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NSR database version of May 24, 2024.

Search: Author = R.J.Nickles

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2020GU18      Phys.Rev. C 102, 034316 (2020)

A.C.Gula, E.A.McCutchan, C.J.Lister, J.P.Greene, S.Zhu, P.A.Ellison, R.J.Nickles, M.P.Carpenter, S.V.Smith, A.A.Sonzogni

State-of-the-art γ-ray assay of 86Y for medical imaging

RADIOACTIVITY 86Y(β+), (EC)[from 86Sr(p, n), E=16 MeV at the University of Wisconsin Medical Physics cyclotron, followed by chemical separation of activity]; measured Eγ, Iγ, γγ-coin, γγ(θ) using the Gammasphere array at ANL. 86Sr; deduced levels, J, π, multipolarities, mixing ratios, I(β++ϵ), logft values, maximum and average positron energies; estimated radiation dose for potential imaging partner to the therapeutic 90Y isotope. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.102.034316
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Data from this article have been entered in the XUNDL database. For more information, click here.


2018AB02      Phys.Rev. C 97, 034312 (2018)

E.P.Abel, H.K.Clause, J.Fonslet, R.J.Nickles, G.W.Severin

Half-lives of 132La and 135La

RADIOACTIVITY 132,133,135La(β+), (EC)[from Ba(p, X), E=16.5 MeV using GE-PET trace cyclotron at University of Wisconsin followed by chemistry]; measured Eγ, Iγ, β radiation, half-lives using gamma-spectrometry and high-precision ionization-chamber. Comparison with previous measurements, and evaluated data. Relevance to medical applications.

RADIOACTIVITY 64Cu(β-), (β+), (EC); measured decay products; deduced T1/2 of 64Cu decay using an ionization chamber.

doi: 10.1103/PhysRevC.97.034312
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Data from this article have been entered in the XUNDL database. For more information, click here.


2017GR12      Phys.Rev. C 96, 014613 (2017)

S.A.Graves, P.A.Ellison, H.F.Valdovinos, T.E.Barnhart, R.J.Nickles, J.W.Engle

Half-life of 51Mn

RADIOACTIVITY 51Mn(β+), (EC)[from 54Fe(p, α), E=16 MeV]; measured Eγ, Iγ, half-life of 51Mn decay from decay curve of 511-keV annihilation radiation following positron emission. Comparison with previous measurements, and with evaluated data in the Nuclear Data Sheets.

doi: 10.1103/PhysRevC.96.014613
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Data from this article have been entered in the XUNDL database. For more information, click here.


2017VA23      Appl.Radiat.Isot. 130, 90 (2017)

H.F.Valdovinos, R.Hernandez, S.Graves, P.A.Ellison, T.E.Barnhart, C.P.Theuer, J.W.Engle, W.Cai, R.J.Nickles

Cyclotron production and radiochemical separation of 55Co and 58mCo from 54Fe, 58Ni and 57Fe targets

NUCLEAR REACTIONS 54,56,57Fe, 23Na(d, n), 54,58Fe(d, α), E=8.2 MeV; 58,60Ni(p, α), 58Ni(p, np), E=16 MeV; measured reaction products, Eγ, Iγ; deduced yields.

doi: 10.1016/j.apradiso.2017.09.005
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2016GR14      Nucl.Instrum.Methods Phys.Res. B386, 44 (2016)

S.A.Graves, P.A.Ellison, T.E.Barnhart, H.F.Valdovinos, E.R.Birnbaum, F.M.Nortier, R.J.Nickles, J.W.Engle

Nuclear excitation functions of proton-induced reactions (Ep = 35-90 MeV) from Fe, Cu, and Al

NUCLEAR REACTIONS Cu(p, X)55Co/57Co/58Co/60Co/61Cu/64Cu/52Mn/54Mn/56Ni/57Ni, Fe(p, X)55Co/56Co/48Cr/51Cr/52Fe/52Mn/54Mn/48V, E=90 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS nuclear model code calculations.

doi: 10.1016/j.nimb.2016.09.018
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2243.


2012EN01      Appl.Radiat.Isot. 70, 355 (2012)

J.W.Engle, G.W.Severin, T.E.Barnhart, L.D.Knutson, R.J.Nickles

Cross sections of the 36Ar(d, α)34mCl, 40Ar(d, α)38Cl, and 40Ar(d, p)41Ar nuclear reactions below 8.4 MeV

NUCLEAR REACTIONS 36,40Ar(d, α), (d, p), E<8.4 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ALICE/ASN code calculations.

doi: 10.1016/j.apradiso.2011.10.003
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1885.


2012EN03      Appl.Radiat.Isot. 70, 1792 (2012)

J.W.Engle, V.Lopez-Rodriguez, R.E.Gaspar-Carcamo, H.F.Valdovinos, M.Valle-Gonzalez, F.Trejo-Ballado, G.W.Severin, T.E.Barnhart, R.J.Nickles, M.A.Avila-Rodriguez

Very high specific activity 66/68Ga from zinc targets for PET

NUCLEAR REACTIONS 66Zn, Zn(p, n)66Ga/68Ga, E=7-16 MeV; measured reaction products, Eγ, Iγ; deduced yields. Comparison with available data.

doi: 10.1016/j.apradiso.2012.30.030
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2012SE03      Appl.Radiat.Isot. 70, 1526 (2012)

G.W.Severin, J.W.Engle, H.F.Valdovinos, T.E.Barnhart, R.J.Nickles

Cyclotron produced 44gSc from natural calcium

NUCLEAR REACTIONS Ca(p, X)43Sc/44Sc/47Sc/48Sc, E=16 MeV; measured reaction products; deduced thick target yields, reactivity.

doi: 10.1016/j.apradiso.2012.04.030
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1940.


2011EN01      Appl.Radiat.Isot. 69, 75 (2011)

J.W.Engle, T.E.Barnhart, O.T.DeJesus, R.J.Nickles

Production of 34mCl and 38Cl via the (d, α) reaction on 36Ar and natAr gas at 8.4 MeV

NUCLEAR REACTIONS 36Ar, Ar(d, α)34Cl/38Cl, E=8.4 MeV; measured reaction products, Eγ, Iγ; deduced thick target yields.

doi: 10.1016/j.apradiso.2010.09.009
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2007NY01      Appl.Radiat.Isot. 65, 407 (2007)

J.A.Nye, M.A.Avila-Rodriguez, R.J.Nickles

A new binary compound for the production of 124I via the 124Te(p, n)124I reaction

NUCLEAR REACTIONS 124Te(p, n), E=11 MeV; measured thick-target yield.

doi: 10.1016/j.apradiso.2006.10.012
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1517.


2007SE01      Appl.Radiat.Isot. 65, 318 (2007)

R.G.Selwyn, R.J.Nickles, B.R.Thomadsen, L.A.DeWerd, J.A.Micka

A new internal pair production branching ratio of 90Y: The development of a non-destructive assay for 90Y and 90Sr

RADIOACTIVITY 90Y(β-); measured Eγ, Iγ. 90Zr transition deduced branching ratio for internal pair production.

doi: 10.1016/j.apradiso.2006.08.009
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2000AL06      Appl.Radiat.Isot. 52, 899 (2000)

F.Alves, M.Jensen, H.J.Jensen, R.J.Nickles, S.Holm

Determination of the Excitation Function for the 10B(p, n)10C Reaction with Implications for the Production of [10C]Carbon Dioxide for the use as a PET Tracer

NUCLEAR REACTIONS 10B(p, n), E=5-30 MeV; measured σ; deduced excitation function, thick target yield. Activation technique.

doi: 10.1016/S0969-8043(99)00140-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2468.


1995RO40      Nucl.Instrum.Methods Phys.Res. B103, 523 (1995)

A.D.Roberts, R.J.Nickles, M.Paul, K.E.Rehm, C.J.Jiang, D.J.Blumenthal, J.Gehring, D.Henderson, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel

Production of a Radioactive 18F Ion Beam for Nuclear Reaction Studies

doi: 10.1016/0168-583X(95)00657-5
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1991NI03      J.Labelled Compd.Radiopharm. 30, 120 (1991)

R.J.Nickles

Production of a Broad Range of Radionuclides with an 11 MeV Proton Cyclotron

NUCLEAR REACTIONS, ICPND 13C, 10B, 15N, 18O(p, X), E=11 MeV; measured residual production.


1990DE23      Appl.Radiat.Isot. 41, 789 (1990)

O.T.Dejesus, R.J.Nickles

Production and Purification of 89Zr, a Potential PET Antibody Label

NUCLEAR REACTIONS, ICPND 89Y(p, n), E=11 MeV; measured thick, thin target yields.


1986NI09      Int.J.Appl.Radiat.Isotop. 37, 649 (1986)

R.J.Nickles, S.J.Gatley, J.R.Votaw, M.L.Kornguth

Production of Reactive Fluorine-18

NUCLEAR REACTIONS, ICPND 18O(p, n), 20Ne(d, α), 15N(α, n), 16O(α, np), (3He, X), (t, n), 19F(γ, n), (n, 2n), 23Na(γ, nα), E ≥ threshold; compiled 18F yields.

doi: 10.1016/0883-2889(86)90258-3
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1984NI02      Int.J.Appl.Radiat.Isotop. 35, 117 (1984)

R.J.Nickles, M.E.Daube, T.J.Ruth

An 18O2 Target for the Production of [18F]F2

NUCLEAR REACTIONS, ICPND 18O(p, n), E=10 MeV; measured thick target 18F saturation yield. Cryogenic enriched gas retrieval.

doi: 10.1016/0020-708X(84)90194-7
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1973BE12      Phys.Lett. 43B, 279 (1973)

F.D.Becchetti, P.R.Christensen, V.I.Manko, R.J.Nickles

Ambiguities in Spectroscopic Factors Deduced from a DWBA Analysis of the (16O, 15N) Reaction

NUCLEAR REACTIONS 40,48Ca, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 90,92,94,96Zr, 92Mo(16O, 15N), E approx 60 MeV; measured σ(E(15N), θ). 41,49Sc, 55Co, 59,65Cu, 87,89Y, 93,97Nb; deduced S.

doi: 10.1016/0370-2693(73)90439-5
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1973BE13      Nucl.Phys. A203, 1 (1973)

F.D.Becchetti, P.R.Christensen, V.I.Manko, R.J.Nickles

Elastic and Inelastic Scattering of 16O and 12C from A = 40-96 Nuclei

NUCLEAR REACTIONS 40,48Ca, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 92,96Zr, 92Mo(16O, 16O), E=60 MeV; 96Zr(16O, 16O), E=49 MeV; 96Zr(12C, 12C), E=38 MeV; 96Zr(12C, 12C'), E=38 MeV; 48Ca, 54Fe, 58Ni, 88Sr, 96Zr(16O, 16O'), E=60 MeV; measured σ(θ); deduced optical model parameters. 48Ca, 54Fe, 58Ni, 88Sr, 96Zr, deduced deformation parameters β.

doi: 10.1016/0375-9474(73)90420-X
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1973CH10      Nucl.Phys. A207, 33 (1973)

P.R.Christensen, V.I.Manko, F.D.Becchetti, R.J.Nickles

A Study of 16,18O and 12C Induced Reactions on A = 40-96 Nuclei

NUCLEAR REACTIONS 58Ni(16O, 13N), 54Fe(16O, 15O), 40,48Ca, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 90,92,94Zr, 92Mo(16O, 16O), (16O, 15N), (16O, 12C), 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 90,92,94Zr, 92Mo(16O, 14C), 48Ca, 92,94,96Zr(16O, 17O), 54Fe, 86,88Sr, 90Zr(16O, 14N), 58Ni, 88Sr(16O, 13C), 54Fe, 58,60Ni, 64Zn, 90Zr(18O, 20Ne), (18O, 19F), (18O, 18O), 54Fe, 58,60Ni(18O, 16O), E=60 MeV; 96Zr(12C, 12C), (12C, 13C), (12C, 11B), E=38 MeV; 90Zr(16O, 16O), (16O, 14N), (16O, 15N), (16O, 12C), (16O, 14C), (18O, 20Ne), (18O, 19F), (18O, 18O), E=66 MeV; 96Zr(16O, 16O), (16O, 17O), (16O, 15N), (16O, 12C), (16O, 14C), E=47, 49 MeV; measured σ(θ); deduced optical model parameters, Q-value effects, particle transfer probabilities.

doi: 10.1016/0375-9474(73)90023-7
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1971MA09      Phys.Lett. 34B, 133 (1971)

R.D.Macfarlane, N.S.Oakey, R.J.Nickles

Beta-Neutrino Correlations and Longitudinal Nuclear Alignment in the Decay of 20Na

RADIOACTIVITY 20Na; measured β-delayed α-spectra; deduced βν anisotropy coefficients.

doi: 10.1016/0370-2693(71)90688-5
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1971NI03      Phys.Rev.Lett. 26, 1267 (1971)

R.J.Nickles, V.I.Manko, P.R.Christensen, F.D.Becchetti

Study of One- and Two-Nucleon Transfer Reactions Induced by 16O Ions Incident on the Even Zr Isotopes

NUCLEAR REACTIONS 90,92,94,96Zr(16O, 15N), (16O, 14C), E=60 MeV; measured σ(E(15N), θ(15N)), σ(E(14C), θ(14C)). 91,93,95,97Nb, 92,94,96Mo deduced transition strengths.

doi: 10.1103/PhysRevLett.26.1267
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1971NI04      Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 65 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 60 (1972)

R.J.Nickles, P.L.Jolivette, G.M.Klody

Oxygen-Beryllium Neutron Tunnelling below the Coulomb Barrier

NUCLEAR REACTIONS 9Be(16O, 17O), E=6-19 MeV; 9Be(18O, 19O), E=12-14 MeV; measured σ(E;Eγ).


1969NI09      Nucl.Phys. A134, 308 (1969)

R.J.Nickles

Some Lifetimes in the A=15-25 Mass Range

NUCLEAR REACTIONS 6,7Li, 9Be, 10B(14N, X), (16O, X), (17O, X), (18O, X), E=15 MeV; measured Doppler-shift attenuation, plunger method. 15,16N, 16,17,18,19O, 19,20F, 19,20,21,22Ne, 23,25Na, 25Mg deduced T1/2 (level). Enriched targets.

doi: 10.1016/0375-9474(69)91054-9
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1966PA03      Nucl.Phys. 75, 515(1966)

D.W.Palmer, W.G.Mourad, J.M.Donhowe, K.E.Nielsen, R.J.Nickles

Shape of Neutron Yield from the 7Li(p, n)7Be Neutrons Near Threshold and Threshold Energy Determination

NUCLEAR REACTIONS 7Li(p, n), E = 1.88 MeV; measured σ(E); deduced effects on threshold of discrete energy levels by protons. Natural target.

doi: 10.1016/0029-5582(66)90973-4
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