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NSR database version of April 27, 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 T_1/2 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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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 (E_p = 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 T_1/2 (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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