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NSR database version of May 8, 2024.

Search: Author = P.D.Kunz

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1997YA02      Phys.Rev. C55, 1890 (1997)

J.Yan, F.E.Cecil, J.A.McNeil, M.A.Hofstee, P.D.Kunz

Deuteron-Induced Reactions on ⁹Be, ¹⁰B, and ¹¹B at Low Energies

NUCLEAR REACTIONS, ICPND ⁹Be(d, p), (d, α), E(cm)=57-139 keV; ¹⁰B(d, p), (d, α), E(cm)=67-141 keV; ¹¹B(d, p), (d, α), E(cm)=76-144 MeV; ⁹Be(d, t), E(cm)=57-139 MeV; measured energy spectra, σ(θ); deduced σ, astrophysical S-factor vs E.

doi: 10.1103/PhysRevC.55.1890
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0452.

1994AL34      Yad.Fiz. 57, No 9, 1678 (1994); Phys.Atomic Nuclei 57, 1608 (1994)

M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz

A Quark Model of (Lambda-bar)(Lambda) Production in (p-bar)p Interactions

NUCLEAR REACTIONS ¹H(p-bar, X), E=threshold-1695 MeV/c; analyzed σ, σ(θ), polarization observables data following (lambda-bar)(lambda) production. Quark model.

1994AL51      Nuovo Cim. 107A, 2483 (1994)

M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz

A Quark Model of (Lambda-bar)Lambda Production in (p-bar)p Interactions

NUCLEAR REACTIONS ¹H(p-bar, X), E=threshold-1.92 GeV/c; calculated σ(θ) for (lambda-bar)(lambda) production. DWBA.

doi: 10.1007/BF02734020
Citations: PlumX Metrics

1994EN04      Nucl.Phys. A578, 93 (1994)

R.Ent, B.L.Berman, H.P.Blok, J.F.J.van den Brand, W.J.Briscoe, M.N.Harakeh, E.Jans, P.D.Kunz, L.Lapikas

The (e, e'd) Reaction on ⁴He, ⁶Li, and ¹²C

NUCLEAR REACTIONS ⁴He, ⁶Li, ¹²C(e, e'd), E(cm) ≈ 30-7- MeV; measured reaction σ vs momentum transfer, σ(θ(e'), E(e'), θ(d)). ¹⁰B levels deduced spectroscopic factors.

doi: 10.1016/0375-9474(94)90971-7
Citations: PlumX Metrics

1994WA06      Phys.Rev. C49, 1534 (1994)

R.E.Warner, J.M.Fetter, R.A.Swartz, A.Okihana, T.Konishi, T.Yoshimura, P.D.Kunz, M.Fujiwara, K.Fukunaga, S.Kakigi, T.Hayashi, J.Kasagi, N.Koori

⁴He(⁴He, ³He)⁵He(g.s.) Reaction at 118 MeV, and Its Distorted Wave Born Approximation Interpretation

NUCLEAR REACTIONS ⁴He(α, ³He), E=118 MeV; measured σ(θ); deduced model parameters. DWBA analysis.

doi: 10.1103/PhysRevC.49.1534
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1591.

1993AL16      Nucl.Phys. A560, 365 (1993)

M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz

A Quark Model of Antilambda-Lambda Production in (p-bar)p Interactions

NUCLEAR REACTIONS ¹H(p-bar, X), E at 1436-1695 MeV/c; calculated (lambda)(lambda-bar) production σ(θ), asymmetry; analyzed σ(θ), polarization, spin correlation coefficients data; deduced model parameters. Quark model, DWBA approach.

doi: 10.1016/0375-9474(93)90102-4
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1992CE02      Nucl.Phys. A539, 75 (1992)

F.E.Cecil, D.Ferg, H.Liu, J.C.Scorby, J.A.McNeil, P.D.Kunz

Radiative Capture of Protons by Light Nuclei at Low Energies

NUCLEAR REACTIONS, ICPND ^6,7Li, ⁹Be, ¹¹B(p, γ), E=40-180 keV; measured capture Eγ, Iγ, γ(θ); deduced astrophysical S-factor. ^7,8Be, ¹⁰B, ¹²C levels deduced γ-ray to charged particle branching ratio. Thick targets, hyperpure Ge detectors.

doi: 10.1016/0375-9474(92)90236-D
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1290.

1990OA01      Phys.Rev. C41, 1081 (1990)

D.S.Oakley, P.D.Kunz, C.L.Morris

Coulomb-Nuclear Interference in Pion Inelastic Scattering

NUCLEAR REACTIONS ²⁰⁸Pb(π⁺, π⁺'), (π^-, π^-'), E=120-250 MeV; analyzed σ(θ); deduced Coulomb-nuclear interference role. ²⁰⁸Pb levels deduced neutron, proton matrix element ratio.

doi: 10.1103/PhysRevC.41.1081
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1989AB01      Phys.Rev. C39, 65 (1989)

R.Abegg, D.A.Hutcheon, C.A.Miller, L.Antonuk, J.M.Cameron, G.Gaillard, J.M.Greben, P.Kitching, R.P.Liljestrand, W.J.McDonald, W.C.Olsen, G.M.Stinson, J.Tinsley, P.D.Kunz

Cross Section and Analyzing Power Measurements for the (p, d) Reaction on ¹⁶O and ⁴⁰Ca at 200 MeV

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca(polarized p, d), E=200 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. ¹⁵O, ³⁹Ca levels deduced spectroscopic factors. DWBA, CCBA analyses.

doi: 10.1103/PhysRevC.39.65
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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
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1985CE12      Nucl.Phys. A441, 477 (1985)

F.E.Cecil, R.J.Peterson, P.D.Kunz

Comparison of ⁶Li(d, n₁)⁷Be and ⁶Li(d, p₁)⁷Li Mirror Reactions at Low Energies

NUCLEAR REACTIONS, ICPND ⁶Li(d, n), (d, p), E=50-160 keV; measured thick target γ-ray yields. ²H deduced electrical polarization effects.

doi: 10.1016/0375-9474(85)90157-5
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1985HI03      Phys.Rev. C31, 1323 (1985)

K.H.Hicks, R.G.Jeppesen, J.J.Kraushaar, P.D.Kunz, R.J.Peterson, R.S.Raymond, R.A.Ristinen, J.L.Ullmann, F.D.Becchetti, J.N.Bradbury, M.Paciotti

Fission of Heavy Nuclei Induced by Energetic Pions

NUCLEAR REACTIONS ²³⁸U, ²⁰⁹Bi, ¹⁹⁷Au(π⁺, F), (π^-, F), E=60-100 MeV; measured fission fragment spectra, mass distribution, σ(fragment θ), (fragment)(fragment)(θ); deduced fission mechanism, σ vs fissility parameter.

doi: 10.1103/PhysRevC.31.1323
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1985KR13      Phys.Rev. C32, 1083 (1985)

J.J.Kraushaar, P.D.Kunz, J.H.Mitchell, J.M.Cameron, D.A.Hutcheon, R.P.Liljestrand, W.J.McDonald, C.A.Miller, W.C.Olsen, J.R.Tinsley, C.E.Stronach

Energy Dependence of the ⁷Li(p, d)⁶Li Reaction

NUCLEAR REACTIONS ⁷Li(p, d), E=200, 400 MeV; measured σ(Ed), σ(θ); deduced optical model parameters. ⁶Li levels deduced spectroscopic factor ratio. DWBA analysis, other data input.

doi: 10.1103/PhysRevC.32.1083
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1984AL05      Phys.Lett. 137B, 334 (1984)

P.W.F.Alons, J.J.Kraushaar, P.D.Kunz

The DWBA Description of the ⁹⁰Zr(p, d)⁸⁹Zr Reaction at Energies from 20 MeV to 185 MeV

NUCLEAR REACTIONS ⁹⁰Zr(p, d), E=20-185 MeV; analyzed σ(θ). ⁸⁹Zr levels deduced spectroscopic factors. Exact finite-range DWBA analysis.

doi: 10.1016/0370-2693(84)91727-1
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1983HA22      Phys.Lett. 129B, 5 (1983)

J.J.Hamill, P.D.Kunz

The Absolute Normalization of Three-Nucleon Transfer Reactions

NUCLEAR REACTIONS ⁴⁰Ca(α, p), E=35.6 MeV; ⁴⁰Ca(⁶Li, t), E=34 MeV; analyzed σ(θ); deduced optical model parameters, absolute normalization reaction dependence. Exact-range, microscopic DWBA analysis.

doi: 10.1016/0370-2693(83)90716-5
Citations: PlumX Metrics

1982KU02      Nucl.Phys. A376, 401 (1982)

P.D.Kunz, T.Kammuri, H.Shimaoka

Microscopic Form Factor for DWBA Analysis of Light-Ion Induced Three-Nucleon Transfer Reactions

NUCLEAR REACTIONS ¹¹⁸Sn(p, α), (polarized p, α), E=20.4, 22 MeV; analyzed σ(θ), analyzing power vs θ. Microscopic form factors, modified zero-range DWBA.

doi: 10.1016/0375-9474(82)90120-8
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1982KU04      Phys.Lett. 112B, 5 (1982)

P.D.Kunz, J.S.Vaagen, J.M.Bang, B.S.Nilsson

Comments on Unhappiness Factors in Simultaneous Transfer DWBA Description of (t, p) and (p, t) Reactions

NUCLEAR REACTIONS ¹⁸O(p, t), E=20 MeV; ⁴⁰Ca(t, p), E=10.1 MeV; ⁴²Ca(p, t), E=39.8 MeV; ⁴⁸Ca(t, p), E=12.08 MeV; calculated σ(θ). Finite-range, one-step DWBA, simultaneous transfer.

doi: 10.1016/0370-2693(82)90893-0
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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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1981KU11      Nucl.Phys. A367, 13 (1981)

P.D.Kunz, G.N.Hassold, J.J.Kraushaar, P.A.Smith

The Energy Dependence of the ⁵⁴Fe(p, t) Reaction

NUCLEAR REACTIONS ⁵⁴Fe(p, t), E=25.2 MeV; measured σ(E(t), θ) absolute. DWBA analysis, zero-range and exact finite-range, energy dependence of enhancement factors. Enriched target.

doi: 10.1016/0375-9474(81)90275-X
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1980KA03      Phys.Lett. 90B, 197 (1980)

T.Kammuri, H.Shimaoka, P.D.Kunz, S.Kato, K.Okada, M.Kondo, K.Hosono, T.Saito, N.Matsuoka, S.Nagamachi, T.Noro, K.Ogino, Y.Kadota

DWBA Form Factor for Three-Particle Transfer Reaction

NUCLEAR REACTIONS ¹³C(polarized p, α), E=65 MeV; analyzed σ(θ), A(θ). DWBA, three-particle transfer form factor, modified Bayman-Kallis model.

doi: 10.1016/0370-2693(80)90722-4
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1980VI03      Nucl.Phys. A340, 183 (1980)

A.Vitturi, L.Ferreira, P.D.Kunz, H.M.Sofia, P.F.Bortignon, R.A.Broglia

Analysis of (⁶Li, d) and (d, ⁶Li) Reactions in the Nickel and Tin Regions

NUCLEAR REACTIONS ⁵⁸Ni, ⁵⁶Fe(⁶Li, d), ¹²²Te(d, ⁶Li), E=34 MeV; calculated σ(θ). DWBA, macroscopic, microscopic form factors.

doi: 10.1016/0375-9474(80)90330-9
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1979KU08      Phys.Rev.Lett. 43, 341 (1979)

P.D.Kunz, A.Saha, H.T.Fortune

Method of Finite-Range Distorted-Wave Born Approximation for Pickup to Unbound Ejectiles

NUCLEAR REACTIONS ¹²C(α, αp), E=65 MeV; calculated σ. Finite range DWBA for pickup to unbound ejectiles.

doi: 10.1103/PhysRevLett.43.341
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1978BR32      Phys.Lett. 79B, 351 (1978)

R.A.Broglia, L.Ferreira, P.D.Kunz, H.Sofia, A.Vitturi

The Alpha-Transfer Reactions and the Pairing Vibrational Model

NUCLEAR REACTIONS ⁵⁶Fe(⁶Li, d), ⁶⁴Zn, ^{122,124,126,128,130}Te(d, ⁶Li), ^{112,114,116,118,120,122,124}Sn(d, ⁶Li); calculated σ(θ) for L=0, α-transfer in terms of pairing vibrational model.

doi: 10.1016/0370-2693(78)90380-5
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1978FI06      Nucl.Phys. A304, 520 (1978)

H.W.Fielding, R.E.Anderson, P.D.Kunz, D.A.Lind, C.D.Zafiratos, W.F.Alford

A Study of the (³He, n) Reaction on Isotopes of Tin

NUCLEAR REACTIONS ^{112,116,118,120,124}Sn(³He, n), E=25.4 MeV; measured σ(En, θ). ^{114,118,120,122,126}Te deduced levels, J, π, L. DWBA analysis, model comparison. Enriched targets, neutron time of flight.

doi: 10.1016/0375-9474(78)90248-8
Citations: PlumX Metrics

1977BL07      Phys.Lett. 69B, 261 (1977)

H.P.Blok, P.D.Kunz

On the Influence of Recoil Effects in the Microscopic Description of Inelastic Scattering

NUCLEAR REACTIONS ¹⁵N(p, p'), E=24.5 MeV; calculated influence of recoil effects on σ. Microscopic description.

doi: 10.1016/0370-2693(77)90539-1
Citations: PlumX Metrics

1977CH28      Phys.Lett. 72B, 7 (1977)

L.A.Charlton, P.D.Kunz

Is (³He, t) Primarily a (³He, α)(α, t) Reaction (Question)

NUCLEAR REACTIONS ⁴⁸Ca(³He, t), E=23 MeV; calculated σ(θ). Two-step process.

doi: 10.1016/0370-2693(77)90049-1
Citations: PlumX Metrics

1976KU02      Phys.Lett. 61B, 1 (1976)

P.D.Kunz, L.A.Charlton

Finite-Range Effects in Multi-Step (p-d, d, n) Reactions

NUCLEAR REACTIONS ⁵⁸Ni(p, n); calculated two-step σ(p, d), σ(d, n).

doi: 10.1016/0370-2693(76)90544-X
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1976SC21      Phys.Lett. 63B, 129 (1976)

M.J.Schneider, J.D.Burch, P.D.Kunz

Competition of Two-Step Processes in the Reactions ^60,62Ni(p, t) Leading to Unnatural Parity States

NUCLEAR REACTIONS ^60,62Ni(p, t), E=26.8 MeV; measured σ(Et, θ); deduced reaction mechanism. DWBA analysis.

doi: 10.1016/0370-2693(76)90631-6
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1975SH06      Phys.Lett. 56B, 135 (1975)

J.R.Shepard, P.D.Kunz, J.J.Kraushaar

The Effect of Pickup-Stripping Contributions on the Selection of a Unique ³He Optical Potential

NUCLEAR REACTIONS ⁵⁸Ni(³He, ³He), (³He, α), (α, ³He), E=83.5 MeV; calculated σ(θ); deduced optical potential.

doi: 10.1016/0370-2693(75)90285-3
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1974FI09      Phys. Rev.Lett. 33, 226 (1974)

H.W.Fielding, L.D.Rickertsen, P.D.Kunz, D.A.Lind, C.D.Zafiratos

Study of the Reaction ⁵⁶Fe(p, n)⁵⁶Co to the Antianalog State

NUCLEAR REACTIONS ⁵⁶Fe(p, n), E=22.8 MeV; measured σ(En, θ); deduced reaction mechanism. ⁵⁶Co deduced levels.

doi: 10.1103/PhysRevLett.33.226
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1974KU04      Phys.Rev. C9, 1659 (1974)

P.D.Kunz, L.D.Rickertsen, G.W.Hoffmann

Macroscopic Analysis of (p, n) Reactions

NUCLEAR REACTIONS ²⁰⁸Pb(p, n), E=20-40 MeV; calculated σ(E); E=26 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.9.1659
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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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1973RI15      Phys.Lett. 47B, 11 (1973)

L.D.Rickertsen, P.D.Kunz

Microscopic Calculations for (p, n) Reactions to Isobaric Analogue States

NUCLEAR REACTIONS ⁴⁰Ar, ⁴⁸Ca, ⁵⁴Fe, ⁵⁸Ni, ⁶⁴Zn, ^90,96Zr(p, n), E=22, 22.8, 30, 40 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(73)90556-X
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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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1972BR09      Phys.Lett. 38B, 383 (1972)

R.A.Broglia, P.D.Kunz, B.Nilsson

Second Order Pairing Phase Transition in the Sn-Isotopes: Competition between Pairing and Shell Effects

NUCLEAR REACTIONS ^{112,116,120,124}Sn(p, t); ¹¹²Sn(t, p); analyzed L=0 transitions; calculated σ(θ). Sn isotopes deduced incomplete pairing phase transition.

doi: 10.1016/0370-2693(72)90162-1
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1972CA30      J.Phys.(London) A5, 1529 (1972)

M.E.Cage, P.D.Kunz, R.R.Johnson, D.A.Lind

A Study of the ¹¹³In(³He, d)¹¹⁴Sn Reaction at 37.7 MeV

NUCLEAR REACTIONS ¹¹³In(³He, d), (³He, ³He), E=37.7 MeV; measured σ(θ); deduced optical model parameters. ¹¹⁴Sn deduced levels, J, π, L(p), p-H strengths.

doi: 10.1088/0305-4470/5/10/019
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1972DU07      Phys.Lett. 38B, 306 (1972)

H.H.Duhm, N.Ueta, W.Heinecke, H.Hafner, H.Homeyer, P.D.Kunz

A Study of the ²⁶Mg(⁶Li, ⁶He)²⁶Al Charge Exchange Reactions

NUCLEAR REACTIONS ²⁶Mg(⁶Li, ⁶Li), (⁶Li, ⁶He), E=36 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1016/0370-2693(72)90252-3
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1971BA93      Phys.Lett. 37B, 128 (1971)

J.Bang, P.D.Kunz

Nuclear Excitation of Giant Dipole and Quadrupole Resonances

NUCLEAR REACTIONS ²⁰⁸Pb(p, p), (p, p'), E=18, 27 MeV; calculated σ(θ) for giant dipole, quadrupole resonances. DWBA, macroscopic form factor.

doi: 10.1016/0370-2693(71)90032-3
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1971CA05      Nucl.Phys. A162, 657 (1971)

M.E.Cage, R.R.Johnson, P.D.Kunz, D.A.Lind

The ³⁹K(³He, ³He)³⁹K and ³⁹K(³He, D)⁴⁰Ca Reactions at 29.3 MeV

NUCLEAR REACTIONS ³⁹K(³He, ³He), ³⁹K(³He, d), E=29.3 MeV; measured σ(θ), σ(Ed, θ). ⁴⁰Ca deduced levels, L, π, S, β₂. Natural targets.

doi: 10.1016/0375-9474(71)90263-6
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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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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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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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1969RA28      Nucl.Phys. A139, 24 (1969)

C.A.Rappleyea, P.D.Kunz

Coulomb Energies in Mass 18 and Mass 42 Nuclei

NUCLEAR STRUCTURE A=18, A=42; calculated Coulomb energies, second energy differences.

doi: 10.1016/0375-9474(69)90256-5
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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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1966KU01      Nucl.Phys. 77, 425 (1966)

P.D.Kunz

A Theoretical Study of the Beta Decay of ⁴⁰Sc

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

doi: 10.1016/0029-5582(66)90185-4
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1965RI06      Phys.Letters 17, 296 (1965)

M.E.Rickey, P.D.Kunz, J.J.Kraushaar, W.G.Anderson

The ⁴⁰Sc-⁴⁰Ca Mass Difference and the ⁴⁰Sc Ground State Spin

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

doi: 10.1016/0031-9163(65)90539-1
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1960HE04      Phys.Rev. 118, 248 (1960)

E.M.Henley, P.D.Kunz

Decay of Be^9* (2.43-MeV State)

NUCLEAR STRUCTURE ⁹Be; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.118.228
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