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NSR database version of April 11, 2024.

Search: Author = P.Kunz

Found 67 matches.

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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. 234,237,236,239,240U, 231,232,233,234,235,236,237,238,239,240,241Np, 235,236,237,238,239,240,241Pu; calculated production yields by inelastic reactions and through decays of precursors: 234,236,237Pa, 231,233,235Pu, 237,239,240U, 235Am, 235,236,238,239,240,241Np 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 198,202,203,206,207,208Hg; 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 197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214Pb, 201,202,203,204,205,206,207,208,209,210Hg. 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. 183,184,185,202,203,206,207,208Hg; 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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2601.


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 225,226,227,228,229Ac; measured hyperfine spectra, and isotope shifts by probing a 2D3/2 to 4P5/2 atomic transition using in-source resonance ionization spectroscopy at the ISAC facility in TRIUMF, where the actinium isotopes were produced in irradiating UCx 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, T1/2, 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 UCx 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. 183,185,187,189Hg, 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 T1/2, 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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Data from this article have been entered in the XUNDL database. For more information, click here.


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 182,183,184,185,186,187,188,189,190Pb [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 182,183,184,185,186,187,188,189,190Pb; 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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0052.


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0371.


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, 122,124,126,128,130Te(d, 6Li), 112,114,116,118,120,122,124Sn(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 112,116,118,120,124Sn(3He, n), E=25.4 MeV; measured σ(En, θ). 114,118,120,122,126Te 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 112,116,120,124Sn(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 Be9* (2.43-MeV State)

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

doi: 10.1103/PhysRev.118.228
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