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NSR database version of April 27, 2024.

Search: Author = P.Kunz

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2023AU02      Phys.Rev. C 107, 064604 (2023)

M.Au, M.Athanasakis-Kaklamanakis, L.Nies, R.Heinke, K.Chrysalidis, U.Koster, P.Kunz, B.Marsh, M.Mougeot, L.Schweikhard, S.Stegemann, Y.Vila Gracia, Ch.E.Dullmann, S.Rothe

Production of neptunium and plutonium nuclides from uranium carbide using 1.4-GeV protons

NUCLEAR REACTIONS U(p, X)²³⁵Np/²³⁶Np/²³⁷Np/²³⁸Np/²³⁹Np/²⁴⁰Np/²⁴¹Np/²³⁵Pu/²³⁶Pu/²³⁷Pu/²³⁸Pu/²³⁹Pu/²⁴⁰Pu/²⁴¹Pu, E=1.4 GeV; measured reaction products using resonance ionization laser ion source (RILIS), general purpose separator (GPS), and ISOLTRAP multireflection time-of-flight mass spectrometer (MR-ToF MS) at CERN-ISOLDE facility. ^{234,237,236,239,240}U, ^{231,232,233,234,235,236,237,238,239,240,241}Np, ^{235,236,237,238,239,240,241}Pu; calculated production yields by inelastic reactions and through decays of precursors: ^234,236,237Pa, ^231,233,235Pu, ^237,239,240U, ²³⁵Am, ^{235,236,238,239,240,241}Np using GEANT4 QGSP_INCLXX+ABLA code. Comparison with predictions of GEANT4 and FLUKA simulations; discussed limit of accelerator-based isotope production at high-energy proton accelerator facilities for nuclides in the actinide region.

ATOMIC PHYSICS ^236,237,239Np, ^236,239,240Pu; measured isotope shifts for the 395.6-nm ground-state transition in Np isotopes, and for the 413.4-nm ground-state transition in Pu isotopes by two-step ionization schemes using intra-cavity doubled Ti:Sa lasers to resonantly ionize Np and Pu isotopes.

doi: 10.1103/PhysRevC.107.064604
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2021DA16      Phys.Rev. C 104, 054322 (2021)

T.Day Goodacre, A.V.Afanasjev, A.E.Barzakh, L.Nies, B.A.Marsh, S.Sels, U.C.Perera, P.Ring, F.Wienholtz, A.N.Andreyev, P.Van Duppen, N.A.Althubiti, B.Andel, D.Atanasov, R.S.Augusto, J.Billowes, K.Blaum, T.E.Cocolios, J.G.Cubiss, G.J.Farooq-Smith, D.V.Fedorov, V.N.Fedosseev, K.T.Flanagan, L.P.Gaffney, L.Ghys, A.Gottberg, M.Huyse, S.Kreim, P.Kunz, D.Lunney, K.M.Lynch, V.Manea, Y.Martinez Palenzuela, T.M.Medonca, P.L.Molkanov, M.Mougeot, J.P.Ramos, M.Rosenbusch, R.E.Rossel, S.Rothe, L.Schweikhard, M.D.Seliverstov, P.Spagnoletti, C.Van Beveren, M.Veinhard, E.Verstraelen, A.Welker, K.Wendt, R.N.Wolf, A.Zadvornaya, K.Zuber

Charge radii, moments, and masses of mercury isotopes across the N=126 shell closure

NUCLEAR MOMENTS ^{198,202,203,206,207,208}Hg; measured hyperfine structure spectra using Versatile Arc Discharge and Laser Ion Source (VADLIS) in CERN-ISOLDE Resonance Ionization Laser Ion Source (RILIS) mode; deduced isotope shifts (δν) and charge radii (δ<r²) with respect to ¹⁹⁸Hg, hyperfine factors a and b, static magnetic dipole (μ) and electric quadrupole (Q) moments for the ground states of ²⁰³Hg and ²⁰⁷Hg, Comparison of g factors with Schmidt values for ²⁰⁷Hg, ²⁰⁹Pb, ²¹⁰Bi and ²¹¹Po, and charge radii, and odd-even staggering (OES) of the mean square charge radii with relativistic Hartree-Bogoliubov (RHB) calculations using DD-ME2, DD-MEδ, DD-PC1 and NL3* covariant energy-density functionals for ^{197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214}Pb, ^{201,202,203,204,205,206,207,208,209,210}Hg. Source of Hg isotopes were produced in Pb(p, X), E=1.4 GeV reaction, and using VADLIS+RILIS ion source, followed by separation of fragments using ISOLDE General Purpose Separator. ^{183,184,185,202,203,206,207,208}Hg; measured ionization and release efficiency as a function of the half-life of mercury isotopes from a molten lead target, and compared with ABRABLA, FLUKA, and GEANT4 simulations.

ATOMIC MASSES ^206,207,208Hg, ²⁰⁸Pb; measured time-of-flight ion-cyclotron resonances, with reference to ²⁰⁸Pb using the RILIS+VADIS ion source and ISOLTRAP MR-ToF mass spectrometer (MS) at CERN-ISOLDE; deduced mass excesses for ^206,207,208Hg, and compared with AME2020 values.

doi: 10.1103/PhysRevC.104.054322
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2020RO18      Phys.Rev. C 102, 044613 (2020)

A.K.H.Robertson, P.Kunz, C.Hoehr, P.Schaffer

Nuclide production cross sections from irradiation of thorium by 438 MeV protons and a comparison to fluka and geant4 simulations

NUCLEAR REACTIONS ²³²Th(p, X)⁸³Rb/⁸⁸Y/⁹⁵Nb/⁹⁵Zr/⁹⁹Mo/¹⁰³Ru/¹⁰⁵Rh/¹⁰⁶Ru/^110mAg/¹¹¹In/¹¹¹Ag/^114mIn/¹¹⁵Cd/^120mSb/¹²¹Te/^121mTe/¹²²Sb/¹²⁴Sb/¹²⁵Sb/¹²⁵Sn/¹²⁶Sb/¹²⁷Sb/¹³¹Ba/¹³²Te/¹³⁴Cs/¹³⁶Cs/¹³⁹Ce/¹⁴⁰Ba/¹⁴¹Ce/¹⁴⁴Ce/²⁰¹Tl/²⁰³Pb/²⁰⁵Bi/²⁰⁶Po/²⁰⁶Bi/²⁰⁷Bi/²²³Ra/²²⁴Ra/²²⁵Ac/²²⁵Ra/²²⁶Ac/²²⁷Ac/²²⁷Th/²²⁸Ra/²²⁸Th/²³⁰Pa/²³³Pa, E=438 MeV from TRIUMF cyclotron; measured off-line Eγ, Iγ; deduced total radioactivity and production σ for 38 out of 47 radioactive isotopes measured and produced in spallation and high-energy fission reactions. Comparison to simulated cross sections calculated using three Monte Carlo computer codes: FLUKA, GEANT4 with Liege intranuclear cascade model, GEANT4 with the binary cascade model, and ABLA evaporation code. Relevance to the production of ²²⁵Ac isotope, a radionuclide of interest in nuclear medicine for the treatment of cancer.

doi: 10.1103/PhysRevC.102.044613
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2019PO06      Phys.Rev. C 100, 054327 (2019)

J.L.Pore, C.Andreoiu, J.K.Smith, A.D.MacLean, A.Chester, J.D.Holt, G.C.Ball, P.C.Bender, V.Bildstein, R.Braid, A.Diaz Varela, R.Dunlop, L.J.Evitts, A.B.Garnsworthy, P.E.Garrett, G.Hackman, S.V.Ilyushkin, B.Jigmeddorj, K.Kuhn, P.Kunz, A.T.Laffoley, K.G.Leach, D.Miller, W.J.Mills, W.Moore, M.Moukaddam, L.N.Morrison, B.Olaizola, E.E.Peters, A.J.Radich, E.T.Rand, F.Sarazin, D.Southall, C.E.Svensson, S.J.Williams, S.W.Yates

Detailed spectroscopy of ⁴⁶Ca: A study of the β^- decay of ⁴⁶K

RADIOACTIVITY ⁴⁶K(β^-)[from U(p, X), E=500 MeV]; measured Eγ, Iγ, γγ-coin, γγ(θ), ce, β particles using GRIFFIN array of 15 HPGe detectors for γ detection, PACES array of five Si(Li) detectors for conversion electrons, and SCEPTAR array of 10 plastic scintillators for β-particle tagging, half-life of ⁴⁶K decay at TRIUMF-ISAC facility. ⁴⁶Ca; deduced levels, J, π, β feedings, logft, γ-branching ratios, multipole mixing ratios. Comparison of level structure with theoretical predictions from microscopic valence space Hamiltonians derived from NN+3N forces.

doi: 10.1103/PhysRevC.100.054327
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2019VE07      Phys.Rev. C 100, 044321 (2019)

E.Verstraelen, A.Teigelhofer, W.Ryssens, F.Ames, A.Barzakh, M.Bender, R.Ferrer, S.Goriely, P.-H.Heenen, M.Huyse, P.Kunz, J.Lassen, V.Manea, S.Raeder, P.Van Duppen

Search for octupole-deformed actinium isotopes using resonance ionization spectroscopy

NUCLEAR MOMENTS ^{225,226,227,228,229}Ac; measured hyperfine spectra, and isotope shifts by probing a ²D_3/2 to ⁴P_5/2 atomic transition using in-source resonance ionization spectroscopy at the ISAC facility in TRIUMF, where the actinium isotopes were produced in irradiating UC_x with 480-MeV proton beam, and ionized by TRIUMF Resonant Ionization Laser Ion Source (TRILIS); deduced mean-square charge radii, hyperfine parameters, magnetic dipole moments, configurations; calculated β₂₀ and β₃₀ deformation parameters using SLy5s1, BSk31, and DD-MEB2 interactions. Comparison with previous experimental measurements, and with self-consistent calculations using energy density functionals SLy5s1, BSk31, and DD-MEB1. Z=82-89, N=120-150; systematics of experimental mean-square charge radii, and odd-even staggering parameter, and compared with theoretical calculations.

doi: 10.1103/PhysRevC.100.044321
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2018RA11      Phys.Rev.Lett. 120, 232503 (2018)

S.Raeder, D.Ackermann, H.Backe, R.Beerwerth, J.C.Berengut, M.Block, A.Borschevsky, B.Cheal, P.Chhetri, Ch.E.Dullmann, V.A.Dzuba, E.Eliav, J.Even, R.Ferrer, V.V.Flambaum, S.Fritzsche, F.Giacoppo, S.Gotz, F.P.Hessberger, M.Huyse, U.Kaldor, O.Kaleja, J.Khuyagbaatar, P.Kunz, M.Laatiaoui, F.Lautenschlager, W.Lauth, A.K.Mistry, E.Minaya Ramirez, W.Nazarewicz, S.G.Porsev, M.S.Safronova, U.I.Safronova, B.Schuetrumpf, P.Van Duppen, T.Walther, C.Wraith, A.Yakushev

Probing Sizes and Shapes of Nobelium Isotopes by Laser Spectroscopy

NUCLEAR MOMENTS ^252,253,254No; measured excitation spectra, hyperfine structure components; deduced nuclear magnetic and quadrupole moments, charge radii. Comparison with the state-of-the-art nuclear density functional calculations.

doi: 10.1103/PhysRevLett.120.232503
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2016LA25      Nature(London) 535, 495 (2016)

M.Laatiaoui, W.Lauth, H.Backe, Mi.Block, D.Ackermann, B.Cheal, P.Chhetri, C.E.Dullmann, P.van Duppen, J.Even, R.Ferrer, F.Giacoppo, S.Gotz, F.P.Hessberger, M.Huyse, O.Kaleja, J.Khuyagbaatar, P.Kunz, F.Lautenschlager, A.K.Mistry, S.Raeder, E.Minaya Ramirez, T.Walther, C.Wraith, A.Yakushev

Atom-at-a-time laser resonance ionization spectroscopy of nobelium

NUCLEAR REACTIONS ^206,208Pb(⁴⁸Ca, 2n), E=217 MeV; measured reaction products; deduced σ, ground-state transition, an upper limit for the ionization potential of nobelium.

doi: 10.1038/nature19345
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2014KU30      Rev.Sci.Instrum. 85, 053305 (2014)

P.Kunz, C.Andreoiu, P.Bricault, M.Dombsky, J.Lassen, A.Teigelhoofer, H.Heggen, F.Wong

Nuclear and in-source laser spectroscopy with the ISAC yield station

RADIOACTIVITY ⁴⁶K(β^-), ²¹⁸At(α); measured decay products, Eγ, Iγ, Eα, Iα; deduced γ-ray energies and relative intensities, T_1/2, laser frequencies. Comparison with available data.

doi: 10.1063/1.4878718
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2013SA43      Eur.Phys.J. A 49, 109 (2013)

J.Sauvage, B.Roussiere, J.Genevey, S.Franchoo, A.N.Andreyev, N.Barre, A.Ben Braham, C.Bourgeois, J.-F.Clavelin, H.De Witte, D.V.Fedorov, V.N.Fedoseyev, L.M.Fraile, X.Grave, G.Huber, M.Huyse, P.Kilcher, U.Koster, P.Kunz, S.R.Lesher, B.A.Marsh, I.Mukha, J.Oms, M.G.Porquet, M.Seliverstov, I.Stefanescu, K.Van de Vel, P.Van Duppen, YU.M.Volkov, A.Wojtasiewicz

Decay of ¹⁸⁵Tl, ^185m+gHg, ^189m+gPb and energy location of the 13/2⁺ isomeric states in ¹⁸⁵Hg, ¹⁸⁹Pb, ¹⁹³Po and ¹⁹⁷Rn

RADIOACTIVITY ¹⁸⁵Hg(β⁺), (EC), (IT);¹⁸⁵Tl, ¹⁸⁹Pb(β⁺), (EC)[from bombarding thick UC_x target by 1.4 GeV protons]; measured Eγ, Iγ(t), X-rays, γγ-coin, (time)γ-coin, Xγ-coin using Ge(HP) detectors with COMET-NARVAL system, α-decay of the decay products, Eα, Iα, αγ-coin. ^{183,185,187,189}Hg, ^187,189Pb, ^191,193,195Po, ^195,197,199Rn deduced partial level scheme, J, π, γ transitions, μ. ¹⁸⁵Hg, ¹⁸⁹Pb, ¹⁹³Po, ¹⁹⁷Rn deduced 13/2⁺ isomeric states.

doi: 10.1140/epja/i2013-13109-5
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2013VI01      Phys.Rev. C 87, 044603 (2013)

A.M.Vinodkumar, W.Loveland, R.Yanez, M.Leonard, L.Yao, P.Bricault, M.Dombsky, P.Kunz, J.Lassen, A.C.Morton, D.Ottewell, D.Preddy, M.Trinczek

Interaction of ¹¹Li with ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹¹Li, X)²¹²At/²¹³At/²¹⁴At/²¹⁵At/²¹⁶At, E=39.9, 36.5, 32.7, 28.6 MeV; measured Eα, Iα from evaporation residues, production σ(E), complete and incomplete fusion σ(E), breakup σ(E) at TRIUMF-ISAC2 facility. ²⁰⁹Bi(⁷Li, X)²¹²Rn/²¹³Rn, E=34.90 MeV; measured complete fusion σ, and compared to earlier experimental results. Comparison with theoretical predictions, and with results from experimental results of other reaction.

doi: 10.1103/PhysRevC.87.044603
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2020.

2009SA09      Eur.Phys.J. A 39, 33 (2009)

J.Sauvage, J.Genevey, B.Roussiere, S.Franchoo, A.N.Andreyev, N.Barre, J.-F.Clavelin, H.De Witte, D.V.Fedorov, V.N.Fedoseyev, L.M.Fraile, X.Grave, G.Huber, M.Huyse, H.B.Jeppesen, U.Koster, P.Kunz, S.R.Lesher, B.A.Marsh, I.Mukha, J.Oms, M.Seliverstov, I.Stefanescu, K.Van de Vel, J.Van de Walle, P.Van Duppen, Yu.M.Volkov

Nuclear structure of ¹⁸⁹Tl states studied via β⁺ /EC decay and laser spectroscopy of ^189m+gPb

RADIOACTIVITY ¹⁸⁹Pb(β⁺), (EC) [from ²³⁸U(p, X), E=1.4 GeV]; measured prompt and delayed Eγ, Iγ, γγ-coin; deduced T_1/2, log ft; calculated nuclear deformation. ¹⁸⁹Tl deduced levels, J, π. In-source laser spectroscopy.

doi: 10.1140/epja/i2008-10693-3
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2009SE13      Eur.Phys.J. A 41, 315 (2009)

M.D.Seliverstov, A.N.Andreyev, N.Barre, A.E.Barzakh, S.Dean, H.De Witte, D.V.Fedorov, V.N.Fedoseyev, L.M.Fraile, S.Franchoo, J.Genevey, G.Huber, M.Huyse, U.Koster, P.Kunz, S.R.Lesher, B.A.Marsh, I.Mukha, B.Roussiere, J.Sauvage, I.Stefanescu, K.Van de Vel, P.Van Duppen, Yu.M.Volkov

Charge radii and magnetic moments of odd- A ^183-189Pb isotopes

NUCLEAR MOMENTS ^{182,183,184,185,186,187,188,189,190}Pb [from ²³⁸U(p, X), E=1, 4 GeV online mass separator using the in-source resonance ionization spectroscopy technique]; measured hfs spectra; deduced μ, hyperfine coupling constants, charge radii. Comparison with other data.

doi: 10.1140/epja/i2009-10817-3
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2007BA58      Eur.Phys.J. D 45, 99 (2007)

H.Backe, P.Kunz, W.Lauth, A.Dretzke, R.Horn, T.Kolb, M.Laatiaoui, M.Sewtz, D.Ackermann, M.Block, F.Herfurth, F.P.Hessberger, S.Hofmann, R.Mann

Towards optical spectroscopy of the element nobelium (Z = 102) in a buffer gas cell

doi: 10.1140/epjd/e2007-00198-1
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2006EL07      Eur.Phys.J. A 28, Supplement 1, 197 (2006)

M.El-Ghazaly, H.Backe, W.Lauth, G.Kube, P.Kunz, A.Sharafutdinov, T.Weber

X-ray phase contrast imaging at MAMI

doi: 10.1140/epja/i2006-09-021-6
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2006LA21      Eur.Phys.J. A 28, Supplement 1, 185 (2006)

W.Lauth, H.Backe, O.Kettig, P.Kunz, A.Sharafutdinov, T.Weber

Coherent X-rays at MAMI

doi: 10.1140/epja/i2006-09-019-0
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2006SE18      Hyperfine Interactions 171, 225 (2006)

M.Seliverstov, A.Andreyev, N.Barre, H.De Witte, D.Fedorov, V.Fedoseyev, S.Franchoo, J.Genevey, G.Huber, M.Huyse, U.Koster, P.Kunz, S.Lesher, B.Marsh, B.Roussiere, J.Sauvage, P.Van Duppen, Yu.Volkov

Study of the neutron deficient ^182-190Pb isotopes by simultaneous atomic- and nuclear-spectroscopy

NUCLEAR MOMENTS ^{182,183,184,185,186,187,188,189,190}Pb; measured hfs, isotope shifts; deduced charge radii. Resonance ionization spectroscopy.

doi: 10.1007/s10751-006-9486-z
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2005BB14      Hyperfine Interactions 162, 3 (2005)

H.Backe, A.Dretzke, St.Fritzsche, R.G.Haire, P.Kunz, W.Lauth, M.Sewtz, N.Trautmann

Laser Spectroscopic Investigation of the Element Fermium (Z = 100)

NUCLEAR MOMENTS ²⁵⁵Fm; measured hfs. Resonance ionization spectroscopy.

doi: 10.1007/s10751-005-9209-x
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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
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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
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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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1988AS02      Nucl.Phys. B296, 493 (1988)

D.Aston, N.Awaji, T.Bienz, F.Bird, J.D'Amore, W.Dunwoodie, R.Endorf, K.Fujii, H.Hayashii, S.Iwata, W.B.Johnson, R.Kajikawa, P.Kunz, D.W.G.S.Leith, L.Levinson, T.Matsui, B.T.Meadows, A.Miyamoto, M.Nussbaum, H.Ozaki, C.O.Pak, B.N.Ratcliff, D.Schultz, S.Shapiro, T.Shimomura, P.K.Sinervo, A.Sugiyama, S.Suzuki, G.Tarnopolsky, T.Tauchi, N.Toge, K.Ukai, A.Waite, S.Williams

A Study of K^-π⁺ Scattering in the Reaction K^-p → K^-π⁺n at 11 GeV/c

NUCLEAR REACTIONS ¹H(K^-, K^-π⁺), E at 11 GeV/c; measured (nπ⁺) invariant mass distribution.

doi: 10.1016/0550-3213(88)90028-4
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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
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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
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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
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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
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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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Note: The following list of authors and aliases matches the search parameter P.Kunz: , P.D.KUNZ