E=196 MeV; 40Ca(γ, p), E=100-300 MeV; calculated σ(θ).

doi: 10.1103/PhysRevLett.61.814
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1988SH07      Phys.Rev. C37, 1130 (1988)

J.R.Shepard, E.Rost, C.-Y.Cheung, J.A.McNeil

Magnetic Response of Closed-Shell ±1 Nuclei in Dirac-Hartree Approximation

NUCLEAR REACTIONS 15N(e, e), E not given; calculated isoscalar M1 form factor. Dirac-Hartree approximation.

NUCLEAR STRUCTURE 15N, 15O; A=15, 17, 39, 41; calculated μ. Dirac-Hartree approximation.

doi: 10.1103/PhysRevC.37.1130
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1987FR05      Phys.Rev. C35, 2236 (1987)

D.Frekers, S.S.M.Wong, R.E.Azuma, T.E.Drake, J.D.King, R.Abegg, K.P.Jackson, C.A.Miller, S.Yen, W.P.Alford, R.L.Helmer, C.Broude, S.Mattsson, E.Rost

Elastic and Inelastic Scattering of 362 MeV polarized Protons from 40Ca

NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=362 MeV; measured σ(θ), analyzing power. Magnetic spectrometer. Model calculations.

doi: 10.1103/PhysRevC.35.2236
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0840.

1987RO02      Phys.Rev. C35, 681 (1987)

E.Rost, J.R.Shepard

Nucleon-Nucleus Inelastic Scattering using a Relativistic Impulse Approximation with Exchange

NUCLEAR REACTIONS 12C(p, p'), (polarized p, p'), E=135, 200, 400 MeV; calculated σ(θ), analyzing powers. Relativistic impulse approximation, exchange.

doi: 10.1103/PhysRevC.35.681
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1986SH01      Phys.Rev. C33, 634 (1986)

J.R.Shepard, E.Rost, J.A.McNeil

Relativistic Plane-Wave Impulse Approximation for Nuclear Inelastic Scattering of Protons and Electrons

NUCLEAR REACTIONS 12C(e, e'), E not given; 12C(p, p'), E=150 MeV; calculated nuclear transition densities, currents. 12C levels deduced structure information. Relativistic plane-wave impulse approximation.

doi: 10.1103/PhysRevC.33.634
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1985SP03      Phys.Rev.Lett. 54, 2207 (1985)

D.A.Sparrow, J.Piekarewicz, E.Rost, J.R.Shepard, J.A.McNeil, T.A.Carey, J.B.McClelland

Relativistic Impulse Approximation, Nuclear Currents, and the Spin-Difference Function

NUCLEAR REACTIONS 12C(p, p'), E=150 MeV; calculated P(θ), analyzing power vs θ difference; deduced nuclear currents role. Relativistic approximation.

doi: 10.1103/PhysRevLett.54.2207
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1984RO02      Phys.Rev. C29, 209 (1984)

E.Rost, J.R.Shepard, E.R.Siciliano, J.A.McNeil

Impulse Approximation Dirac Theory of Inelastic Proton Nucleus Collective Excitations

NUCLEAR REACTIONS 54Fe(polarized p, p), E=800 MeV; calculated σ(θ), analyzing power vs θ. Dirac theory, impulse approximation.

doi: 10.1103/PhysRevC.29.209
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1984SH08      Phys.Rev. C29, 2243 (1984)

J.R.Shepard, E.Rost, E.R.Siciliano, J.A.McNeil

Dirac Single-Particle Wave Functions in Inelastic Electron Scattering

NUCLEAR REACTIONS 12C(e, e), (e, e'), E not given; calculated charge, transverse form factors; deduced transverse isoscalar transition linear inelastic amplitude role. Dirac single particle wave functions.

doi: 10.1103/PhysRevC.29.2243
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1984SH21      Phys.Rev. C30, 1604 (1984)

J.R.Shepard, E.Rost, J.Piekarewicz

Microscopic Relativistic Nucleon-Nucleus Inelastic Scattering

NUCLEAR REACTIONS 12C(p, p'), E not given; calculated natural, unnatural parity level amplitudes. Relativistic treatment.

doi: 10.1103/PhysRevC.30.1604
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1982RO09      Phys.Rev.Lett. 49, 448 (1982)

E.Rost, J.R.Shepard, D.Murdock

Dirac Wave Functions in Nuclear Distorted-Wave Calculations

NUCLEAR REACTIONS 90Zr(p, n), E=80 MeV; calculated σ(θ), analyzing power vs θ. Distorted waves, Dirac, Schrodinger approaches.

doi: 10.1103/PhysRevLett.49.448
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1982SH03      Phys.Rev. C25, 1127 (1982)

J.R.Shepard, E.Rost, P.D.Kunz

Failure of the Distorted-Wave Born Approximation in Analysis of the 24Mg(p(pol), d)23Mg Reaction at T(p) = 94 MeV

NUCLEAR REACTIONS 24Mg(polarized p, d), E=94 MeV; calculated σ(θ), analyzing power vs θ; deduced DWBA inadequacy. DWBA, CCBA, exact finite-range effects, deuteron tensor interaction, breakup, multi-step process, radial cutoff.

doi: 10.1103/PhysRevC.25.1127
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1982SH06      Phys.Rev. C25, 2660 (1982)

J.R.Shepard, E.Rost

Analytic Eikonal Model for Intermediate Energy Stripping and Pickup Reactions

NUCLEAR REACTIONS 16O(d, p), E=400, 660 MeV; 12C(p, d), E=800 MeV; calculated σ(θ). Eikonal model.

doi: 10.1103/PhysRevC.25.2660
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1982SH11      Phys.Rev.Lett. 49, 14 (1982)

J.R.Shepard, E.Rost, D.Murdock

Dirac Phenomenology for Deuteron Elastic Scattering

NUCLEAR REACTIONS 58Ni(d, d), (polarized d, d), E=80 MeV; analyzed σ(θ), vector analyzing power vs θ; deduced effective central potential. Dirac, Schrodinger equation approaches.

doi: 10.1103/PhysRevLett.49.14
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1981WE03      Nucl.Phys. A355, 45 (1981)

R.C.Weiss, R.E.Anderson, J.J.Kraushaar, R.A.Ristinen, E.Rost, S.Shastry

A Study of Particle-Vibration Multiplets in 203Tl using the 205Tl(p, t)203Tl, 208Pb(p, t)206Pb and 206Pb(p, t)204Pb Reactions

NUCLEAR REACTIONS 205Tl, 206,208Pb(p, t), E=26.2 MeV; measured σ(θ, Et). 203Tl deduced levels, L, J, π. 203Tl, 204,206Pb levels deduced L=0, 2 enhancement factors, J, π. DWBA analysis, intermediate coupling wave functions.

doi: 10.1016/0375-9474(81)90131-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0161.

1980BA45      Phys.Lett. B97, 45 (1980)

B.M.Barnett, W.Gyles, R.R.Johnson, K.L.Erdman, J.Johnstone, J.J.Kraushaar, S.Lepp, T.G.Masterson, E.Rost, D.R.Gill, A.W.Thomas, J.Alster, I.Navon, R.H.Landau

Proton Radii Determinations from the Ratio of π+ Elastic Scattering from 11B and 12C

NUCLEAR REACTIONS 12C, 11B(π+, π+), E=38.6, 47.7 MeV; measured σ(θ). 12C, 11B deduced rms charge radii differences.

doi: 10.1016/0370-2693(80)90543-2
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1979DI01      Phys.Rev. C19, 1132 (1979)

N.J.DiGiacomo, R.L.Boudrie, I.Brissaud, J.J.Kraushaar, R.J.Peterson, R.A.Ristinen, E.S.Rost, G.R.Smith

Elastic and Inelastic Diffraction Scattering of 0.8 GeV Protons by 89Y and 90Zr

NUCLEAR REACTIONS 89Y, 90Zr(p, p'), E=0.8 GeV; measured σ(θ). 89Y, 90Zr levels deduced β(L). Optical model, DWBA analysis.

doi: 10.1103/PhysRevC.19.1132
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1979JO08      Phys.Rev.Lett. 43, 844 (1979)

R.R.Johnson, T.Masterson, B.Bassalleck, W.Gyles, T.Marks, K.L.Erdman, A.W.Thomas, D.R.Gill, E.Rost, J.J.Kraushaar, J.Alster, C.Sabev, J.Arvieux, M.Krell

Neutron Radii Determinations from the Ratio of π- Elastic Scattering From 12,13C and 16,18O

NUCLEAR REACTIONS 12,13C(π-, π-), E=29.2-49.5 MeV; 16,18O(π-, π-), E=29.2 MeV; measured σ(θ). 13C, 18O deduced neutron radii relative to 12C, 16O. Optical model analysis.

doi: 10.1103/PhysRevLett.43.844
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1979SH21      Phys.Lett. 89B, 13 (1979)

J.R.Shepard, E.Rost, G.R.Smith

Evidence for Pion Exchange Currents in the Analysis of the 4He(p, d)3He Reaction at Intermediate Energies

NUCLEAR REACTIONS 4He(p, d), E=434, 770 MeV; calculated σ(θ). DWBA, no pion exchange currents.

doi: 10.1016/0370-2693(79)90065-0
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1978AR16      Nucl.Phys. A312, 368 (1978)

J.Arvieux, J.P.Albanese, J.Bolger, E.Boschitz, C.H.Q.Ingram, L.Pflug, J.Jansen, J.Zichy, E.Rost, A.S.Rosenthal

Elastic and Inelastic Scattering of π± by 208Pb

NUCLEAR REACTIONS 208Pb(π+, π+), E=80, 116 MeV; 208Pb(π-, π-), E=116 MeV; measured σ(θ) for ground state at 80, 116 MeV, for first 3- excited state at 116 MeV. Optical potential, collective model analysis.

doi: 10.1016/0375-9474(78)90597-3
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1978RO06      Phys.Rev. C17, 1513 (1978)

E.Rost, J.R.Shepard, D.A.Sparrow

Distorted-Wave Born-Approximation Description of the 4He(p, d)3He Reaction at E = 770 MeV

NUCLEAR REACTIONS 4He(p, d), E=770 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.17.1513
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1977DI03      Phys.Lett. 66B, 421 (1977)

N.J.Digiacomo, A.S.Rosenthal, E.Rost, D.A.Sparrow

Pion-Nucleus Scattering at 50 MeV

NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(π+, X), (π+, π+), E=50 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(77)90575-5
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1977RO25      Phys.Lett. 71B, 237 (1977)

A.S.Rosenthal, E.Rost, D.A.Sparrow, N.J.Digiacomo

Second Order Density Effects in Low Energy Pion Scattering

NUCLEAR REACTIONS 56Fe, 208Pb(π+, π+), E=50 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(77)90202-7
Citations: PlumX Metrics

1976IV03      Phys.Rev. C14, 1733 (1976)

M.S.Iverson, E.Rost

Pion-Gamma Angular Correlations Following Inelastic Scattering

NUCLEAR REACTIONS 12C(π, π'γ), E=30-150 MeV; calculated pion-γ angular correlation.

doi: 10.1103/PhysRevC.14.1733
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1975IV05      Phys.Rev. C12, 1589 (1975)

M.S.Iverson, E.Rost

Pion Elastic Scattering from Aligned Targets

NUCLEAR REACTIONS 165Ho(π, π), E=100-200 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.12.1589
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1975RO29      Phys.Lett. 59B, 413 (1975)

E.Rost, J.R.Shepard

Exact Finite Range DWBA Results for the 12C(p, d)11C Reaction at 700 MeV

NUCLEAR REACTIONS 12C(p, d), E=700 MeV; calculated σ(Ed, θ). DWBA calculation.

doi: 10.1016/0370-2693(75)90332-9
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1974BA58      Phys.Lett. 52B, 57 (1974)

S.D.Baker, R.Bertini, R.Beurtey, F.Brochard, G.Bruge, H.Catz, A.Chaumeaux, G.Cvijanovich, J.M.Durand, J.C.Faivre, J.M.Fontaine, D.Garreta, F.Hibou, D.Legrand, J.C.Lugol, J.Saudinos, J.Thirion, E.Rost

The 12C(p, d)11C Reaction at 700 MeV

NUCLEAR REACTIONS 12C(p, d), E=700 MeV; measured σ(Ed, θ). 11C levels deduced reaction mechanism.

doi: 10.1016/0370-2693(74)90718-7
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1974GE09      Phys.Lett. 52B, 39 (1974)

E.Gerlic, J.Van de Wiele, H.Langevin-Joliot, J.P.Didelez, G.Duhamel, E.Rost

The (τ, α) Reaction at 216 MeV

NUCLEAR REACTIONS 12C, 16O(3He, α), E=216 MeV; measured σ(Eα, θ). 11C, 15O levels deduced reaction mechanism.

doi: 10.1016/0370-2693(74)90712-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0243.

1974KU17      Phys.Lett. 53B, 9 (1974)

P.D.Kunz, E.Rost

On the Analysis of the 12C(d, τ)11B Reaction at 80 MeV

NUCLEAR REACTIONS 12C(d, 3He), E=80 MeV; calculated σ(E(3He), θ). 11B deduced β2.

doi: 10.1016/0370-2693(74)90329-3
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1973BA13      Ann.Phys.(New York) 76, 437 (1973)

H.W.Baer, J.J.Kraushaar, C.E.Moss, N.S.P.King, R.E.L.Green, P.D.Kunz, E.Rost

Study of the (p, t) Reaction on the Even-A Titanium Isotopes

NUCLEAR REACTIONS 46,48,50Ti(p, t), E=19, 23, 27 MeV; measured σ(Et, θ). Deduced L. 44,46,48Ti deduced levels, J, π.

doi: 10.1016/0003-4916(73)90043-2
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1973RO10      Phys.Lett. 43B, 17 (1973)

E.Rost, P.D.Kunz

Analysis of (π+, p) and (p, π+) Reactions

NUCLEAR REACTIONS 12C(π+, p), (p, π+), E=68, 185 MeV; calculated σ(θ). DWBA.

doi: 10.1016/0370-2693(73)90531-5
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1971AB01      Nucl.Phys. A162, 173 (1971)

P.M.Abraham, E.Rost

Rotational Levels of Deformed Doubly Even Nuclei

NUCLEAR STRUCTURE 158Dy, 164Er, 168Yb, 174Hf; calculated intrinsic, rotational energies.

doi: 10.1016/0375-9474(71)90492-1
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1971ED02      Phys.Rev.Lett. 26, 785 (1971)

G.W.Edwards, E.Rost

π-Carbon Inelastic Scattering Near the 33 Resonance

NUCLEAR REACTIONS 12C(π-, π-'), E=120-280 MeV; calculated σ(θ). 12C deduced deformation parameters. DWBA, Kisslinger optical potential.

doi: 10.1103/PhysRevLett.26.785
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1971RO04      Nucl.Phys. A162, 376 (1971)

E.Rost, P.D.Kunz

Finite-Range Corrections in Two-Nucleon Transfer Reactions

NUCLEAR REACTIONS 48Ti(p, t), E=27 MeV; calculated σ(θ). Finite-range DWBA.

doi: 10.1016/0375-9474(71)90992-4
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1971RO12      Phys.Rev. C3, 2491 (1971)

E.Rost, R.Schaeffer

Shapes of Angular Distributions of (3He, t) and (p, n) Transitions to 0+ Antianalog States

NUCLEAR REACTIONS 40Ar(3He, t), E not given; calculated σ(θ), form factors for antianalog transitions.

doi: 10.1103/PhysRevC.3.2491
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1971RO32      Phys.Lett. 37B, 247 (1971)

E.Rost, G.W.Edwards

Pion-Nucleus Charge Exchange Scattering at Intermediate Energies

NUCLEAR REACTIONS 93Nb(π+, π-), E < 300 MeV; calculated σ(E;θ). Kisslinger optical model.

doi: 10.1016/0370-2693(71)90009-8
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1970DE18      Nucl.Phys. A150, 187 (1970)

D.W.Devins, M.E.Rickey, S.Hayakawa, E.Rost

T = 9/2 Analogue State in 63Ni

NUCLEAR REACTIONS 64Ni(p, d), E=27.5 MeV; measured σ(Ed, θ). 63Ni deduced isobaric analog state, S. Enriched target.

doi: 10.1016/0375-9474(70)90465-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0120.

1969HA21      Phys.Letters 29B, 327 (1969)

S.I.Hayakawa, J.J.Kraushaar, P.D.Kunz, E.Rost

Study of the Effective Two-Body Force Using the 54Fe(3He, t) Charge Exchange Reaction

NUCLEAR REACTIONS 54Fe(3He, t), E=37.5 MeV; measured σ(E, θ). Microscopic DWBA analysis.

doi: 10.1016/0370-2693(69)90374-8
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1969HA47      Nucl.Phys. A139, 465 (1969)

S.I.Hayakawa, W.L.Fadner, J.J.Kraushaar, E.Rost

Study of the 90Zr(3He, t) Reaction

NUCLEAR REACTIONS 90Zr(3He, t), E=37.7 MeV; measured σ(Et, θ). 90Nb deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(69)91123-3
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1969KU02      Phys.Rev. 177, 1737(1969)

P.D.Kunz, E.Rost, R.R.Johnson

Particle Transfer Reactions on Deformed Nuclei

NUCLEAR REACTIONS 24Mg(p, p), (p, d), E=27.3 MeV; measured σ(Ed, θ). 23Mg deduced levels. Enriched target, optical-model analysis.

doi: 10.1103/PhysRev.177.1737
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1969KU09      Phys.Rev. 185, 1528 (1969)

P.D.Kunz, E.Rost, R.R.Johnson, G.D.Jones, S.I.Hayakawa

Analyses of Quasielastic and Quasi-Inelastic (3He, t) Scattering from the Ni Isotopes

NUCLEAR REACTIONS 58,60,62,64Ni(3He, t), E = 37.5 MeV; measured σ(θ). Coupled-channel analysis, macroscopic, microscopic interaction models.

doi: 10.1103/PhysRev.185.1528
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1969RO18      Phys.Letters 30B, 231 (1969)

E.Rost, P.D.Kunz

Role of Tensor Force in Charge Exchange Reactions

NUCLEAR REACTIONS 54Fe(3He, t), E = 37.7 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(69)90424-9
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1966RO01      Phys.Letters 21, 87 (1966)


Proton Core Excitation in the Ground State in 18O

NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)91353-9
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1965GL01      Bull.Am.Phys.Soc. 10, No.1, 121, KD3 (1965)

C.Glashausser, M.Kondo, M.E.Rickey, E.Rost

Evidence for f7/2 Admixture in the Ground State of 40Ca from Neutron Pickup Reactions

NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.

1965GL02      Phys.Letters 14, 113 (1965)

C.Glashausser, M.Kondo, M.E.Rickey, E.Rost

Configuration Mixing in the Ground State of Ca40

NUCLEAR STRUCTURE 39Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90443-9
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1965SH06      Phys.Rev. 139, B1272 (1965)

R.Sherr, B.F.Bayman, E.Rost, M.E.Rickey, C.G.Hoot

Excitation of Isobaric Analog States in Medium-Weight Nuclei by the (p, d) Reaction at 28 MeV

NUCLEAR STRUCTURE 61Ni, 55Fe, 52Cr, 51Cr, 53Fe, 57Fe, 57Ni, 59Ni, 49Cr, 49Ti, 47Ti; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B1272
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1964FU07      Phys.Rev. 134, B117 (1964)

H.O.Funsten, N.R.Roberson, E.Rost

Inelastic Proton Scattering from Nuclei with 28 Neutrons

NUCLEAR STRUCTURE 54Fe, 52Cr, 50Ti, 51V; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.134.117
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1326.

1964LE10      Phys.Rev. 134, B752 (1964)

J.C.Legg, E.Rost

(p, d) Reactions on Nuclei from V to Ni

NUCLEAR STRUCTURE 54Mn, 51Cr, 55Fe, 56Fe, 53Fe, 50V, 59Ni, 57Ni, 58Co, 57Fe; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.134.B752
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1964SH12      Phys.Rev.Letters 12, 420 (1964)

R.Sherr, E.Rost, M.E.Rickey

J Dependence of the Angular Distributions from (p, d) Reaction at 28 Mev

NUCLEAR STRUCTURE 59Ni, 57Fe, 57Ni, 55Fe, 61Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.12.420
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1962BA67      Phys.Rev. 128, 2693 (1962)

R.H.Bassel, G.R.Satchler, R.M.Drisko, E.Rost

Analysis of the Inelastic Scattering of Alpha Particles. I

doi: 10.1103/PhysRev.128.2693
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Note: The following list of authors and aliases matches the search parameter E.Rost: , E.S.ROST