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NSR database version of April 26, 2024.

Search: Author = R.Ledoux

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2011JO11      J.Korean Phys.Soc. 59, 1414s (2011)

M.S.Johnson, J.M.Hall, D.P.McNabb, J.L.McFarland, E.B.Norman, W.Bertozzi, S.E.Korbly, R.J.Ledoux, W.H.Park

Applications of Photonuclear Physics for International Safeguards and Security

NUCLEAR REACTIONS ²³⁹Pu(γ, γ'), E=0-5.5 MeV[from HIGS (High-Intensity Gamma-ray Source) using bremsstrahlung spectra with endpoint energy 4.0-5.5 MeV]; measured thick target Eγ, Iγ using HPGe. ²³⁹Pu deduced prompt γ transitions.²⁷Al, ⁵⁵Mn, ⁵⁶Fe(γ, γ'), E=0-5.5 MeV;¹H, ¹⁴N, ³⁵Cl, ^52,53Cr(n, γ), E=background;⁵⁵Mn, ⁵⁶Fe(n, n'γ), E=background; measured Eγ, Iγ. ²⁸Al, ⁵⁶Fe deduced β-delayed γ transitions (NRF - Nuclear Resonance Fluorescence) peaks.

doi: 10.3938/jkps.59.1414
Citations: PlumX Metrics

2008BE31      Phys.Rev. C 78, 041601 (2008)

W.Bertozzi, J.A.Caggiano, W.K.Hensley, M.S.Johnson, S.E.Korbly, R.J.Ledoux, D.P.McNabb, E.B.Norman, W.H.Park, G.A.Warren

Nuclear resonance fluorescence excitations near 2 MeV in ²³⁵U and ²³⁹Pu

NUCLEAR REACTIONS ²³⁵U(γ, γ'), E=2.2 MeV;²³⁹Pu(γ, γ), E=2.8 MeV; measured Eγ, Iγ, σ; deduced level energies, dipole excitations.

doi: 10.1103/PhysRevC.78.041601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0139. Data from this article have been entered in the XUNDL database. For more information, click here.

1997AH03      Phys.Rev. C55, 2604 (1997)

L.Ahle, Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.LeVine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, K.Shigaki, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, S.Ueno, J.H.van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, H.E.Wegner, D.S.Woodruff, Y.D.Wu, K.Yagi, X.Yang, D.Zachary, W.A.Zajc, and the E802 Collaboration

Baryon Emission at Target Rapidities in Si + Al, Cu, Au Collisions at 14.6A GeV/c and Au + Au Collisions at 11.7A GeV/c

NUCLEAR REACTIONS ²⁷Al, Cu, ¹⁹⁷Au(²⁸Si, X), E at 14.6 GeV/c/nucleon; ¹⁹⁷Au(¹⁹⁷Au, X), E at 11.7 GeV/c/nucleon; measured light charged particle momentum density distribution; deduced proton distributions at minimum bias target rapidities, pseudorapidity distributions shapes. Model comparison.

doi: 10.1103/PhysRevC.55.2604
Citations: PlumX Metrics

1997AK04      Phys.Rev. C56, 1544 (1997)

Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.K.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, J.H.Van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, D.S.Woodruff, Y.D.Wu, X.Yang, D.Zachary, W.A.Zajc

Two-Particle Rapidity Correlations from the Bose-Einstein Effect in Central ²⁸Si + Au Collisions at 14.6A GeV/c and Intermittency

NUCLEAR REACTIONS ¹⁹⁷Au(²⁸Si, X), E at 14.6 GeV/c/nucleon; measured two-pion correlation functions vs Q(inv), rapidity, pseudorapidity; deduced correlation length, Bose-Einstein effect role.

doi: 10.1103/PhysRevC.56.1544
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1996AK04      Phys.Rev.Lett. 76, 2021 (1996)

Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.K.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, J.H.Van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, D.S.Woodruff, Y.D.Wu, X.Yang, D.Zachary, W.A.Zajc, and the E-802 Collaboration

Production of φ Mesons in Central ²⁸Si + ¹⁹⁷Au Collisions at 14.6A GeV/c

NUCLEAR REACTIONS ¹⁹⁷Au(²⁸Si, X), E at 14.6 GeV/c/nucleon; measured invariant φ yield; deduced invariant transverse mass distribution width.

doi: 10.1103/PhysRevLett.76.2021
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1995AB18      Phys.Rev. C52, 2663 (1995)

T.Abbott, Y.Akiba, D.Alburger, D.Beavis, P.Beery, M.A.Bloomer, P.D.Bond, C.Chasman, Z.Chen, Y.Y.Chu, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, E.Duek, J.Engelage, S.Y.Fung, L.Grodzins, S.Gushue, H.Hamagaki, O.Hansen, P.Haustein, S.Homma, H.Z.Huang, Y.Ikeda, J.Kang, S.Katcoff, S.Kaufman, R.J.Ledoux, M.J.Levine, P.J.Lindstrom, Y.Miake, R.J.Morse, S.Nagamiya, J.Olness, C.G.Parsons, L.P.Remsberg, H.Sakurai, M.Sarabura, R.Seto, S.G.Steadman, G.S.F.Stephans, T.Sugitate, M.Tanaka, M.J.Tannenbaum, M.Torikoshi, J.H.van Dijk, F.Videbaek, M.Vient, P.Vincent, E.Vulgaris, V.Vutsadakis, W.A.Watson III, H.E.Wegner, D.S.Woodruff, W.A.Zajc, and the E-802 Collaboration

Multiplicity Distributions from Central Collisions of ¹⁶O + Cu at 14.6A GeV/c and Intermittency

NUCLEAR REACTIONS Cu(¹⁶O, X), E=14.6 GeV/c/nucleon; measured central relativistic collisions associated multiplicity distributions. Negative binomial distributions analysis.

doi: 10.1103/PhysRevC.52.2663
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1993AB04      Phys.Rev. C47, R1351 (1993)

T.Abbott, Y.Akiba, D.Beavis, M.A.Bloomer, P.D.Bond, C.Chasman, Z.Chen, Y.Y.Chu, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.-Y.Fung, S.Gushue, H.Hamagaki, O.Hansen, R.Hayano, S.Hayashi, S.Homma, H.Z.Huang, Y.Ikeda, I.Juricic, J.Kang, S.Katcoff, S.Kaufman, K.Kimura, K.Kitamura, K.Kurita, R.J.Ledoux, M.J.Le Vine, Y.Miake, R.J.Morse, B.Moskowitz, S.Nagamiya, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, H.Sakurai, M.Sarabura, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sugitate, M.J.Tannenbaum, J.H.Van Dijk, F.Videbaek, M.Vient, P.Vincent, V.Vutsadakis, H.E.Wegner, D.S.Woodruff, Y.D.Wu, W.A.Zajc, and the E-802 Collaboration

Antiproton Production in p + A Collisions at 14.6 GeV/c

NUCLEAR REACTIONS ⁹Be, ²⁷Al, Cu(p, p-bar), E at 14.6 GeV/c; measured p-bar production σ, multiplicity.

doi: 10.1103/PhysRevC.47.R1351
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1992AB07      Phys.Rev. D45, 3906 (1992)

T.Abbott, Y.Akiba, D.Beavis, M.A.Bloomer, P.D.Bond, C.Chasman, Z.Chen, Y.Y.Chu, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Z.Huang, Y.Ikeda, I.Juricic, J.Kang, S.Katcoff, S.Kaufman, K.Kimura, K.Kitamura, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, R.J.Morse, B.Moskowitz, S.Nagamiya, J.Olness, C.G.Parsons, L.P.Remsberg, H.Sakurai, M.Sarabura, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sugitate, M.J.Tannenbaum, J.H.van Dijk, F.Videbaek, M.Vient, P.Vincent, V.Vutsadakis, H.E.Wegner, D.S.Woodruff, Y.D.Wu, W.Zajc, and the E-802 Collaboration

Measurement of Particle Production in Proton-Induced Reactions at 14.6 GeV/c

NUCLEAR REACTIONS ⁹Be, ²⁷Al, Cu, ¹⁹⁷Au(p, xp), (p, xπ⁺), (p, xπ^-), (p, xK⁺), (p, xK^-), (p, xp), E at 14.6 GeV/c; measured invariant particle production σ; deduced particle production mechanism.

doi: 10.1103/PhysRevD.45.3906
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1986OR01      Phys.Lett. 173B, 39 (1986)

C.E.Ordonez, R.J.Ledoux, E.R.Cosman

Rotational Band of ¹²C + ¹²C Gross-Structure Resonances and Its Representation by a Double-Minimum Optical Potential

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, ¹²C), E(cm)=5.5-33 MeV; analyzed reaction σ(E). ²⁴Mg deduced shape isomeric doorway states. Double minimum optical potential.

doi: 10.1016/0370-2693(86)91226-8
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1986VU01      Phys.Rev. C33, 2017 (1986); Erratum Phys.Rev. C34, 1495 (1986)

E.Vulgaris, L.Grodzins, S.G.Steadman, R.Ledoux

Fusion, Transfer, and Elastic Scattering at Sub-Barrier Energies for ^16,18O Ions on ²⁰⁸Pb and ¹⁵N and ¹⁶O Ions on ²⁰⁹Bi

NUCLEAR REACTIONS, ICPND ²⁰⁹Bi, ²⁰⁸Pb(¹⁶O, X), (¹⁶O, F), (¹⁶O, ¹⁶O), ²⁰⁸Pb(¹⁸O, X), (¹⁸O, F), (¹⁸O, ¹⁸O), E(cm)=70-98 MeV; ²⁰⁹Bi(¹⁵N, X), E(cm) ≈ 64-90 MeV; measured fusion, evaporation residue σ(E), fission fragment, elastic σ(θ); deduced parameters.

doi: 10.1103/PhysRevC.33.2017
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1984AL25      Phys.Rev. C30, 1223 (1984)

H.A.Aljuwair, R.J.Ledoux, M.Beckerman, S.B.Gazes, J.Wiggins, E.R.Cosman, R.R.Betts, S.Saini, O.Hansen

Isotopic Effects in the Fusion of ⁴⁰Ca with ^40,44,48Ca

NUCLEAR REACTIONS, ICPND ^44,48,40Ca(⁴⁰Ca, X), E=90-135 MeV; measured fusion σ(E). Velocity filter.

doi: 10.1103/PhysRevC.30.1223
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1984LE19      Phys.Rev. C30, 866 (1984)

R.J.Ledoux, C.E.Ordonez, M.J.Bechara, H.A.Al-Juwair, G.Lavelle, E.R.Cosman

Selective Alpha Particle Decay of ¹²C + ¹²C Resonances to Excited ²⁰Ne Rotational Bands Observed in the ¹²C(¹²C, α)²⁰Ne Reaction

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, α), E(cm)=14-20.6 MeV; measured σ(Eα), σ(θ) vs E, yield vs E. ²⁴Mg deduced resonances, J, π, Γα, reduced widths, possible isomeric resonance selective decay to ²⁰Ne rotational band.

doi: 10.1103/PhysRevC.30.866
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1983BE09      Phys.Rev. C27, 1540 (1983)

M.J.Bechara, A.J.Lazzarini, R.J.Ledoux, E.R.Cosman

¹²C(¹⁶O, α)²⁴Mg Reaction in the Energy Region E(c.m.) = 26.6 to 42.9 MeV

NUCLEAR REACTIONS ¹²C(¹⁶O, α), E=62-100 MeV; measured σ(θ), σ(Eα), σ(θ, E). ²⁴Mg deduced levels. ²⁸Si deduced intermediate resonances, Γ, nonstatistical character.

doi: 10.1103/PhysRevC.27.1540
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1983DI06      Phys.Lett. 127B, 172 (1983)

F.A.Dilmanian, L.Grodzins, J.W.Ball, M.Beckerman, R.Boisseau, S.Gazes, R.Ledoux, A.Sperduto

Angular Momentum Partition as a Function of the Mass Asymmetry in Heavy-Ion Induced Fision

NUCLEAR REACTIONS ¹⁰⁷Ag(³⁷Cl, F), ¹¹²Cd(³²S, F), E=150-210 MeV; measured fission fragment energy, mass distributions, γ(θ), γ-multiplicity; deduced fragment mass asymmetry, fission fragment spin, compound nuclear angular momentum relationships.

doi: 10.1016/0370-2693(83)90870-5
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1983LA07      Phys.Rev. C27, 1550 (1983)

A.J.Lazzarini, S.G.Steadman, R.J.Ledoux, A.Sperduto, G.R.Young, K.Van Bibber, E.R.Cosman

Structure in the ¹²C + ¹²C and ⁸Be + ¹⁶O Fission Width Distribution of ²⁴Mg Observed via the Reaction ¹²C(¹⁶O, α)²⁴Mg → X + Y

NUCLEAR REACTIONS, ICPND ¹²C(¹⁶O, α), E=77 MeV; measured σ(Eα), (α)(¹²C)(¹²C)-, (α)(⁸Be)(¹⁶O)-coin, summed three-body yields. ²⁴Mg deduced resonances, Γ(¹²C)/Γ, three-body breakup characteristics. Cross correlation analysis.

doi: 10.1103/PhysRevC.27.1550
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1983LE05      Phys.Rev. C27, 1103 (1983)

R.J.Ledoux, M.J.Bechara, C.E.Ordonez, H.A.Al-Juwair, E.R.Cosman

¹²C + ¹²C Elastic Scattering Excitation Functions and Phase Shift Analysis

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, ¹²C), E(cm)=14.6-31.3 MeV; measured σ(θ) vs E; deduced reaction σ. ²⁴Mg deduced intermediate resonances, J, π. Phase shift analysis.

doi: 10.1103/PhysRevC.27.1103
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1982KA08      Phys.Rev. C25, 1838 (1982)

J.S.Karp, S.G.Steadman, S.B.Gazes, R.Ledoux, F.Videbaek

Statistical Behavior of Nucleon Transfer to Highly Excited States in Heavy-Ion Collisions

NUCLEAR REACTIONS, ICPND ²³²Th(¹⁶O, X)¹⁰Be/¹¹B/¹²C/¹³C/¹⁴C/¹⁵N, E=97, 105, 115, 125 MeV; deduced total σ, reaction σ. ¹⁸¹Ta, ²³²Th(¹⁵N, X), E=86, 95, 103 MeV; ¹⁸¹Ta(³⁵Cl, X), E=205 MeV; measured σ(fragment θ, E) for X=^9,10,11Be, ^11,12,13B, ^{12,13,14,15,16}C, ^15,16,17N, ^16,17,18,19O, ^30,31,32Si, ^31,32,33,34P, ^33,34,35,36S, ^36,37Cl; deduced reaction mechanism, dependence on transferred nucleon number, (Q)-dependence. Surprisal analysis.

doi: 10.1103/PhysRevC.25.1838
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1982LE09      Phys.Rev. C25, 2844 (1982)

S.Y.Lee, H.W.Wilschut, R.Ledoux

Intermediate Structure of ¹²C + ¹²C System

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, ¹²C), E=15.2-22.5 MeV; calculated σ(θ); ¹²C(¹²C, ¹²C'), E(cm)=15-21 MeV; calculated total σ vs E. ²⁴Mg deduced intermediate structure resonances, J, π. Phase shift analysis.

doi: 10.1103/PhysRevC.25.2844
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1980CO03      Phys.Rev. C21, 2111 (1980)

E.R.Cosman, R.Ledoux, A.J.Lazzarini

¹²C + ¹²C Intermediate Structures Correlated among Elastic and Reaction Channels

NUCLEAR REACTIONS ¹²C(¹²C, α), E(cm)=5-35 MeV; ¹²C(¹²C, p), ¹²C(¹²C, ¹²C'), E(cm)=16-23 MeV; ¹²C(¹²C, ¹²C), E=11-27 MeV; analyzed σ(E). ²⁴Mg deduced intermediate structure resonances, Γ, Γα, Γ(¹²C) strength function, J, π. Cross correlation, Breit-Wigner analysis.

doi: 10.1103/PhysRevC.21.2111
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1979LI14      Phys.Rev. C20, 605 (1979)

C.J.Lister, G.R.Young, D.Cline, J.Srebrny, D.Elmore, P.A.Butler, R.Ledoux, R.Fridieu

High Spin States and Isomers in ¹⁵¹Dy

NUCLEAR REACTIONS ¹²²Sn(³²S, 3n), E=115-165 MeV; ¹⁴¹Pr(¹⁴N, 4n), E=60-101 MeV; measured σ(E), Iγ(θ), γγ-coin. ¹⁵¹Dy deduced levels, branching ratios, J, T_1/2, multipolarity, B(E2). Enriched targets, Ge(Li) detectors. Spherical, oblate spheroidal model calculations.

doi: 10.1103/PhysRevC.20.605
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1977VA02      Phys.Rev.Lett. 38, 334 (1977)

K.Van Bibber, R.Ledoux, S.G.Steadman, F.Videbaek, G.Young, C.Flaum

Fragment Spin Orientation Following Deep-Inelastic Scattering

NUCLEAR REACTIONS ²⁷Al(¹⁶O, X), E=100 MeV; measured σ(Eγ, Z).

doi: 10.1103/PhysRevLett.38.334
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Note: The following list of authors and aliases matches the search parameter R.Ledoux: , R.J.LEDOUX