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NSR database version of April 11, 2024.

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2024SA12      Phys.Rev. C 109, 025808 (2024)

R.N.Sahoo, M.Paul, Y.Kashiv, M.Tessler, M.Friedman, S.Halfon, A.Kreisel, A.Shor, L.Weissman

Stellar s-process neutron capture cross section of Ce isotopes

doi: 10.1103/PhysRevC.109.025808
Citations: PlumX Metrics


2022PA36      Eur.Phys.J. A 58, 207 (2022)

M.Paul, M.Tessler, M.Friedman, S.Halfon, L.Weissman

The liquid-lithium target at the soreq applied research accelerator facility

doi: 10.1140/epja/s10050-022-00863-y
Citations: PlumX Metrics


2022TE02      Phys.Rev. C 105, 035801 (2022)

M.Tessler, M.Paul, S.Halfon, Y.Kashiv, D.Kijel, A.Kreisel, A.Shor, L.Weissman

Stellar s-process neutron capture cross sections of 69, 71Ga

NUCLEAR REACTIONS 69,71Ga(n, γ), kT ≈ 40 keV; measured Eγ, Iγ; deduced capture σ, Maxwellian averaged σ (MACS) for kT=30 keV using the energy dependence from ENDF/B-VIII.0, JENDL-4.0, JEFF-3.3, CENDL-3.2 and TENDL-2019 libraries. Activation technique. Neutron activation performed at the superconducting linear accelerator of the Soreq Applied Research Accelerator Facility (SARAF) using the 7Li(p, n) (Ep=1925 keV) reaction via LiLiT - liquid lithium target. Comparison to compiled and evaluated KADoNiS database, and previous experimental results.

RADIOACTIVITY 70Ga(β-)[from 69Ga(n, γ), kT ≈ 40 keV]; measured Eγ, Iγ; deduced T1/2.

doi: 10.1103/PhysRevC.105.035801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31850. Data from this article have been entered in the XUNDL database. For more information, click here.


2021TE06      Phys.Rev. C 104, 015806 (2021)

M.Tessler, J.Zappala, S.Cristallo, L.Roberti, M.Paul, S.Halfon, T.Heftrich, W.Jiang, D.Kijel, A.Kreisel, M.Limongi, Z.-T.Lu, P.Muller, R.Purtschert, R.Reifarth, A.Shor, D.Veltum, D.Vescovi, M.Weigand, L.Weissman

Stellar s-process neutron capture cross sections on 78, 80, 84, 86Kr determined via activation, atom trap trace analysis, and decay counting

NUCLEAR REACTIONS 78,80,84,86Kr(n, γ)79Kr/79mKr/80Kr/81Kr/81mKr/84Kr/85Kr/85mKr/87Kr, kT=42.5 keV, quasi-Maxwellian; 80,86Kr(γ, n)79Kr/85mKr, E=14.6, 17.6 MeV; measured Eγ, Iγ, average σ(E), 81Kr/80Kr and 85Kr/84Kr isotopic ratios in (n, γ) reactions by activation method, Atom Trap Trace Analysis (ATTA) and decay counting at SARAF-LiLiT facility, Argonne National Laboratory and low-level counting (LLC) facility of the University of Bern; deduced Maxwellian-averaged cross sections (MACS) at kt=3-300 keV, and stellar reaction rates for s-process in 0.01-4 GK range for (n, γ) reactions. 197Au(n, γ)198Au, kT=42.5 keV; 197Au(γ, n)196Au, E=14.6, 17.6 MeV; measured Eγ, Iγ, used as monitor reactions. Comparison with previous experimental cross sections, and with data in JEFF-3.3 library. Discussed astrophysical implications, and impact on s-process calculations of abundances of krypton and neighboring nuclides.

RADIOACTIVITY 79Kr(EC); 85mKr(IT); 85mKr, 87Kr(β-)[from 78,84,86Kr(n, γ), kT=42.5 keV]; measured half-lives from γ-decay curves and compared with evaluated data.

doi: 10.1103/PhysRevC.104.015806
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31837. Data from this article have been entered in the XUNDL database. For more information, click here.


2019GU28      Phys.Lett. B 797, 134809 (2019); Erratum Phys.Lett. B 802, 135268 (2020)

C.Guerrero, M.Tessler, M.Paul, J.Lerendegui-Marco, S.Heinitz, E.A.Maugeri, C.Domingo-Pardo, R.Dressler, S.Halfon, N.Kivel, U.Koster, T.Palchan-Hazan, J.M.Quesada, D.Schumann, L.Weissman

The s-process in the Nd-Pm-Sm region: Neutron activation of 147Pm

NUCLEAR REACTIONS 147Pm, 197Au(n, γ), E ∼ 40 keV; measured reaction products, Eγ, Iγ; deduced Maxwellian averaged σ. Comparison with available data.

doi: 10.1016/j.physletb.2019.134809
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31815.


2019PA01      Nucl.Instrum.Methods Phys.Res. B438, 77 (2019)

S.Pavetich, A.Carey, L.K.Fifield, M.B.Froehlich, S.Halfon, A.Kinast, M.Martschini, D.Nelson, M.Paul, A.Shor, J.H.Sterba, M.Tessler, S.G.Tims, L.Weissman, A.Wallner

93Zr developments at the Heavy Ion Accelerator Facility at ANU

NUCLEAR REACTIONS 92Zr(n, γ), E thermal; measured reaction products; deduced sensitivity and rejection of 93Nb background.

doi: 10.1016/j.nimb.2018.07.019
Citations: PlumX Metrics


2019PA03      Phys.Rev. C 99, 015801 (2019)

S.Pavetich, A.Wallner, M.Martschini, S.Akhmadaliev, I.Dillmann, K.Fifield, S.Halfon, T.Heftrich, F.Kappeler, C.Lederer-Woods, S.Merchel, M.Paul, R.Reifarth, G.Rugel, P.Steier, M.Tessler, S.Tims, M.Weigand, L.Weissman

Accelerator mass spectrometry measurement of the reaction 35Cl (n, γ) 36Cl at keV energies

NUCLEAR REACTIONS 35Cl(n, γ), kT=2-100 keV; measured Maxwellian averaged σ(E) (MACS) using neutron activation combined with accelerator mass spectrometry (AMS) technique; deduced 36Cl/35Cl ratios for three neutron irradiated samples, MACS at kt=30 keV, and stellar abundances of 35Cl, 36Cl and 36S. Neutron activations performed at the Karlsruhe Van de Graaff accelerator and at the superconducting linear accelerator of the Soreq Applied Research Accelerator Facility using the 7Li(p, n)7Be reaction. AMS measurements of the irradiated samples performed at the 3 MV Vienna Environmental Research Accelerator, the 6 MV tandem accelerator at the Dresden AMS facility, and the 14 UD tandem accelerator of the Australian National University in Canberra. Comparison with previous experimental values, NON-SMOKER and MOST theoretical calculations, compiled KADoNiS database, and evaluated libraries ENDF-B/VII.1, JEFF-3.2, JENDL-4.0 and TENDL-2015.

doi: 10.1103/PhysRevC.99.015801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23468.


2019PA22      Eur.Phys.J. A 55, 44 (2019)

M.Paul, M.Tessler, M.Friedman, S.Halfon, T.Palchan, L.Weissman, A.Arenshtam, D.Berkovits, Y.Eisen, I.Eliahu, G.Feinberg, D.Kijel, A.Kreisel, I.Mardor, G.Shimel, A.Shor, I.Silverman

Reactions along the astrophysical s-process path and prospects for neutron radiotherapy with the Liquid-Lithium Target (LiLiT) at the Soreq Applied Research Accelerator Facility (SARAF)

NUCLEAR REACTIONS 7Li(p, n)7Be, E=1880.4 - 1.92 keV[reaction threshold]; measured thick-target Eγ, Iγ(θ) using the Liquid-Lithium Target (LiLiT) system with the Soreq Applied Research Accelerator Facility (SARAF) Phase I; deduced astrophysical s-process sequence of nuclei.

doi: 10.1140/epja/i2019-12723-5
Citations: PlumX Metrics


2019PA57      Nucl.Instrum.Methods Phys.Res. B438, 172 (2019)

R.C.Pardo, T.Palchan-Hazan, R.Scott, M.Paul, O.Nusair, W.Bauder, R.Vondrasek, D.Seweryniak, S.Baker, R.Talwar, P.Collon, F.G.Kondev, G.Youinou, M.Salvatores, G.Palmiotti, J.Berg, J.Giglio, M.T.Giglio, G.Imel, C.Nair, C.L.Jiang

Laser Ablation Positive-Ion AMS of Neutron Activated Actinides

NUCLEAR REACTIONS 236U, 242Pu(n, X), E not given; measured reaction products; deduced neutron transmutation rates by accelerator mass spectrometry.

doi: 10.1016/j.nimb.2018.05.004
Citations: PlumX Metrics


2019WE14      Phys.Rev. C 100, 065804 (2019)

L.Weissman, M.Tessler, A.Barak, H.Dafna, A.Grin, B.Kaizer, D.Kijel, A.Kreisel, M.Paul, A.Perry, I.Silverman, N.Tamim, T.Zchut

Measurement of 63, 65Cu (n, γ)64, 66Cu and 59Co(n, γ)60Co Maxwellian-averaged neutron-capture cross sections

NUCLEAR REACTIONS 59Co, 63,64Cu(n, γ)60Co/64Cu/65Cu, E=20-40 keV, [neutron beam from 7Li(p, n), E=1.90-1.94 MeV using liquid lithium target]; measured Eγ, Iγ, capture σ using activation method at the Soreq Applied Research Accelerator Facility (SARAF) facility; deduced Maxwellian averaged cross sections (MACS) at E(n)=30 keV from the experimental cross sections using ENDF/B-VIII.0, JENDL-4.0, JEFF-3.3, and TENDL-2017 nuclear reaction data libraries. Comparison with previous experimental results in the literature. Relevance to abundances of the heavier elements produced via the astrophysical s process.

doi: 10.1103/PhysRevC.100.065804
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31817.


2018MA39      Eur.Phys.J. A 54, 91 (2018)

I.Mardor, O.Aviv, M.Avrigeanu, D.Berkovits, A.Dahan, T.Dickel, I.Eliyahu, M.Gai, I.Gavish-Segev, S.Halfon, M.Hass, T.Hirsh, B.Kaiser, D.Kijel, A.Kreisel, Y.Mishnayot, I.Mukul, B.Ohayon, M.Paul, A.Perry, H.Rahangdale, J.Rodnizki, G.Ron, R.Sasson-Zukran, A.Shor, I.Silverman, M.Tessler, S.Vaintraub, L.Weissman

The Soreq Applied Research Accelerator Facility (SARAF): Overview, research programs and future plans

doi: 10.1140/epja/i2018-12526-2
Citations: PlumX Metrics


2018SH12      Phys.Rev. C 97, 034303 (2018)

A.Shor, L.Weissman, O.Aviv, Y.Eisen, M.Brandis, M.Paul, A.Plompen, M.Tessler, S.Vaintraub

Branching ratio to the 803 keV level in 210Po α decay

RADIOACTIVITY 210Po(α)[from 210Bi(β-) decay, 210Bi from 209Bi(n, γ), E=thermal at Soreq nuclear reactor facility]; measured Eγ, Iγ, Eα, Iα, α-branching ratio to the 803-keV level in 206Pb. Comparison with previous experimental results from 1951 to 1999, and evaluated data in ENSDF and DDEP databases. Relevance to cross section for 209Bi(n, γ)210Bi involved in termination of the astrophysical s process.

NUCLEAR REACTIONS 209Bi(n, γ), E=thermal; measured Eα, Iα from decay of 210Po; deduced σ for thermal capture σ.

doi: 10.1103/PhysRevC.97.034303
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2018TE04      Phys.Rev.Lett. 121, 112701 (2018)

M.Tessler, M.Paul, S.Halfon, B.S.Meyer, R.Pardo, R.Purtschert, K.E.Rehm, R.Scott, M.Weigand, L.Weissman, S.Almaraz-Calderon, M.L.Avila, D.Baggenstos, P.Collon, N.Hazenshprung, Y.Kashiv, D.Kijel, A.Kreisel, R.Reifarth, D.Santiago-Gonzalez, A.Shor, I.Silverman, R.Talwar, D.Veltum, R.Vondrasek

Stellar 36, 38Ar(n, γ)37, 39Ar Reactions and Their Effect on Light Neutron-Rich Nuclide Synthesis

NUCLEAR REACTIONS 36,38Ar(n, γ), E ∼ 30 keV; measured reaction products, Eβ, Iβ; deduced thermal σ, Maxwellian average cross sections (MACS). Comparison with available data.

doi: 10.1103/PhysRevLett.121.112701
Citations: PlumX Metrics


2017OS02      Phys.Rev. C 95, 055809 (2017)

K.M.Ostdiek, T.S.Anderson, W.K.Bauder, M.R.Bowers, A.M.Clark, P.Collon, W.Lu, A.D.Nelson, D.Robertson, M.Skulski, R.Dressler, D.Schumann, J.P.Greene, W.Kutschera, M.Paul

Activity measurement of 60Fe through the decay of 60mCo and confirmation of its half-life

RADIOACTIVITY 60Fe(β-)[from Cu(p, X), E=590 MeV at PSI followed by chemical separation]; 60mCo(IT); measured Eγ, Iγ from 60mCo decay, half-life of 60Fe via the 2+ isomeric state of 60Co, number of atoms of 60Fe from 60Fe/56Fe isotopic ratios of samples using accelerator mass spectrometry (AMS) technique. Experiments performed at the university of Notre Dame. Comparison with previous half-life measurements.

doi: 10.1103/PhysRevC.95.055809
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2017SH47      Phys.Rev. C 96, 055805 (2017)

A.Shor, M.Tessler, A.Plompen, A.Arenshtam, O.Aviv, D.Berkovits, M.Brandis, Y.Eisen, I.Eliyahu, G.Feinberg, M.Friedman, S.Halfon, M.Hult, B.Kaizer, D.Kijel, A.Krasa, A.Kreisel, T.Palchan, M.Paul, A.Perry, I.Silverman, S.Vaintraub, L.Weissman

Bismuth activation with quasi-Maxwellian neutrons at kT ∼ 30 keV

NUCLEAR REACTIONS 209Bi(n, γ), kT≈30 keV quasi-Maxwellian neutrons; measured Eβ from the decay of 210Bi and Eα and Eγ, Iγ from the decay of 206Po using PIPS silicon detector for particles and HPGe detector for γ rays at the linear accelerator of Soreq Applied Research Accelerator facility (SARAF); deduced Maxwellian averaged (MACS) σ, and compared with previous experimental results, and with evaluated cross sections in the ENDF, JEFF and JENDL data libraries. Relevance to termination point of the s-process cycle of nucleosynthesis in stellar environments.

doi: 10.1103/PhysRevC.96.055805
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31780.


2017WE08      Phys.Rev. C 96, 015802 (2017)

L.Weissman, M.Tessler, A.Arenshtam, I.Eliyahu, S.Halfon, C.Guerrero, B.Kaizer, D.Kijel, A.Kreisel, T.Palchan, M.Paul, A.Perry, G.Schimel, I.Silverman, A.Shor, N.Tamim, S.Vaintraub

Measurement of 208Pb(n, γ)209Pb Maxwellian averaged neutron capture cross section

NUCLEAR REACTIONS 208Pb, 197Au, 63Cu(n, γ), E=30 keV, quasi-Maxwellian neutron source produced in Li(p, n), E=1.94 MeV; measured Eβ, Iβ, Eγ, Iγ, MACS cross sections by activation method at Soreq Applied Research Accelerator Facility (SARAF). Monte Carlo simulations performed with the codes SIMLIT-GEANT4. Comparison with previous experimental data, and with ENDF and JENDL evaluated nuclear data libraries.

doi: 10.1103/PhysRevC.96.015802
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31779.


2016MU05      Phys.Rev. C 93, 065502 (2016)

H.P.Mumm, M.G.Huber, W.Bauder, N.Abrams, C.M.Deibel, C.R.Huffer, P.R.Huffman, K.W.Schelhammer, R.Janssens, C.L.Jiang, R.H.Scott, R.C.Pardo, K.E.Rehm, R.Vondrasek, C.M.Swank, C.M.O'Shaughnessy, M.Paul, L.Yang

High-sensitivity measurement of 3He - 4He isotopic ratios for ultracold neutron experiments

ATOMIC MASSES 3,4He; measured absolute isotopic ratio of 3He to 4He with a high sensitivity at ATLAS-ANL facility. Relevance to neutron half-life measurements using ultra-cold neutrons.

doi: 10.1103/PhysRevC.93.065502
Citations: PlumX Metrics


2016WA09      Nature(London) 532, 69 (2016)

A.Wallner, J.Feige, N.Kinoshita, M.Paul, L.K.Fifield, R.Golser, M.Honda, U.Linnemann, H.Matsuzaki, S.Merchel, G.Rugel, S.G.Tims, P.Steier, T.Yamagata, S.R.Winkler

Recent near-Earth supernovae probed by global deposition of interstellar radioactive 60Fe

ATOMIC MASSES 60Fe; measured 60Fe/Fe ratios using atomic mass spectroscopy; deduced the rate of supernovae in our local Galactic neighbourhood.

doi: 10.1038/nature17196
Citations: PlumX Metrics


2015OS02      Nucl.Instrum.Methods Phys.Res. B361, 638 (2015)

K.Ostdiek, T.Anderson, W.Bauder, M.Bowers, P.Collon, R.Dressler, J.Greene, W.Kutschera, W.Lu, M.Paul, D.Robertson, D.Schumann, M.Skulski, A.Wallner

Towards a measurement of the half-life of 60Fe for stellar and early Solar System models

RADIOACTIVITY 60Fe(β-); measured decay products; deduced T1/2. Accelerator mass spectrometry, comparison with available data.

doi: 10.1016/j.nimb.2015.05.033
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2015TE06      Phys.Lett. B 751, 418 (2015)

M.Tessler, M.Paul, A.Arenshtam, G.Feinberg, M.Friedman, S.Halfon, D.Kijel, L.Weissman, O.Aviv, D.Berkovits, Y.Eisen, I.Eliyahu, G.Haquin, A.Kreisel, I.Mardor, G.Shimel, A.Shor, I.Silverman, Z.Yungrais

Stellar 30-keV neutron capture in 94, 96Zr and the 90Zr(γ, n)89Zr photonuclear reaction with a high-power liquid-lithium target

NUCLEAR REACTIONS 94,96Zr(n, γ), E=30 keV; 90Zr(γ, n), E not given; measured reaction products, Eγ, Iγ; deduced yields, Maxwellian averaged σ. Comparison with available data.

doi: 10.1016/j.physletb.2015.10.058
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31765.


2014CA08      Phys.Rev.Lett. 112, 192701 (2014)

P.F.F.Carnelli, S.Almaraz-Calderon, K.E.Rehm, M.Albers, M.Alcorta, P.F.Bertone, B.Digiovine, H.Esbensen, J.O.Fernandez Niello, D.Henderson, C.L.Jiang, J.Lai, S.T.Marley, O.Nusair, T.Palchan-Hazan, R.C.Pardo, M.Paul, C.Ugalde

Measurements of Fusion Reactions of Low-Intensity Radioactive Carbon Beams on 12C and their Implications for the Understanding of X-Ray Bursts

NUCLEAR REACTIONS 12C(10C, X), (12C, X), (13C, X), (14C, X), (15C, X), E=40-50 MeV; measured fusion reaction products; deduced S-factors, σ. Time-dependent HF calculations.

doi: 10.1103/PhysRevLett.112.192701
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2117.


2014YO05      Nucl.Data Sheets 119, 169 (2014)

G.Youinou, R.Vondrasek, H.Veselka, M.Salvatores, M.Paul, R.Pardo, G.Palmiotti, T.Palchan, O.Nusair, J.Nimmagadda, C.Nair, P.Murray, T.Maddock, S.Kondrashev, F.G.Kondev, W.Jones, G.Imel, C.Glass, J.Fonnesbeck, J.Berg, W.Bauder

MANTRA: An Integral Reactor Physics Experiment to Infer the Neutron Capture Cross Sections of Actinides and Fission Products in Fast and Epithermal Spectra

doi: 10.1016/j.nds.2014.08.047
Citations: PlumX Metrics


2013FR01      Nucl.Instrum.Methods Phys.Res. A698, 117 (2013)

M.Friedman, D.Cohen, M.Paul, D.Berkovits, Y.Eisen, G.Feinberg, G.Giorginis, S.Halfon, A.Krasa, A.J.M.Plompen, A.Shor

Simulation of the neutron spectrum from the 7Li(p, n) reaction with a liquid-lithium target at Soreq Applied Research Accelerator Facility

NUCLEAR REACTIONS 7Li(p, n), E<3.5 MeV; analyzed available data; deduced neutron source parameters for Maxwellian-averaged σ measurements. Comparison with available data.

doi: 10.1016/j.nima.2012.09.027
Citations: PlumX Metrics


2012FE06      Phys.Rev. C 85, 055810 (2012)

G.Feinberg, M.Friedman, A.Krasa, A.Shor, Y.Eisen, D.Berkovits, D.Cohen, G.Giorginis, T.Hirsh, M.Paul, A.J.M.Plompen, E.Tsuk

Quasi-stellar neutrons from the 7Li(p, n)7Be reaction with an energy-broadened proton beam

NUCLEAR REACTIONS 7Li(p, n)7Be, E=1.85-1.95 MeV; measured time of flight, spectrum, E(n), I(n), σ(θ), narrow and broad-energy proton beam; deduced angle-integrated spectrum and Maxwellian-flux distribution. 27Al(p, γ), E=0.985-1.0 MeV; measured thick-target σ(E). 197Au(n, γ), E<160 keV; measured Eγ, Iγ, average activation σ for neutrons from 7Li(p, n) reaction. Relevance to s-process cross sections.

doi: 10.1103/PhysRevC.85.055810
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23284.


2012FE11      J.Phys.:Conf.Ser. 337, 012044 (2012)

G.Feinberg, A.Shor, D.Berkovits, Y.Eisen, M.Friedman, G.Giorginis, T.Hirsh, A.Krasa, M.Paul, A.Plompen, E.Tsuk

Energy-broadened proton beam for production of quasi-stellar neutrons from the 7Li(p, n)7Be reaction

NUCLEAR REACTIONS 7Li(p, n), E=1912 keV; measured thick target En, In(θ) using ToF with 6Li glass detectors and both narrow- and broad-energy beams; deduced σ(En, θ).

doi: 10.1088/1742-6596/337/1/012044
Citations: PlumX Metrics


2012KI16      Science 335, 1614 (2012)

N.Kinoshita, M.Paul, Y.Kashiv, P.Collon, C.M.Deibel, B.DiGiovine, J.P.Greene, D.J.Henderson, C.L.Jiang, S.T.Marley, T.Nakanishi, R.C.Pardo, K.E.Rehm, D.Robertson, R.Scott, C.Schmitt, X.D.Tang, R.Vondrasek, A.Yokoyama

A Shorter 146Sm Half-Life Measured and Implications for 146Sm-142Nd Chronology in the Solar System

RADIOACTIVITY 146Sm(α); measured decay products, Eα, Iα; deduced T1/2 and its uncertainty and 146Sm/144Sm ratio. 146Sm - 142Nd clock, comparison with available data.

doi: 10.1126/science.1215510
Citations: PlumX Metrics


2011AL09      Phys.Rev.Lett. 106, 172701 (2011)

M.Alcorta, K.E.Rehm, B.B.Back, S.Bedoor, P.F.Bertone, C.M.Deibel, B.DiGiovine, H.Esbensen, J.P.Greene, C.R.Hoffmann, C.L.Jiang, J.C.Lighthall, S.T.Marley, R.C.Pardo, M.Paul, A.M.Rogers, C.Ugalde, A.H.Wuosmaa

Fusion Reactions with the One-Neutron Halo Nucleus 15C

NUCLEAR REACTIONS 232Th(13C, X), (14C, X), (15C, X), E(cm)=50-70 MeV; measured fusion fission fragments; deduced yields, σ, 15C+232Th cross section enhancement. Comparison with experimental data, couple-channel calculations.

doi: 10.1103/PhysRevLett.106.172701
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1831.


2011DE28      Phys.Rev. C 84, 045802 (2011)

C.M.Deibel, K.E.Rehm, J.M.Figueira, J.P.Greene, C.L.Jiang, B.P.Kay, H.Y.Lee, J.C.Lighthall, S.T.Marley, R.C.Pardo, N.Patel, M.Paul, C.Ugalde, A.Woodard, A.H.Wuosmaa, G.Zinkann

First measurement of the 33Cl(p, α)30S reaction

NUCLEAR REACTIONS 1H(33Cl, α)30S, [33Cl secondary beam from 2H(32S, 33Cl), E=320 MeV primary reaction], E=208.1, 229.1, 250.6 MeV; measured Eα, Iα, particle spectra, (30S)α-coin; deduced cross sections. Enge split-pole magnetic spectrograph. Comparison of measured σ with NON-SMOKER code calculations.

doi: 10.1103/PhysRevC.84.045802
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1869.


2011YO13      J.Korean Phys.Soc. 59, 1940s (2011)

G.Youinou, G.Palmiotti, C.McGrath, G.Imel, M.Paul, R.Pardo, F.Kondev, M.Salvatores

MANTRA: An Integral Reactor Physics Experiment to Infer Actinide Capture Cross-Sections from Thorium to Californium with Accelerator Mass Spectrometry

doi: 10.3938/jkps.59.1940
Citations: PlumX Metrics


2010TA05      Phys.Rev. C 81, 045809 (2010)

X.D.Tang, K.E.Rehm, I.Ahmad, C.R.Brune, A.Champagne, J.P.Greene, A.Hecht, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, D.Kahl, E.F.Moore, M.Notani, R.C.Pardo, N.Patel, M.Paul, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, A.H.Wuosmaa

Determination of the E1 component of the low-energy 12C(α, γ)16O cross section

RADIOACTIVITY 16N(β-α); measured Eα, Iα, α12C-coin, half-life; deduced E1 component of the S factor for 12C(α, γ)16O reaction using a set of twin ionization chambers. R-matrix analysis. Comparison with previous studies.

NUCLEAR REACTIONS 2H(15N, p)15N/16N/16O/20Ne, E=82 MeV; measured fragment yields.

doi: 10.1103/PhysRevC.81.045809
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2009DI04      Phys.Rev. C 79, 065805 (2009)

I.Dillmann, C.Domingo-Pardo, M.Heil, F.Kappeler, A.Wallner, O.Forstner, R.Golser, W.Kutschera, A.Priller, P.Steier, A.Mengoni, R.Gallino, M.Paul, C.Vockenhuber

Determination of the stellar (n, γ) cross section of 40Ca with accelerator mass spectrometry

NUCLEAR REACTIONS 40Ca(n, γ), E<106 keV; measured σ, σ(E) using activation technique and accelerator mass spectrometry; deduced Maxwellian averaged cross sections. Neutrons from 7Li(p, n)7Be reaction at E(p)=1912 keV. 197Au(n, γ), E<106 keV; measured σ and used as a standard. Comparison with previous experimental data and theoretical predictions.

doi: 10.1103/PhysRevC.79.065805
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2009FE12      Nucl.Phys. A827, 590c (2009)

G.Feinberg, M.Paul, A.Arenshtam, D.Berkovits, D.Kijel, A.Nagler, I.Silverman

LiLiT - a Liquid-Lithium Target as an Intense Neutron Source for Nuclear Astrophysics at the Soreq Applied Research Accelerator Facility

doi: 10.1016/j.nuclphysa.2009.05.130
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2009JI08      Phys.Rev. C 80, 044613 (2009)

C.L.Jiang, K.E.Rehm, D.Ackermann, I.Ahmad, J.P.Greene, B.Harss, D.Henderson, W.F.Henning, R.V.F.Janssens, J.Nolen, R.C.Pardo, P.Reiter, J.P.Schiffer, D.Seweryniak, A.Sonzogni, J.Uusitalo, I.Wiedenhover, A.H.Wuosmaa, F.Brumwell, G.McMichael, M.Paul, R.E.Segel

Experimental study of the 56Ni(3He, d)57Cu reaction in inverse kinematics

NUCLEAR REACTIONS 3He(56Ni, d), E=250 MeV; measured Ed, Id, σ, σ(θ). 57Cu; deduced levels, J, π, spectroscopic factors. DWBA analysis. Discussed implications for 56Ni(p, γ)57Cu reaction of astrophysical interest.

doi: 10.1103/PhysRevC.80.044613
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2009PA22      Acta Phys.Pol. B40, 685 (2009)

M.Paul

Counting Rare Atoms for Nuclear Astrophysics


2008KI05      J.Phys.(London) G35, 014033 (2008)

N.Kinoshita, T.Hashimoto, T.Nakanishi, A.Yokoyama, H.Amakawa, T.Mitsugashira, T.Ohtsuki, N.Takahashi, I.Ahmad, J.P.Greene, D.J.Henderson, C.L.Jiang, M.Notani, R.C.Pardo, N.Patel, K.E.Rehm, R.Scott, R.Vondrasek, L.Jisonna, P.Collon, D.Robertson, C.Schmitt, X.D.Tang, Y.Kashiv, H.Nassar, M.Paul

Ultra-sensitive detection of p-process nuclide 146Sm produced by (γ, n), (p, 2nε) and (n, 2n) reactions

doi: 10.1088/0954-3899/35/1/014033
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2008VO01      J.Phys.(London) G35, 014034 (2008)

C.Vockenhuber, C.O.Ouellet, L.-S.The, L.Buchmann, J.Caggiano, A.A.Chen, J.M.D'Auria, B.Davids, L.Fogarty, D.Frekers, A.Hussein, D.A.Hutcheon, W.Kutschera, D.Ottewell, M.Paul, M.M.Pavan, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, A.Wallner

40Ca(α, γ)44Ti and the production of 44Ti in supernovae

NUCLEAR REACTIONS 4He(40Ca, γ), E=600-1150 keV/nucleon; measured Eγ, γγ-, (recoil)γ-coin, excitation function.

doi: 10.1088/0954-3899/35/1/014034
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2008WU05      Phys.Rev. C 78, 041302 (2008)

A.H.Wuosmaa, J.P.Schiffer, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, J.C.Lighthall, S.T.Marley, E.F.Moore, R.C.Pardo, N.Patel, M.Paul, D.Peterson, S.C.Pieper, G.Savard, R.E.Segel, R.H.Siemssen, X.D.Tang, R.B.Wiringa

Structure of 7He by proton removal from 8Li with the (d, 3He) reaction

NUCLEAR REACTIONS 2H(8Li, 3He), E=76 MeV; 2H(7Li, t), (7Li, 3He), E=81 MeV; measured charged particle spectra, (particle)(particle)-coin, angular distributions, σ, σ(θ), spectroscopic factors. 7He; deduced levels, J, π. Comparisons with data from 2H(6He, p) experiment. Comparisons with nuclear structure models and variational quantum Monte Carlo calculations.

doi: 10.1103/PhysRevC.78.041302
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2007HA49      J.Nucl.Radiochem.Sci. 8, 109 (2007)

T.Hashimoto, T.Nakanishi, A.Yokoyama, H.Amakawa, T.Mitsugashira, T.Ohtsuki, N.Takahashi, I.Ahmad, J.P.Greene, D.J.Henderson, C.L.Jiang, M.Notani, R.C.Pardo, N.Patel, K.E.Rehm, R.Scott, R.Vondrasek, L.Jisonna, P.Collon, D.Robertson, C.Schmitt, X.D.Tang, Y.Kashiv, M.Paul

Technological Development for Half-life Measurement of 146Sm Nuclide

NUCLEAR REACTIONS 147Sm(γ, n), E < 50 MeV; 147Sm(n, 2n), E=6-10 MeV; 147Sm(p, 2n), E=21 MeV; measured Eα, Iα.


2007PA15      J.Radioanal.Nucl.Chem. 272, 243 (2007)

M.Paul, A.Valenta, I.Ahmad, D.Berkovits, C.Bordeanu, S.Ghelberg, Y.Hashimoto, A.Hershkowitz, S.Jiang, T.Nakanishi, K.Sakamoto

An upper limit to interstellar 244Pu abundance as deduced from radiochemical search in deep-sea sediment: An account

doi: 10.1007/s10967-007-0508-3
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2007TA34      Phys.Rev.Lett. 99, 052502 (2007)

X.D.Tang, K.E.Rehm, I.Ahmad, C.R.Brune, A.Champagne, J.P.Greene, A.A.Hecht, D.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, D.Kahl, E.F.Moore, M.Notani, R.C.Pardo, N.Patel, M.Paul, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, B.Shumard, A.H.Wuosmaa

New Determination of the Astrophysical S Factor SE1 of the 12C(α, γ)16O Reaction

RADIOACTIVITY 16N(β-), (β-α); measured Eα, Iα, 12Cα-coin. 12C(α, γ); deduced astrophysical S-factor.

doi: 10.1103/PhysRevLett.99.052502
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2007VO03      Nucl.Instrum.Methods Phys.Res. B259, 688 (2007)

C.Vockenhuber, C.O.Ouellet, L.Buchmann, J.Caggiano, A.A.Chen, J.M.D'Auria, D.Frekers, A.Hussein, D.A.Hutcheon, W.Kutschera, K.Jayamanna, D.Ottewell, M.Paul, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, A.Wallner

The 40Ca(α, γ)44Ti reaction at DRAGON

NUCLEAR REACTIONS 4He(40Ca, γ)44Ti, E=1.135 MeV/nucleon; measured yield and resonance strength at DRAGON recoil mass spectrometer.

doi: 10.1016/j.nimb.2007.01.222
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2007VO06      Phys.Rev. C 76, 035801 (2007)

C.Vockenhuber, C.O.Ouellet, L.-S.The, L.Buchmann, J.Caggiano, A.A.Chen, H.Crawford, J.M.D'Auria, B.Davids, L.Fogarty, D.Frekers, A.Hussein, D.A.Hutcheon, W.Kutschera, A.M.Laird, R.Lewis, E.O'Connor, D.Ottewell, M.Paul, M.M.Pavan, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, B.Wales, A.Wallner

Measurement of the 40Ca(α, γ)44Ti reaction relevant for supernova nucleosynthesis

NUCLEAR REACTIONS 4He(40Ca, γ)44Ti, E=0.60-1.15 MeV/nucleon; measured recoil energies, yields, and cross section.

doi: 10.1103/PhysRevC.76.035801
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2007WA15      Nucl.Instrum.Methods Phys.Res. B259, 677 (2007)

A.Wallner, M.Bichler, I.Dillmann, R.Golser, F.Kappeler, W.Kutschera, M.Paul, A.Priller, P.Steier, C.Vockenhuber

AMS measurements of 41Ca and 55Fe at VERA - two radionuclides of astrophysical interest

doi: 10.1016/j.nimb.2007.01.207
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2007WU05      Eur.Phys.J. Special Topics 150, 79 (2007)

A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, J.C.Lighthall, S.T.Marley, E.F.Moore, R.C.Pardo, N.Patel, M.Paul, D.Peterson, S.C.Pieper, G.Savard, J.P.Schiffer, R.E.Segal, R.H.Siemssen, S.Sinha, X.Tang, R.B.Wiringa

Nucleon transfer reactions with exotic beams at ATLAS

doi: 10.1140/epjst/e2007-00271-y
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2006AH10      Phys.Rev.C 74, 065803 (2006)

I.Ahmad, J.P.Greene, E.F.Moore, S.Ghelberg, A.Ofan, M.Paul, W.Kutschera

Improved measurement of the 44Ti half-life from a 14-year long study

RADIOACTIVITY 44Ti(EC) [from 45Sc(p, 2n)]; measured Eγ, Iγ, T1/2.

doi: 10.1103/PhysRevC.74.065803
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2006JI06      Phys.Lett. B 640, 18 (2006)

C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, S.Misicu, K.E.Rehm, P.Collon, C.N.Davids, J.Greene, D.J.Henderson, L.Jisonna, S.Kurtz, C.J.Lister, M.Notani, M.Paul, R.Pardo, D.Peterson, D.Seweryniak, B.Shumard, X.D.Tang, I.Tanihata, X.Wang, S.Zhu

First evidence of fusion hindrance for a small Q-value system

NUCLEAR REACTIONS 64Ni(28Si, X), E=63-95 MeV; measured fusion-evaporation σ, fusion excitation function; deduced hindrance at sub-barrier energies. Coupled-channels analysis.

doi: 10.1016/j.physletb.2006.07.007
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2006NA02      Phys.Rev.Lett. 96, 041102 (2006)

H.Nassar, M.Paul, I.Ahmad, Y.Ben-Dov, J.Caggiano, S.Ghelberg, S.Goriely, J.P.Greene, M.Hass, A.Heger, A.Heinz, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, Y.Kashiv, B.S.Nara Singh, A.Ofan, R.C.Pardo, T.Pennington, K.E.Rehm, G.Savard, R.Scott, R.Vondrasek

40Ca(α, γ)44Ti Reaction in the Energy Regime of Supernova Nucleosynthesis

NUCLEAR REACTIONS 4He(40Ca, γ), E(cm) ≈ 0.6-1.2 MeV/nucleon; measured yield. 40Ca(α, γ), E=low; deduced astrophysical reaction rate. Accelerator mass spectrometry.

doi: 10.1103/PhysRevLett.96.041102
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2005JI02      Phys.Rev. C 71, 044613 (2005)

C.L.Jiang, K.E.Rehm, H.Esbensen, R.V.F.Janssens, B.B.Back, C.N.Davids, J.P.Greene, D.J.Henderson, C.J.Lister, R.C.Pardo, T.Pennington, D.Peterson, D.Seweryniak, B.Shumard, S.Sinha, X.D.Tang, I.Tanihata, S.Zhu, P.Collon, S.Kurtz, M.Paul

Hindrance of heavy-ion fusion at extreme sub-barrier energies in open-shell colliding systems

NUCLEAR REACTIONS 100Mo(64Ni, X), E=196-262 MeV; measured fusion-evaporation σ, fusion excitation function; deduced hindrance at sub-barrier energies. 58,60,64Ni, 74Ge, 90,91,94Zr, 92,100Mo, 124Sn(58Ni, X), 89Y(60Ni, X), 64Ni, 74Ge, 92,96Zr, 92,100Mo, 124Sn(64Ni, X), E(cm) ≈ 120 MeV; analyzed fusion σ, sub-barrier hindrance.

doi: 10.1103/PhysRevC.71.044613
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2005NA08      Phys.Rev.Lett. 94, 092504 (2005)

H.Nassar, M.Paul, I.Ahmad, D.Berkovits, M.Bettan, P.Collon, S.Dababneh, S.Ghelberg, J.P.Greene, A.Heger, M.Heil, D.J.Henderson, C.L.Jiang, F.Kappeler, H.Koivisto, S.O'Brien, R.C.Pardo, N.Patronis, T.Pennington, R.Plag, K.E.Rehm, R.Reifarth, R.Scott, S.Sinha, X.Tang, R.Vondrasek

Stellar (n, γ) Cross Section of 62Ni

NUCLEAR REACTIONS 62Ni(n, γ), E=spectrum; measured total σ. Fast-neutron activation, accelerator mass spectrometry. Astrophysical implications discussed.

doi: 10.1103/PhysRevLett.94.092504
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2005NA30      Nucl.Phys. A758, 411c (2005)

H.Nassar, M.Paul, S.Ghelberg, A.Ofan, N.Trubnikov, Y.Ben-Dov, M.Hass, B.S.Nara Singh

Study of the supernova nucleosynthesis 40Ca(α, γ)44Ti reaction: progress report

NUCLEAR REACTIONS 4He(40Ca, γ), E=72 MeV; measured yields. Radiochemical separation, accelerator mass spectrometry. Astrophysical implications discussed.

doi: 10.1016/j.nuclphysa.2005.05.075
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2005WU03      Phys.Rev.Lett. 94, 082502 (2005)

A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, E.F.Moore, R.C.Pardo, M.Paul, D.Peterson, S.C.Pieper, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, X.Tang, R.B.Wiringa

Neutron Spectroscopic Factors in 9Li from 2H(8Li, p)9Li

NUCLEAR REACTIONS 2H(8Li, p), E ≈ 76 MeV; measured Ep, excitation energy spectra, σ(θ). 9Li deduced levels, J, π, spectroscopic factors. Comparison with model predictions.

doi: 10.1103/PhysRevLett.94.082502
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2005WU08      Phys.Rev. C 72, 061301 (2005)

A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, E.F.Moore, R.C.Pardo, M.Paul, D.Peterson, Steven C.Pieper, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, X.Tang, R.B.Wiringa

Search for excited states in 7He with the (d, p) reaction

NUCLEAR REACTIONS 2H(6He, p), E=69 MeV; 2H(7Li, p), E=81 MeV; measured particle spectra, σ(θ). 7He deduced ground-state J, π, excited state energy, width.

doi: 10.1103/PhysRevC.72.061301
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2004GR05      Nucl.Instrum.Methods Phys.Res. A521, 12 (2004)

J.P.Greene, M.C.Wiescher, M.Paul

Using a wide-beam ion source to produce large area sputtered films for low-energy laboratory studies of alpha capture cross-sections

NUCLEAR REACTIONS 24Mg(α, γ), E=1-1.5 MeV; measured Eγ, Iγ. 28Si deduced resonance features. Wide-beam ion source for target production.

doi: 10.1016/j.nima.2003.11.406
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2004JI05      Phys.Rev.Lett. 93, 012701 (2004)

C.L.Jiang, K.E.Rehm, R.V.F.Janssens, H.Esbensen, I.Ahmad, B.B.Back, P.Collon, C.N.Davids, J.P.Greene, D.J.Henderson, G.Mukherjee, R.C.Pardo, M.Paul, T.O.Pennington, D.Seweryniak, S.Sinha, Z.Zhou

Influence of Nuclear Structure on Sub-Barrier Hindrance in Ni + Ni Fusion

NUCLEAR REACTIONS 64Ni(64Ni, X), E=171-220 MeV; measured fusion excitation function; deduced structure effects in sub-barrier hindrance. Comparison with similar reactions.

doi: 10.1103/PhysRevLett.93.012701
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2004JI07      Prog.Theor.Phys.(Kyoto), Suppl. 154, 61 (2004)

C.L.Jiang, H.Esbensen, K.E.Rehm, B.B.Back, R.V.F.Janssens, C.N.Davids, J.P.Greene, D.J.Henderson, G.Mukherjee, R.C.Pardo, T.O.Pennington, D.Seweryniak, S.Sinha, Z.Zhou, M.Paul, P.Collon, J.A.Caggiano, A.M.Heinz, I.Nishinaka

Systematics of Heavy-Ion Fusion Reactions at Extreme Sub-Barrier Energies

NUCLEAR REACTIONS 64Ni(64Ni, X), E=172-212 MeV; measured fusion excitation function; deduced barrier distribution. Fragment mass analyzer, S-factor analysis, fusion reaction systematics discussed.

doi: 10.1143/PTPS.154.61
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2004NA39      Nucl.Phys. A746, 613c (2004)

H.Nassar, S.Ghelberg, M.Paul, S.Dababneh, M.Heil, F.Kappeler, R.Plag, I.Ahmad, J.P.Greene, D.J.Henderson, C.L.Jiang, R.C.Pardo, T.Pennington, K.E.Rehm, R.Scott, S.Sinha, X.Tang, R.Vondrasek, H.Koivisto, D.Berkovits, M.Bettan, R.Reifarth, P.Collon, S.O'Brien, N.Patronis

Production and isobaric separation of 63Ni ions for determination of the 62Ni(n, γ)63Ni reaction cross section at stellar temperatures

NUCLEAR REACTIONS 62Ni(n, γ), E=fast; measured yields.

doi: 10.1016/j.nuclphysa.2004.09.140
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2004WI13      Nucl.Phys. A746, 311c (2004)

W.T.Winter, K.E.Rehm, C.L.Jiang, I.Ahmad, S.J.Freedman, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann

Determination of the 8B neutrino spectrum

RADIOACTIVITY 8B(EC); measured β-delayed Eα; deduced neutrino spectrum. 20Na(EC); measured β-delayed Eα.

doi: 10.1016/j.nuclphysa.2004.09.029
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2003MU09      Nucl.Instrum.Methods Phys.Res. B204, 536 (2003)

P.Muller, L.-B.Wang, K.Bailey, G.W.F.Drake, X.Du, J.Greene, A.M.Heinz, R.J.Holt, D.Henderson, R.V.Janssens, C.-L.Jiang, C.Law, Z.-T.Lu, I.D.Moore, T.P.O'Connor, R.C.Pardo, M.Paul, T.Pennington, K.E.Rehm, J.P.Schiffer

Towards measuring the charge radius of 6He and 8He

RADIOACTIVITY 6He(β-) [from 12C(7Li, 6He)]; measured Eβ, T1/2. Magneto-optical trap for charge radius measurement.

doi: 10.1016/S0168-583X(02)02128-6
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2003PA34      Nucl.Phys. A718, 239c (2003)

M.Paul, C.Feldstein, I.Ahmad, D.Berkovits, C.Bordeanu, J.Caggiano, S.Ghelberg, J.Goerres, J.Greene, M.Hass, A.Heinz, D.Henderson, S.K.Hui, R.V.F.Janssens, C.L.Jiang, S.Jiang, Y.Nirel, R.C.Pardo, T.Pennington, K.E.Rehm, G.Savard, G.Verri, R.Vondrasek, I.Wiedenhover, M.Wiescher

Counting 44Ti Nuclei from the 40Ca(α, γ)44Ti Reaction

NUCLEAR REACTIONS 4He(40Ca, X)44Ti, E=70.9 MeV; measured yield. 44Ti deduced resonance strength. Chemical separation, accelerator mass spectrometry.

doi: 10.1016/S0375-9474(03)00720-6
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2003PA37      Nucl.Phys. A719, 29c (2003)

M.Paul, A.Valenta, I.Ahmad, D.Berkovits, C.Bordeanu, S.Ghelberg, Y.Hashimoto, A.Hershkowitz, S.Jiang, T.Nakanishi, K.Sakamoto

A window on nucleosynthesis through detection of short-lived radionuclides

doi: 10.1016/S0375-9474(03)00954-0
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2003RE16      Phys.Rev. C 67, 065809 (2003)

K.E.Rehm, A.H.Wuosmaa, C.L.Jiang, J.Caggiano, J.P.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, T.Pennington, J.P.Schiffer, R.H.Siemssen, M.Paul, L.Jisonna, R.E.Segel

Branching ratio Γαγ of the 4.033 MeV 3/2+ state in 19Ne

NUCLEAR REACTIONS 3He(20Ne, α), E ≈ 98 MeV; measured particle spectra, yields, (particle)(recoil)-coin; deduced excitation energy spectra. 19Ne levels deduced α-decay branching widths. 15O(α, γ), E=low; deduced astrophysical reaction rates.

doi: 10.1103/PhysRevC.67.065809
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2003RE25      Nucl.Phys. A718, 151c (2003)

K.E.Rehm, A.H.Wuosmaa, C.L.Jiang, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, L.Jisonna, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, J.P.Schiffer, R.E.Segel, R.H.Siemssen

The Branching Ratio Γαγ of the 4.033 MeV State in 19Ne

NUCLEAR REACTIONS 3He(20Ne, α), E=105 MeV; measured particle spectra, (particle)(recoil)-coin. 19Ne levels deduced α-branching ratios, radiative widths. 15O(α, γ), E=low; deduced astrophysical reaction rates.

doi: 10.1016/S0375-9474(03)00706-1
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2003RE26      Nucl.Phys. A718, 443c (2003)

K.E.Rehm, W.Winter, C.L.Jiang, I.Ahmad, S.J.Freedman, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann

Study of the 8B Neutrino Spectrum With a New Technique

RADIOACTIVITY 8B, 20Na(α) [from 3He(6Li, n), (19F, 2n)]; measured Eα.

doi: 10.1016/S0375-9474(03)00841-8
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2003WI11      Nucl.Phys. A721, 553c (2003)

W.Winter, K.E.Rehm, C.L.Jiang, I.Ahmad, S.J.Freedman, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann

Measurement of the 8B Neutrino Spectrum

RADIOACTIVITY 8B, 20Na(β+), (EC) [from 3He(6Li, n) and 3He(19F, 2n)]; measured β-delayed Eα. Mass-separated sources.

doi: 10.1016/S0375-9474(03)01122-9
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2003WI16      Phys.Rev.Lett. 91, 252501 (2003)

W.T.Winter, S.J.Freedman, K.E.Rehm, I.Ahmad, J.P.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, C.L.Jiang, E.F.Moore, G.Mukherjee, R.C.Pardo, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann, M.Paul

Determination of the 8B Neutrino Spectrum

RADIOACTIVITY 8B, 20Na(β+α) [from 3He(6Li, n) and 3He(19F, 2n)]; measured β-delayed Eα, Iα, βα-coin; deduced neutrino spectrum. Comparison with previous results.

doi: 10.1103/PhysRevLett.91.252501
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2002HA15      Phys.Rev. C65, 035803 (2002)

B.Harss, C.L.Jiang, K.E.Rehm, J.P.Schiffer, J.Caggiano, P.Collon, J.P.Greene, D.Henderson, A.Heinz, R.V.F.Janssens, J.Nolen, R.C.Pardo, T.Pennington, R.H.Siemssen, A.A.Sonzogni, J.Uusitalo, I.Wiedenhover, M.Paul, T.F.Wang, F.Borasi, R.E.Segel, J.C.Blackmon, M.Smith, A.Chen, P.Parker

Widths of Astrophysically Important Resonances in 18Ne

NUCLEAR REACTIONS 1H(17F, p), (17F, α), E(cm)=3.07-3.94 MeV; measured σ, σ(E, θ). 17F(p, p'), E(cm) ≈ 3.5 MeV; deduced σ(θ). 14O(α, p), E=low; deduced astrophysical reaction rates. 18Ne deduced resonance parameters.

doi: 10.1103/PhysRevC.65.035803
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2002RE29      Phys.Rev.Lett. 89, 132501 (2002)

K.E.Rehm, C.L.Jiang, I.Ahmad, J.Caggiano, P.Collon, J.P.Greene, D.Henderson, A.Heinz, R.V.F.Janssens, R.C.Pardo, T.Pennington, J.P.Schiffer, R.H.Siemssen, A.H.Wuosmaa, M.Paul, P.Mohr

Large Angle Elastic Alpha Scattering on a N = Z Nucleus above A = 40

NUCLEAR REACTIONS 4He(44Ti, 44Ti), (44Ti, 44Ti'), (40Ca, 40Ca), E(cm)=21.8 MeV; measured σ(θ); deduced angle-integrated σ, optical model parameters.

doi: 10.1103/PhysRevLett.89.132501
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2001BO25      Prog.Part.Nucl.Phys. 46, 97 (2001)

C.Bordeanu, D.Berkovits, E.Boaretto, M.Hass, S.Jiang, M.Paul

Towards a Measurement of σ[3He(4He, γ)7Be] with Accelerator Mass Spectrometry (AMS)

doi: 10.1016/S0146-6410(01)00112-0
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2000HU16      Nucl.Instrum.Methods Phys.Res. B172, 642 (2000)

S.K.Hui, M.Paul, D.Berkovits, E.Boaretto, S.Ghelberg, M.Hass, A.Hershkowitz, E.Navon

44Ti Atom Counting for Nuclear Astrophysics

NUCLEAR REACTIONS 12C(34S, 2n), E=20 MeV; measured production σ. 40Ca(α, γ), E=low; calculated yields. Accelerator mass spectrometry.

doi: 10.1016/S0168-583X(00)00101-4
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2000PA59      Nucl.Instrum.Methods Phys.Res. B172, 152 (2000)

M.Paul

Accelerator Mass Spectrometry and Radioactive-Ion Beams

doi: 10.1016/S0168-583X(00)00278-0
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2000RE11      Nucl.Instrum.Methods Phys.Res. A449, 208 (2000)

K.E.Rehm, F.Borasi, C.J.Jiang, D.Ackermann, I.Ahmad, F.Brumwell, C.N.Davids, P.Decrock, S.M.Fischer, J.Gorres, J.P.Greene, G.Hackmann, B.Harss, D.Henderson, W.Henning, R.V.F.Janssens, G.McMichael, V.Nanal, D.Nisius, J.Nolen, R.C.Pardo, M.Paul, P.Reiter, J.P.Schiffer, D.Seweryniak, R.E.Segel, I.Wiedenhover, M.Wiescher, A.H.Wuosmaa

Experiments with a Radioactive 56Ni Beam

NUCLEAR REACTIONS 63,65Cu, 58Ni(p, X), E=50 MeV; measured delayed Eγ, Iγ; deduced evidence for 56Ni, 56,57Co, 52Mn, 65Zn. 2H(28Si, 29Si), E=125 MeV; 2H(56Co, 57Co), E=250 MeV; measured σ(Ep, θ). 57Co levels deduced spectroscopic factors.

doi: 10.1016/S0168-9002(99)01439-4
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2000SO01      Phys.Rev.Lett. 84, 1651 (2000)

A.A.Sonzogni, K.E.Rehm, I.Ahmad, F.Borasi, D.L.Bowers, F.Brumwell, J.Caggiano, C.N.Davids, J.P.Greene, B.Harss, A.Heinz, D.Henderson, R.V.F.Janssens, C.L.Jiang, G.McMichael, J.Nolen, R.C.Pardo, M.Paul, J.P.Schiffer, R.E.Segel, D.Seweryniak, R.H.Siemssen, J.W.Truran, J.Uusitalo, I.Wiedenhover, B.Zabransky

The 44Ti(α, p) Reaction and Its Implication on the 44Ti Yield in Supernovae

NUCLEAR REACTIONS 44Ti(α, p), E(cm)=5.7-9 MeV; measured σ, astrophysical reaction rate. Comparison with statistical model calculations. Effects on the production of 44Ti in core-collapsed supernovae discussed.

doi: 10.1103/PhysRevLett.84.1651
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1999HA14      Phys.Rev.Lett. 82, 3964 (1999); Comment Phys.Rev.Lett. 84, 1635 (2000)

B.Harss, J.P.Greene, D.Henderson, R.V.F.Janssens, C.L.Jiang, J.Nolen, R.C.Pardo, K.E.Rehm, J.P.Schiffer, R.H.Siemssen, A.A.Sonzogni, J.Uusitalo, I.Wiedenhover, M.Paul, T.F.Wang, F.Borasi, R.E.Segel, J.C.Blackmon, M.S.Smith, A.Chen, P.Parker

Stellar Reactions with Short-Lived Nuclei: 17F(p, α)14O

NUCLEAR REACTIONS 1H(17F, 14O), E(cm)=2.2-3.8 MeV; measured particle energies, (14O)α-coin, σ(E). 18Ne deduced resonance parameters. Implications for astrophysical processes discussed.

doi: 10.1103/PhysRevLett.82.3964
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1998AH03      Phys.Rev.Lett. 80, 2550 (1998)

I.Ahmad, G.Bonino, G.C.Castagnoli, S.M.Fischer, W.Kutschera, M.Paul

Three-Laboratory Measurement of the 44Ti Half-Life

RADIOACTIVITY 44Ti(EC) [from 45Sc(p, 2n), E=45 MeV]; measured T1/2. Astrophysical implications.

doi: 10.1103/PhysRevLett.80.2550
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1998RE01      Phys.Rev.Lett. 80, 676 (1998)

K.E.Rehm, F.Borasi, C.L.Jiang, D.Ackermann, I.Ahmad, B.A.Brown, F.Brumwell, C.N.Davids, P.Decrock, S.M.Fischer, J.Gorres, J.Greene, G.Hackmann, B.Harss, D.Henderson, W.Henning, R.V.F.Janssens, G.McMichael, V.Nanal, D.Nisius, J.Nolen, R.C.Pardo, M.Paul, P.Reiter, J.P.Schiffer, D.Seweryniak, R.E.Segel, M.Wiescher, A.H.Wuosmaa

Study of the 56Ni(d, p)57Ni Reaction and the Astrophysical 56Ni(p, γ)57Cu Reaction Rate

NUCLEAR REACTIONS 2H(56Ni, p), E=250 MeV; measured σ(Ep, θ). 57Ni deduced levels, J, π, spectroscopic factors, astrophysical (p, γ) reaction rates.

doi: 10.1103/PhysRevLett.80.676
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1998RE18      Phys.Rev.Lett. 81, 3341 (1998)

K.E.Rehm, H.Esbensen, C.L.Jiang, B.B.Back, F.Borasi, B.Harss, R.V.F.Janssens, V.Nanal, J.Nolen, R.C.Pardo, M.Paul, P.Reiter, R.E.Segel, A.Sonzogni, J.Uusitalo, A.H.Wuosmaa

Fusion Cross Sections for the Proton Drip Line Nucleus 17F at Energies Below the Coulomb Barrier

NUCLEAR REACTIONS 208Pb(17F, X), E(cm)=80-92 MeV; 208Pb(19F, X), E(cm)=78-100 MeV; measured fusion-fission σ; deduced no enhancement for lighter projectile. Dynamical model calculations.

doi: 10.1103/PhysRevLett.81.3341
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1998RE24      Nucl.Instrum.Methods Phys.Res. A418, 355 (1998)

K.E.Rehm, C.L.Jiang, M.Paul, D.Blumenthal, L.A.Daniel, C.N.Davids, P.Decrock, S.M.Fischer, D.Henderson, C.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, D.Seweryniak, R.E.Segel

Study of Radiative Capture Reactions with Radioactive Ion Beams

NUCLEAR REACTIONS 1H(18F, 19Ne), E=13.4 MeV; measured σ upper limit. 18F(p, γ), E(cm)=670 keV; deduced σ upper limit. Radioactive beams, inverse kinematics, fragment mass analyzer.

doi: 10.1016/S0168-9002(98)00885-7
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1997RE02      Phys.Rev. C55, R566 (1997)

K.E.Rehm, C.L.Jiang, M.Paul, D.Blumenthal, L.A.Daniel, C.N.Davids, P.Decrock, S.M.Fischer, D.Henderson, C.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, D.Seweryniak, R.E.Segel

Exploring the 18F(p, γ)19Ne Gateway to the Formation of Heavy Elements in Hot Stars

NUCLEAR REACTIONS, ICPND 18F(p, γ)19Ne, E=13.4 MeV; measured σ. 18O(p, γ)19F, E=14.4-18 MeV; measured σ; calculated σ(E); deduced 19Ne production, astrophysical reaction rate for 18F(p, γ)19Ne upper limits. 19Ne level deduced upper limit for Γγ.

doi: 10.1103/PhysRevC.55.R566
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1997RE05      Nucl.Phys. A616, 115c (1997)

K.E.Rehm, M.Paul, A.D.Roberts, C.L.Jiang, D.Blumenthal, C.N.Davids, P.DeCrock, S.M.Fischer, J.Gehring, D.Henderson, C.J.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel

Nuclear Reaction Studies with Radioactive 18F Beams at ATLAS

NUCLEAR REACTIONS, ICPND 1H(18F, α), E(cm) ≈ 5.75-7 MeV; measured σ(E). 1H(18F, γ), E(cm)=0.67 MeV; measured σ; deduced reaction rates ratio, small contribution from (p, γ) route to 19Ne formation.

doi: 10.1016/S0375-9474(97)00080-8
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1997RE17      Nucl.Phys. A621, 191c (1997)

K.E.Rehm, M.Paul, A.D.Roberts, C.L.Jiang, D.Blumenthal, C.N.Davids, P.DeCrock, S.M.Fischer, J.Gehring, D.Henderson, C.J.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel, D.Seweryniak

The Influence of 18F Induced Reactions in the Hot CNO Cycle

NUCLEAR REACTIONS, ICPND 1H(18F, 15O), (18F, 19Ne), E=11.7-15.1 MeV; measured resonance reaction σ vs E; deduced reaction rates features. 19Ne deduced resonance strengths, widths. Astrophysical implications, radioactive beam.

doi: 10.1016/S0375-9474(97)00236-4
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1996RE05      Phys.Rev. C53, 1950 (1996)

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

Astrophysical Reaction Rate for the 18F(p, α)15O Reaction

NUCLEAR REACTIONS, ICPND 18F(p, α), E(cm)=600-800 keV; measured σ(E), resonance yield; calculated reaction rate. 19Ne deduced resonance, J, π, Γp, Γα, Γ.

doi: 10.1103/PhysRevC.53.1950
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1995RE11      Phys.Rev. C52, R460 (1995)

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

Study of the 18F(p, α)15O Reaction at Astrophyical Energies using a 18F Beam

NUCLEAR REACTIONS 18F(p, α), E(cm)=580-760 keV; measured σ(θ) vs E; deduced nuclosynthesis, CNO cycle implications. 19Ne deduced resonance, Γp, Γα, s-wave resonance strength. Gas-filled magnet technique.

doi: 10.1103/PhysRevC.52.R460
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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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1994RE25      Nucl.Instrum.Methods Phys.Res. A344, 614 (1994)

K.E.Rehm, M.Paul, J.Gehring, B.Glagola, D.Henderson, W.Kutschera, A.H.Wuosmaa

Measurements of Heavy-Ion Induced Fusion Cross Sections with the Gas-Filled-Magnet Technique

NUCLEAR REACTIONS 64Ni, 197Au(32S, X), E=157 MeV; 172Yb(64Ni, X), E=219.8 MeV; 100Mo(64Ni, X), E=217.2 MeV; measured elastically scattered, evaporation residue fragment spectra, σ(θ) in some cases; deduced evaporation residue σ. Gas filled magnet technique.

doi: 10.1016/0168-9002(94)90883-4
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1993FR02      Phys.Lett. 302B, 18 (1993)

E.Friedman, M.Paul, M.Schechter, A.Altman, B.K.Jennings, G.J.Wagner, N.Fazel, R.R.Johnson, N.Suen, Z.Fraenkel

Integral Cross Sections for π-p Interaction in the 3, 3 Resonance Region

NUCLEAR REACTIONS 1H(π-, X), E=126-202 MeV; measured total, single charge exchange σ. Model comparison.

doi: 10.1016/0370-2693(93)90629-V
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1993RE11      Phys.Lett. 317B, 31 (1993)

K.E.Rehm, H.Esbensen, J.Gehring, B.Glagola, D.Henderson, W.Kutschera, M.Paul, F.Soramel, A.H.Wuosmaa

Sub-Barrier Fusion Cross Sections in 58,62Ni + 92,100Mo Studied with the Gas-Filled Magnet Technique

NUCLEAR REACTIONS, ICPND 92,100Mo(58Ni, X), (64Ni, X), E(cm) ≈ 130-160 MeV; measured fusion σ(E), σ(evaporation residue, θ). Gas filled magnet technique for product separation. Coupled-channels model.

doi: 10.1016/0370-2693(93)91565-5
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1992ME13      Appl.Radiat.Isot. 43, 1420 (1992)

O.Meirav, M.Adam, E.Boaretto, S.A.Dias, R.R.Johnson, M.Paul, E.Venczel

Measurements of 129I in a Nuclear Power Reactor by Accelerator Mass Spectrometry

doi: 10.1016/0883-2889(92)90020-F
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1991PA10      Z.Phys. A340, 249 (1991)

M.Paul, I.Ahmad, W.Kutschera

Half-Life of 41Ca

RADIOACTIVITY 41Ca; measured T1/2, X-ray spectra, internal bremsstrahlung spectra; deduced recommended T1/2. Si(Li) detector, sample concentration by mass spectrometry, specific activity technique.

doi: 10.1007/BF01294672
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1989KU33      Radiocarbon 31, 311 (1989)

W.Kutschera, I.Ahmad, P.J.Billquist, B.G.Glagola, K.Furer, R.C.Pardo, M.Paul, K.E.Rehm, P.J.Solta, Jr., R.E.Taylor, J.L.Yntema

Studies Towards a Method for Radiocalcium Dating of Bones

RADIOACTIVITY 41Ca(EC); measured X-ray spectra, approximate T1/2.

doi: 10.1017/S0033822200011851
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1987FI11      Nucl.Instrum.Methods Phys.Res. B29, 275 (1987)

D.Fink, M.Paul, G.Hollos, S.Theis, S.Vogt, R.Stueck, P.Englert, R.Michel

Measurements of 41Ca Spallation Cross Sections and 41Ca Concentrations in the Grant Meteorite by Accelerator Mass Spectrometry

NUCLEAR REACTIONS, ICPND Ni, Fe, Ti(p, X)41Ca, E=40-600 MeV; measured residual spallation production σ(E).

doi: 10.1016/0168-583X(87)90249-7
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1986PA17      Phys.Rev. C34, 1980 (1986)

M.Paul, I.Ahmad, W.Kutschera

Search for 34Si Ions in 241Am Decay

RADIOACTIVITY 241Am(SF); measured fission fragment distribution; deduced (fission/α) branching ratio, (34Si/α) branching ratio upper limit. Lexan polycarbonate foils.

doi: 10.1103/PhysRevC.34.1980
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1985KU24      Phys.Rev. C32, 2036 (1985)

W.Kutschera, I.Ahmad, S.G.Armato III, A.M.Friedman, J.E.Gindler, W.Henning, T.Ishii, M.Paul, K.E.Rehm

Spontaneous 14C Emission from 223Ra

RADIOACTIVITY 223Ra(14C), (α) [from 227Th decay]; measured 14C(SF-decay), (14C)/α branching ratio. Enge split-pole magnetic spectrograph.

doi: 10.1103/PhysRevC.32.2036
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1984KU28      Nucl.Instrum.Methods Phys.Res., B5, 430 (1984)

W.Kutschera, P.J.Billquist, D.Frekers, W.Henning, K.J.Jensen, Ma Xiuzeng, R.Pardo, M.Paul, K.E.Rehm, R.K.Smither, J.L.Yntema, L.F.Mausner

Half-Life of 60Fe

RADIOACTIVITY 60Fe(β-) [from Cu(p, X), E=191 MeV]; measured T1/2. Specific activity, radioisotope concentration techniques.

doi: 10.1016/0168-583X(84)90555-X
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1983RE08      Phys.Rev.Lett. 51, 1426 (1983)

K.E.Rehm, D.G.Kovar, W.Kutschera, M.Paul, G.Stephans, J.L.Yntema

Large Cross Sections for Quasielastic Neutron-Pickup Reactions Induced by 37Cl, 48Ti, and 58Ni on 208Pb

NUCLEAR REACTIONS 208Pb(58Ni, 59Ni), (58Ni, 60Ni), (58Ni, X), (37Cl, X), (48Ti, X), E=250, 300, 375 MeV; measured quasielastic yields, σ(fragment A), σ(E(59Ni)), σ(E(60Ni)), σ(θ(59Ni)), σ(θ(60Ni)); deduced σ(reaction), neutron pickup σ contributions. DWBA analysis.

doi: 10.1103/PhysRevLett.51.1426
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1982ER08      Phys.Lett. 119B, 307 (1982)

H.Ernst, W.Henning, C.N.Davids, W.S.Freeman, T.J.Humanic, M.Paul, S.J.Sanders, F.W.Prosser, Jr., R.A.Racca

Prompt Compound Nuclear K X-Rays in Fusion Reactions Induced by a Heavy Projectile

NUCLEAR REACTIONS 116,120,124Sn(32S, X), E=130-202 MeV; measured E(X-ray), I(X-ray), (X-ray)(X-ray)-coin, K X-ray production σ, multiplicities; deduced K X-ray yield role in complete fusion.

doi: 10.1016/0370-2693(82)90676-1
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1982FI14      Nucl.Phys. A389, 18 (1982)

D.Fink, E.Friedman, M.Paul, A.Moalem

Experimental Determination of the Normalization Constant of the (α, t) Reaction

NUCLEAR REACTIONS 48Ca, 92Mo(α, t), E=26-30 MeV; 48Ca, 92Mo(3He, d), E=16 MeV; measured absolute σ(θ). 49Sc, 93Tc level deduced normalizations. Enriched targets.

doi: 10.1016/0375-9474(82)90287-1
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1982PA17      Phys.Rev. C26, 1295 (1982)

M.Paul, I.Labaton, D.Fink, A.Marinov, O.Meirav

Selective Population of States in 36Ar by the 12C(28Si, α)36Ar Reaction

NUCLEAR REACTIONS 12,13C(28Si, α), E=75-102 MeV; measured σ(Eα), σ(θ=0°) vs E. 36Ar deduced levels.

doi: 10.1103/PhysRevC.26.1295
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1981JA10      Phys.Rev. C24, 2070 (1981)

C.M.Jachcinski, D.G.Kovar, R.R.Betts, C.N.Davids, D.F.Geesaman, C.Olmer, M.Paul, S.J.Sanders, J.L.Yntema

Fusion of 24Mg + 24Mg

NUCLEAR REACTIONS 24Mg(24Mg, X), E(cm)=24.7-66.2 MeV; measured σ(fusion, E). Activation technique.

doi: 10.1103/PhysRevC.24.2070
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1981MC02      Nucl.Phys. A358, 411c (1981)

R.D.McKeown, J.P.Schiffer, H.E.Jackson, M.Paul, S.J.Sanders, J.R.Specht, E.J.Stephenson, R.P.Redwine, R.E.Segel, J.Arends, J.Eyink, H.Hartmann, A.Hegerath, B.Mecking, G.Noldeke, H.Rost

Comparison of Pion and Photon Induced Reactions on Complex nuclei

NUCLEAR REACTIONS 12C(π+, p), (π-, p), E=220 MeV; 12C(γ, p), E=343 MeV; analyzed σ(θp, Ep); deduced Δ production mechanism.

doi: 10.1016/0375-9474(81)90354-7
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1981MC09      Phys.Rev. C24, 211 (1981)

R.D.McKeown, S.J.Sanders, J.P.Schiffer, H.E.Jackson, M.Paul, J.R.Specht, E.J.Stephenson, R.P.Redwine, R.E.Segel

Inclusive Reactions of Pions on Nuclei

NUCLEAR REACTIONS 4He, 6Li, 9Be, 12C, 27Al, Ni, 181Ta(π+, p), (π-, p), (π+, π+'), (π-, π-'), E=100, 160, 220 MeV; measured σ(θ, Ep), inclusive pion yields.

doi: 10.1103/PhysRevC.24.211
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