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NSR database version of April 25, 2024.

Search: Author = R.Bimbot

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2004FA04      Eur.Phys.J. A 19, 105 (2004)

G.Fares, R.Bimbot, S.Hachem, M.Mirea, R.Anne, T.Benfoughal, C.Cabot, F.Clapier, P.Delbourgo-Salvador, T.Ethvignot, A.Lefebvre, M.Lewitowicz, P.Roussel-Chomaz, M.G.Saint-Laurent, J.E.Sauvestre, J.L.Sida, Y.Y.Feng

Fragmentation of 95 MeV/u ¹²C and 75 MeV/u ¹³C. Application to secondary-beam production

NUCLEAR REACTIONS ⁹Be, Cu, ¹⁹⁷Au(¹²C, X), E=95 MeV/nucleon; ⁹Be, Ni, ¹⁸¹Ta(¹³C, X), E=75 MeV/nucleon; measured fragments isotopic σ(E, θ=0°), momentum distributions. Application go exotic beam production discussed.

doi: 10.1140/epja/i2002-10247-9
Citations: PlumX Metrics

2002GO22      Phys.Rev. C66, 014609 (2002); Erratum Phys.Rev. C66, 039901 (2002)

A.N.Golovchenko, J.Skvarc, N.Yasuda, M.Giacomelli, S.P.Tretyakova, R.Ilic, R.Bimbot, M.Toulemonde, T.Murakami

Total Charge-Changing and Partial Cross-Section Measurements in the Reactions of ∼ 110-250 MeV/nucleon ¹²C in Carbon, Paraffin, and Water

NUCLEAR REACTIONS H, C, O(¹²C, X), E ≈ 110-250 MeV/nucleon; measured total and partial charge-changing σ. Etched track detector, comparison with model predictions.

doi: 10.1103/PhysRevC.66.014609
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1044.

1999GO32      Nucl.Instrum.Methods Phys.Res. B159, 233 (1999)

A.N.Golovchenko, J.Skvarc, R.Ilic, L.Sihver, V.P.Bamblevski, S.P.Tretyakova, D.Schardt, R.K.Tripathi, J.W.Wilson, R.Bimbot

Fragmentation of 200 and 244 MeV/u Carbon Beams in Thick Tissue-Like Absorbers

NUCLEAR REACTIONS H, C, O(¹²C, X), E=200, 244 MeV/nucleon; measured fragments charge distributions in thick targets; deduced charge removal σ. Lucite, water targets, CR-39 track detectors.

doi: 10.1016/S0168-583X(99)00546-7
Citations: PlumX Metrics

1995AN20      Z.Phys. A352, 397 (1995)

R.Anne, D.Bazin, R.Bimbot, M.J.G.Borge, J.M.Corre, S.Dogny, H.Emling, D.Guillemaud-Mueller, P.G.Hansen, P.Hornshoj, P.Jensen, B.Jonson, M.Lewitowicz, A.C.Mueller, R.Neugart, T.Nilsson, G.Nyman, F.Pougheon, M.G.Saint-Laurent, G.Schrieder, O.Sorlin, O.Tengblad, K.Wilhelmsen-Rolander

Projectile Coulomb Excitation with Fast Radioactive Beams

NUCLEAR REACTIONS Pb(⁸He, ⁸He'), (¹¹Be, ¹¹Be'), (¹²Be, ¹²Be'), (¹⁴Be, ¹⁴Be'), E=30-46 MeV/nucleon; measured Eγ, Iγ following projectile Coulomb excitation. ¹¹Be level deduced γ-transition associated σ.

doi: 10.1007/BF01299757
Citations: PlumX Metrics

1995BI25      Appl.Radiat.Isot. 46, 537 (1995)

R.Bimbot

Nuclear Physics with Radioactive Beams

NUCLEAR REACTIONS ⁹Be(¹²⁴Xe, X), E=1095 MeV/nucleon; Ni(¹¹²Sn, X), E=63 MeV/nucleon; compiled, reviewed these, other radioactive beams induced reactions.

doi: 10.1016/0969-8043(95)00081-X
Citations: PlumX Metrics

1995DO19      Nucl.Phys. A593, 503 (1995)

C.Donzaud, L.Tassan-Got, C.Stephan, D.Bachelier, C.O.Bacri, R.Bimbot, B.Borderie, J.L.Boyard, F.Clapier, T.Hennino, M.F.Rivet, P.Roussel, D.Bazin, C.Grunberg, D.Disdier, B.Lott, C.Volant

Dissipative Aspects in 200 MeV/u Kr-Induced Reactions

NUCLEAR REACTIONS ¹⁹⁷Au, ⁵⁹Co(⁸⁴Kr, X), E=200 MeV/nucleon; measured projectile-like fragment isotopic distribution, momentum, pp-coin rates, excitation energy distribution, neutron-rich nucleus production. Intranuclear-cascade, statistical abrasion, Goldhaber's models analysis.

doi: 10.1016/0375-9474(95)00322-R
Citations: PlumX Metrics

1995TA04      Nucl.Phys. A583, 453c (1995)

L.Tassan-Got, D.Bachelier, C.O.Bacri, R.Bimbot, B.Borderie, J.L.Boyard, F.Clapier, C.Donzaud, T.Hennino, M.F.Rivet, P.Roussel, C.Stephan, D.Bazin, C.Grunberg, D.Disdier, B.Lott, C.Volant

Dissipative Aspects in Projectile Fragmentation at 200 MeV/u

NUCLEAR REACTIONS ⁵⁹Co(⁸⁴Kr, X), E=200 MeV/nucleon; measured projectile-like fragment mass, charge, momentum distributions, nucleon, other particle emission multiplicities. Intranuclear cascade model analysis.

doi: 10.1016/0375-9474(94)00703-P
Citations: PlumX Metrics

1994AN12      Nucl.Phys. A575, 125 (1994)

R.Anne, R.Bimbot, S.Dogny, H.Emling, D.Guillemaud-Mueller, P.G.Hansen, P.Hornshoj, F.Humbert, B.Jonson, M.Keim, M.Lewitowicz, P.Moller, A.C.Mueller, R.Neugart, T.Nilsson, G.Nyman, F.Pougheon, K.Riisager, M.-G.Saint-Laurent, G.Schrieder, O.Sorlin, O.Tengblad, K.Wilhelmsen Rolander

Exclusive and Restricted-Inclusive Reactions Involving the ¹¹Be One-Neutron Halo

NUCLEAR REACTIONS ⁹Be, Ti, ¹⁹⁷Au(¹¹Be, X), E=41 MeV/nucleon; measured inclusive, exclusive σ(θn) up to 97°; double-differential σ(θ, En) near 0°, integral σ(¹⁰Be) following projectile breakup. Analysis in terms of Coulomb, Serber and diffractive mechanisms.

doi: 10.1016/0375-9474(94)90142-2
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1994KE06      Z.Phys. A348, 61 (1994)

H.Keller, R.Anne, D.Bazin, R.Bimbot, M.J.G.Borge, J.M.Corre, S.Dogny, H.Emling, D.Guillemaud-Mueller, P.G.Hansen, P.Hornshoj, F.Humbert, P.Jensen, B.Jonson, M.Lewitowicz, A.C.Mueller, R.Neugart, T.Nilsson, G.Nyman, F.Pougheon, M.G.Saint-Laurent, G.Schrieder, O.Sorlin, O.Tengblad, K.Wilhelmsen Rolander

Search for Forbidden β-Decay of the Drip Line Nucleus ¹²Be

RADIOACTIVITY ¹²Be(β^-) [from ⁹Be(¹⁸O, X), E=63 MeV/nucleon]; measured βγ-coin, T_1/2; deduced ft. ¹²B levels deduced β-branching ratio.

doi: 10.1007/BF01291655
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1994UZ01      Phys.Lett. 331B, 280 (1994)

J.L.Uzureau, P.Delbourgo-Salvador, T.Ethvignot, J.E.Sauvestre, J.Trochon, B.Bonnereau, M.Szmigiel, R.Anne, D.Bazin, J.M.Corre, M.Lewitowicz, M.G.St Laurent, R.Bimbot, H.Keller, A.C.Mueller, O.Sorlin

Production of Pure ^42mSc Isomeric Beam

NUCLEAR REACTIONS ¹²C(⁴⁰Ca, ¹⁰B)⁴²Sc/^42mSc, E=30 MeV/nucleon; measured γ spectra following ^42mSc decay; deduced residual (as secondary beam) intensity.

RADIOACTIVITY ^42mSc(β⁺) [from ¹²C(⁴⁰Ca, ¹⁰B), E=30 MeV/nucleon]; measured Eγ, Iγ. Source as secondary beam.

doi: 10.1016/0370-2693(94)91052-9
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1993AN05      Phys.Lett. 304B, 55 (1993)

R.Anne, S.E.Arnell, R.Bimbot, S.Dogny, H.Emling, H.Esbensen, D.Guillemaud-Mueller, P.G.Hansen, P.Hornshoj, F.Humbert, B.Jonson, M.Keim, M.Lewitowicz, P.Moller, A.C.Mueller, R.Neugart, T.Nilsson, G.Nyman, F.Pougheon, K.Riisager, M.-G.Saint-Laurent, G.Schrieder, O.Sorlin, O.Tengblad, K.Wilhelmsen Rolander, D.Wolski

Dissociation Reactions of the ¹¹Be One-Neutron Halo. The Interplay between Structure and Reaction Mechanism

NUCLEAR REACTIONS ¹⁹⁷Au, Ti, ⁹Be(¹¹Be, X), E=41 MeV/nucleon; measured exclusive, inclusive σ(θ); deduced structure, reaction mechanism interplay.

doi: 10.1016/0370-2693(93)91399-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1327.

1993AN13      Bull.Rus.Acad.Sci.Phys. 57, 118 (1993)

R.Anne, K.Borcha, R.Bimbot, V.Borrel, D.Giimo-Muller, F.A.Gareev, Z.Dlougy, S.Dogny, S.N.Ershov, G.S.Kazacha, A.Kordyasz, M.Levitovich, S.M.Lukyanov, A.S.Mueller, Yu.E.Penionzhkevich, F.Puzho, M.-G.Sen-Loran, N.K.Skobelev, S.P.Tretiakova, Ya.Shvanda

Elastic Scattering of ¹¹Li Ions with an Energy of 29 MeV per Nucleon on ²⁸Si Nuclei

NUCLEAR REACTIONS ²⁸Si(¹¹Li, ¹¹Li), E=29 MeV/nucleon; measured σ(θ). ²⁸Si(⁷Li, ⁷Li), E=177.8 MeV; analyzed σ(θ); deduced model parameters, projectile neutron halo effects role. Optical model, Wood-Saxon potential.

1993KI06      Nucl.Phys. A552, 66 (1993)

J.Kiener, A.Lefebvre, P.Aguer, C.O.Bacri, R.Bimbot, G.Bogaert, B.Borderie, F.Clapier, A.Coc, D.Disdier, S.Fortier, C.Grunberg, L.Kraus, I.Linck, G.Pasquier, M.F.Rivet, F.St.Laurent, C.Stephan, L.Tassan-Got, J.P.Thibaud

Determination of the ¹³N(p, γ)¹⁴O Reaction Rate Through the Coulomb Break-Up of a ¹⁴O Radioactive Beam

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁴O, p¹³N), E=70 MeV/nucleon; measured projectile-breakup reaction σ. ¹⁴O level deduced radiative width. Astrophysical ¹³N(p, γ) reaction rate discussed.

doi: 10.1016/0375-9474(93)90331-Q
Citations: PlumX Metrics

1993LE14      Nucl.Phys. A562, 301 (1993)

M.Lewitowicz, C.Borcea, F.Carstoiu, M.G.Saint-Laurent, A.Kordyasz, R.Anne, P.Roussel-Chomaz, R.Bimbot, V.Borrel, S.Dogny, D.Guillemaud-Mueller, A.C.Mueller, F.Pougheon, F.A.Gareev, S.N.Ershov, S.Lukyanov, Yu.Penionzhkevich, N.Skobelev, S.Tretyakova, Z.Dlouhy, L.Nosek, J.Svanda

Elastic Scattering of a Secondary ¹¹Li Beam on ²⁸Si at 29 MeV/Nucleon

NUCLEAR REACTIONS ²⁸Si(⁷Li, ⁷Li), E=177.8 MeV; ²⁸Si(¹¹Li, ¹¹Li), E=319 MeV; measured σ(θ); deduced reaction mechanism. ¹¹Li deduced neutron halo role. Optical model, phenomenological potential, coupled-channel model, double-folding potential, DDM3Y interaction.

doi: 10.1016/0375-9474(93)90201-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1879.

1992RI01      Nucl.Phys. A540, 365 (1992)

K.Riisager, R.Anne, S.E.Arnell, R.Bimbot, H.Emling, D.Guillemaud-Mueller, P.G.Hansen, L.Johannsen, B.Jonson, A.Latimier, M.Lewitowicz, S.Mattsson, A.C.Mueller, R.Neugart, G.Nyman, F.Pougheon, A.Richard, A.Richter, M.G.Saint-Laurent, G.Schrieder, O.Sorlin, K.Wilhelmsen

Two-Neutron Removal Reactions for Very Neutron-Rich Nuclei

NUCLEAR REACTIONS ⁹Be, Ni, ¹⁹⁷Au(¹¹Li, ⁹Li), (¹⁴Be, ¹²Be), (⁸He, ⁶He), E=30 MeV/nucleon; measured σ(θ); deduced correlation with two-neutron separation energies, nn-distribution.

doi: 10.1016/0375-9474(92)90210-B
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1645.

1991AS01      Phys.Rev. C43, 456 (1991)

K.Asahi, M.Ishihara, T.Ichihara, M.Fukuda, T.Kubo, Y.Gono, A.C.Mueller, R.Anne, D.Bazin, D.Guillemaud-Mueller, R.Bimbot, W.D.Schmidt-Ott, J.Kasagi

Observation of Spin-Aligned Secondary Fragment Beams of ¹⁴B

NUCLEAR REACTIONS ⁹Be(¹⁸O, X), E=60 MeV/nucleon; measured ¹⁴B production yield, spin alignment. Doubly achromatic spectrometer, secondary beams.

doi: 10.1103/PhysRevC.43.456
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1990AN28      Phys.Lett. 250B, 19 (1990)

R.Anne, S.E.Arnell, R.Bimbot, H.Emling, D.Guillemaud-Mueller, P.G.Hansen, L.Johannsen, B.Jonson, M.Lewitowicz, S.Mattsson, A.C.Mueller, R.Neugart, G.Nyman, F.Pougheon, A.Richter, K.Riisager, M.G.Saint-Laurent, G.Schrieder, O.Sorlin, K.Wilhelmsen

Observation of Forward Neutrons from the Break-Up of the ¹¹Li Neutron Halo

NUCLEAR REACTIONS ⁹Be, Ni, ¹⁹⁷Au(¹¹Li, ⁹Li), E=29 MeV/nucleon; measured σ(θ) following projectile breakup; deduced neutron halo radius.

doi: 10.1016/0370-2693(90)91147-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1646.

1990LI39      Europhys.Lett. 13, 401 (1990)

E.Liatard, J.F.Bruandet, F.Glasser, S.Kox, T.U.Chan, G.J.Costa, C.Heitz, Y.El Masri, F.Hanappe, R.Bimbot, D.Guillemaud-Mueller, A.C.Mueller

Matter Distribution in Neutron-Rich Light Nuclei and Total Reaction Cross-Section

NUCLEAR STRUCTURE ^6,7,8,9,11Li, ^{9,10,11,12,14}Be, ^{10,11,12,13,14,15,17}B; analyzed data; deduced rms radii.

doi: 10.1209/0295-5075/13/5/004
Citations: PlumX Metrics

1989SA10      Z.Phys. A332, 457 (1989)

M.G.Saint-Laurent, R.Anne, D.Bazin, D.Guillemaud-Mueller, U.Jahnke, Jin Gen-Ming, A.C.Mueller, J.F.Bruandet, F.Glasser, S.Kox, E.Liatard, Tsan Ung Chan, G.J.Costa, C.Heitz, Y.El-Masri, F.Hanappe, R.Bimbot, E.Arnold, R.Neugart

Total Cross Sections of Reactions Induced by Neutron-Rich Light Nuclei

NUCLEAR REACTIONS Cu(X, X), E not given; measured reaction σ for projectile X=^4,6He, ^6,7,8,9,11Li, ^{7,9,10,11,12,14}Be, ^{10,11,12,13,14,15,17}B, ^{11,12,13,14,15,16,17,18,19}C, ^{13,14,15,16,17,18,19}N, ^{15,16,17,18,19,20,21}O, ^18,19,20,21F, ^20,21Ne. Secondary beams, 4π γ method.

1985JA14      Nucl.Phys. A445, 140 (1985)

D.Jacquet, J.Galin, M.F.Rivet, R.Bimbot, B.Borderie, D.Gardes, B.Gatty, D.Guerreau, L.Kowalski, M.Lefort, X.Tarrago

Fission following Carbon Interactions on Gold and Uranium between 30 and 84 MeV/u

NUCLEAR REACTIONS ¹⁹⁷Au, ²³⁸U(¹²C, F), E=30, 60, 84 MeV/nucleon; measured binary fission fragment mass spectra; deduced fusion mechanism. ²⁰⁹At, ²⁵⁰Cf deduced excitation energy.

doi: 10.1016/0375-9474(85)90365-3
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1984BI02      Nucl.Phys. A413, 489 (1984)

R.Bimbot, D.Gardes, L.De Reilhac, M.F.Rivet, A.Fleury, F.Hubert, Y.Llabador

Influence of the Potential Energy Surface on the Cross Sections for Deeply Inelastic Transfer Reactions Induced by Heavy Ions

NUCLEAR REACTIONS, ICPND ¹⁴⁸Sm(⁴⁰Ca, X), E=193, 211, 236, 266 MeV; ^144,150Sm, ^142,144,146Nd(⁴⁰Ca, X), E=211, 236 MeV; ¹⁵⁴Sm(⁴⁰Ca, X), E=236 MeV; ¹⁴⁴Sm(⁴⁰Ar, X), E=211, 245 MeV; measured production σ for ^151,150Dy, ¹⁴⁹Tb; deduced transfer reaction potential energy surface dependence, reaction mechanism.

doi: 10.1016/0375-9474(84)90423-8
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1983BO14      Nucl.Phys. A402, 57 (1983)

B.Borderie, M.F.Rivet, I.Forest, J.Galin, D.Guerreau, R.Bimbot, D.Gardes, B.Gatty, M.Lefort, H.Oeschler, S.Song, B.Tamain, X.Tarrago

Emission of Light Charged Particles and Associated Heavy Partners in Reactions Induced on Ni by C Projectiles at 30, 60 and 84 MeV/u

NUCLEAR REACTIONS Ni(¹²C, pX), (¹²C, dX), (¹²C, tX), (¹²C, ³HeX), (¹²C, αX), E=30, 60, 84 MeV/nucleon; measured(fragment)(fragment)-coin, σ(Ep), σ(Ed), σ(Et), σ(E³He), σ(α); deduced reaction mechanism.

doi: 10.1016/0375-9474(83)90562-6
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1983SO07      Phys.Lett. 130B, 14 (1983)

S.Song, M.F.Rivet, R.Bimbot, B.Borderie, I.Forest, J.Galin, D.Gardes, B.Gatty, M.Lefort, H.Oeschler, B.Tamain, X.Tarrago

Evidence for the Formation of Highly Excited Compound-Like Nuclei (T≈5 MeV) in Collisions of 720 MeV C Projectiles with ²³⁸U, ²³²Th and ¹⁹⁷Au Targets

NUCLEAR REACTIONS ²³²Th(¹²C, pF), (¹²C, αF), E=720 MeV; measured fission fragment(p)-, (fragment)(α)-coin. ¹⁹⁷Au, ²³⁸U(¹²C, F), E=720 MeV; measured fission (fragment)(fragment)(light particle)-coin; deduced reaction mechanism.

doi: 10.1016/0370-2693(83)91053-5
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1982GA15      Phys.Rev.Lett. 48, 1787 (1982)

J.Galin, H.Oeschler, S.Song, B.Borderie, M.F.Rivet, I.Forest, R.Bimbot, D.Gardes, B.Gatty, H.Guillemot, M.Lefort, B.Tamain, X.Tarrago

Evidence for a Limitation of the Linear Momentum Transfer in ¹²C-Induced Reactions between 30 and 84 MeV/u

NUCLEAR REACTIONS, Fission U, Au, Ni(¹²C, F), E=30-84 MeV/nucleon; measured σ(θ₁, θ₂) for fragment pair; deduced linear momentum transfer limitation. Surface barrier detectors.

doi: 10.1103/PhysRevLett.48.1787
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1982RI01      Nucl.Phys. A379, 173 (1982)

M.F.Rivet, R.Bimbot, D.Gardes, A.Fleury, F.Hubert, Y.Llabador

Cross Sections for Deeply Inelastic Transfer Reactions induced by Heavy Ions in Rare-Earth Targets

NUCLEAR REACTIONS ^{142,143,144,145,146}Nd, ^{144,147,148,149,150}Sm, ^151,153Eu, ¹⁵⁵Gd(Ar, X), E=275, 245 MeV; ¹³⁹La, ^140,142Ce, ¹⁴¹Pr, ^148,150Nd, ^{154,156,157,158,160}Gd, ¹⁵⁹Tb, ^152,154Sm(Ar, X), E=275 MeV; ^{142,143,144,145,146}Nd, ^{144,147,148,149,150,152}Sm(Cr, X), E=332 MeV; ^{142,144,146,148}Nd, ^{148,149,150,152,154}Sm(Fe, X), E=356 MeV; ^140,142Ce, ^{142,144,146,148}Nd, ^{144,148,149,150,152}Sm, ^151,153Eu, ^154,156,158Gd(Cu, X), E=401 MeV; measured cumulative yields, production σ for ^149,150,151Dy. Enriched targets, activation technique.

doi: 10.1016/0375-9474(82)90562-0
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1982RI06      Z.Phys. A307, 365 (1982)

M.F.Rivet, B.Gatty, H.Guillemot, B.Borderie, R.Bimbot, I.Forest, J.Galin, D.Gardes, D.Guerreau, M.Lefort, X.Tarrago, B.Tamain, L.Novicki

Correlations between Fission Fragments and Light Charged-Particles in the Reaction ²⁰Ne + ¹⁹⁷Au at 13 MeV/Nucleon

NUCLEAR REACTIONS ¹⁹⁷Au(²⁰Ne, pF), (²⁰Ne, dF), (²⁰Ne, tF), (²⁰Ne, αF), E=265 MeV; measured fission fragment(light particle)-coin, σ(θp, Ep, fragment θ), σ(θα, Eα, fragment θ); deduced fission σ(total), fusion L(critical), reaction mechanism. ²¹⁷Ac deduced fission characteristics, particle multiplicities. Rotating liquid drop model.

doi: 10.1007/BF01421298
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1981DU03      Phys.Rev. C23, 801 (1981)

J.P.Dufour, A.Fluery, R.Bimbot

Secondary Reactions as a Tool to Produce Exotic Nuclei

NUCLEAR REACTIONS ²⁰⁶Pb(α, xn), E=150 MeV; calculated average production σ for ^{205,204,203,202,201,200,199}Po. ^{199,200,201,202,203,204,205}Po(α, xn), E=100-150 MeV; calculated σ limit for energy averaged production of ¹⁹⁹Rn in secondary reaction. Inverse fusion, fragmentation production of exotic nuclei.

doi: 10.1103/PhysRevC.23.801
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1980BO27      Z.Phys. A298, 235 (1980)

B.Borderie, R.Bimbot, C.Cabot, D.Gardes, L.Nowicki, B.Tamain, C.Gregoire, C.Ngo, M.Berlanger, F.Hanappe

Limitation to the Fusion Cross Section for the System Mg + Cu at High Energy

NUCLEAR REACTIONS Cu(²⁴Mg, X), E=161-341 MeV; measured σ(θ) for evaporation residue, σ(fusion, E); deduced critical angular momentum. Sharp cutoff model.

doi: 10.1007/BF01418662
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1980DU02      Z.Phys. A294, 107 (1980)

J.P.Dufour, A.Fleury, F.Hubert, Y.Llabador, M.B.Mauhourat, R.Bimbot, D.Gardes

New Isotope ¹⁸⁴Pb

RADIOACTIVITY ¹⁸⁴Pb; measured Eα.

NUCLEAR REACTIONS ^147,148Sm(⁴⁰Ca, xn), E=190-250 MeV; measured α yield vs E, αα(t); deduced evidence for ¹⁸⁴Pb.

doi: 10.1007/BF01473127
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1980GA13      Phys.Rev. C21, 2447 (1980)

D.Gardes, R.Bimbot, J.Maison, M.F.Rivet, A.Fleury, F.Hubert, Y.Llabador

Angular Distributions and Ranges of Heavy Products from Quasi-Elastic Transfer Reactions Induced by Heavy Ions in ²⁰⁹Bi

NUCLEAR REACTIONS ²⁰⁹Bi(¹⁴N, X), E=74, 99 MeV; ²⁰⁹Bi(¹⁶O, X), E=85, 102 MeV; ²⁰⁹Bi(¹⁹F, X), E=95, 110 MeV; ²⁰⁹Bi(⁴⁰Ar, X), E=203, 212, 275 MeV; ²⁰⁹Bi(⁴⁰Ca, X), E=217 MeV; ¹⁹⁷Au(¹⁶O, X), E=112 MeV; Tl(⁴⁰Ar, X), E=242 MeV; measured production σ(θ), ranges for ²¹⁰Po, ²¹¹At, ²¹¹Rn, ^198,200Tl, ²⁰⁴Bi; deduced reaction mechanism.

doi: 10.1103/PhysRevC.21.2447
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1980RI03      Z.Phys. A296, 201 (1980)

M.F.Rivet, R.Bimbot, D.Gardes, G.Mouchaty, A.Fleury, F.Hubert, Y.Llabador

Deeply Inelastic Transfer Reactions Induced by Heavy Ions in Rare-Earth Targets

NUCLEAR REACTIONS ¹⁴¹Pr(⁴⁰Ar, xnyp), E=278 MeV; ^142,145Nd(⁴⁰Ar, xnyp), E=276 MeV; ^144,149Sm, ¹⁵¹Eu(⁴⁰Ar, xnyp), E=275 MeV; ¹⁴⁴Nd(⁵²Cr, xnyp), E=331 MeV; ¹⁴⁸Sm(⁵²Cr, xnyp), E=332 MeV; ¹⁴⁴Nd(⁵⁶Fe, xnyp), E=364 MeV; ¹⁴⁸Sm(⁵⁶Fe, xnyp), E=289, 366 MeV; ¹⁴⁴Nd(⁶³Cu, xnyp), E=421 MeV; ¹⁴⁸Sm(⁶³Cu, xnyp), E=330, 421 MeV; measured production σ(θ, fragment E) for ^150,151Dy, ¹⁴⁹Tb; deduced damping level in deep inelastic transfer reactions.

doi: 10.1007/BF01415834
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1979BI01      Z.Phys. A290, 157 (1979)

R.Bimbot, D.Gardes, J.Cugnon, R.da Silveira

Simple Formulae for Heavy Ion Subcoulomb Transfer Probabilities. Application to One and Two-Proton Transfers in Bismuth

NUCLEAR REACTIONS ²⁰⁹Bi(¹⁴N, ¹³C), (¹⁴N, ¹²B), E=50-70 MeV; ²⁰⁹Bi(¹⁶O, ¹⁵N), (¹⁶O, ¹⁴C), E=70-80 MeV; ²⁰⁹Bi(¹⁹F, ¹⁸O), (¹⁹F, ¹⁷N), E=70-90 MeV; ²⁰⁹Bi(⁴⁰Ar, ³⁹Cl), (⁴⁰Ar, ³⁸S), E=150-170 MeV; ²⁰⁹Bi(⁴⁰Ca, ³⁹K), (⁴⁰Ca, ³⁸Ar), E=150-180 MeV; ²⁰⁹Bi(⁵⁷Fe, ⁵⁵Mn), (⁵⁶Fe, ⁵⁴Cr), E=200-230 MeV; ²⁰⁹Bi(⁶³Cu, ⁶²Ni), (⁶³Cu, ⁶¹Co), E=220-250 MeV; calculated σ(E). DWBA approach.

doi: 10.1007/BF01408110
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1979BI02      Nucl.Phys. A318, 215 (1979)

R.Bimbot, M.F.Rivet, J.Girard, R.Lucas, J.Poitou

Complete Fusion and Transfer Reactions Induced by 273 MeV ⁴⁰Ar on ¹⁵⁹Tb

NUCLEAR REACTIONS ¹⁵⁹Tb(⁴⁰Ar, X), E=273 MeV; measured projected ranges, σ(E(recoil), Z, θ), Z=45-80, off line X-ray spectrometry. Compared calculated distributions for transfer products.

doi: 10.1016/0375-9474(79)90480-9
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1979LL01      Z.Phys. A289, 173 (1979)

Y.Llabador, F.Hubert, A.Fleury, D.Gardes, M.F.Rivet, R.Bimbot

Angular Distribution Analysis for Quasi-Elastic Transfer Reactions Induced in ²⁰⁹Bi Targets with Heavy Ions

NUCLEAR REACTIONS ²⁰⁹Bi(¹⁴N, ¹³C), (¹⁴N, ¹²B), E=74, 99 MeV; measured σ(θ). ²⁰⁹Bi(¹⁶O, ¹⁴C), E=83, 102 MeV; ²⁰⁹Bi(¹⁹F, ¹⁷N), E=95, 110 MeV; ²⁰⁹Bi(⁴⁰Ar, ³⁸S), E=203, 212, 275 MeV; ²⁰⁹Bi(⁴⁰Ca, ³⁸Ar), E=217 MeV; measured σ(θ). DWBA analysis of quasielastic transfer.

doi: 10.1007/BF01435935
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1979RI05      Z.Phys. A290, 57 (1979)

M.F.Rivet, R.Bimbot, D.Gardes, A.Fleury, F.Hubert, Y.Llabador

Production of ^149gTb in Deep Inelastic Transfer Reactions: An Approach to the Angular Momentum of Fragments

NUCLEAR REACTIONS ^142,145Nd, ^144,148Sm, ¹⁵⁴Gd(Ar, X), E=160-280 MeV; ¹⁴⁴Nd, ¹⁴⁸Sm, ¹⁵¹Eu, ¹⁵⁴Gd(Cu, X), E=280-420 MeV; measured σ(E). ¹⁴⁹Tb deduced production σ in deep-inelastic transfer reactions.

doi: 10.1007/BF01408480
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1978GA17      Phys.Rev. C18, 1298 (1978)

D.Gardes, R.Bimbot, J.Maison, L.de Reilhac, M.F.Rivet, A.Fleury, F.Hubert, Y.Llabador

Excitation Functions for Quasielastic Transfer Reactions Induced with Heavy Ions in Bismuth

NUCLEAR REACTIONS ²⁰⁹Bi(¹²C, X), (¹⁴N, X), (¹⁶O, X), (¹⁹F, X), (²⁰Ne, X), (⁴⁰Ar, X), ²⁰⁹Bi(⁵⁶Fe, X), (⁶³Cu, X), E=4.5-10 MeV/nucleon; measured σ(E) for production of ^{207,208,209,210,211}At, ²¹¹Rn.

doi: 10.1103/PhysRevC.18.1298
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0113.

1977RI02      Nucl.Phys. A276, 157 (1977)

M.F.Rivet, R.Bimbot, A.Fleury, D.Gardes, Y.Llabador

Evolution from Deep Inelastic Transfer to Quasi-Fission

NUCLEAR REACTIONS ¹⁴⁸Sm(⁵⁶Fe, X), E=300, 377 MeV; ¹⁴⁸Sm(⁶³Cu, X), E=342, 431 MeV; measured σ(E(recoil), θ) for production of ^150,151Dy, ^149gTb. Enriched targets.

doi: 10.1016/0375-9474(77)90164-6
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1975BI11      Nucl.Phys. A248, 377 (1975)

R.Bimbot, D.Gardes, R.L.Hahn, Y.De Moras, M.F.Rivet

Recoil Study of Ar Induced Multinucleon Transfer Reactions. Capture of 1 to 9 Charges by Rare-Earth Targets

NUCLEAR REACTIONS ¹³⁹La, ^140,142Ce, ¹⁴¹Pr, ^{144,147,148,149,150,152,154}Sm, ^151,153Eu, ^{154,155,156,157,158,160}Gd, ¹⁵⁹Tb(Ar, X), E=282 MeV; measured σ, σ(E(recoil), θ) for production of ¹⁵¹Dy, ¹⁵⁰Dy, ^149gTb. Enriched targets.

doi: 10.1016/0375-9474(75)90171-2
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1975GA04      J.Phys.(Paris), Suppl.Lett. 36, L-59 (1975)

D.Gardes, R.Bimbot, A.Fleury, F.Hubert, M.F.Rivet

Influence of Energetics on the Thresholds of Heavy Ion Transfer Reactions

NUCLEAR REACTIONS ²⁰⁹Bi(¹⁴N, ¹³C), (¹⁴N, ¹²B), (¹⁶O, ¹⁵N), (¹⁶O, ¹⁴C), E=50-110 MeV; calculated interaction potential.

doi: 10.1051/jphyslet:0197500360305900
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1974BI11      Nucl.Phys. A228, 85 (1974)

R.Bimbot, D.Gardes, R.L.Hahn, Y.de Moras, M.F.Rivet

Recoil Study of Multinucleon Transfer Reactions: Capture of Six Charges by Nd Targets in Ar Induced Reactions

NUCLEAR REACTIONS ^{142,143,144,145,146,148,150}Nd(⁴⁰Ar, X), E=257, 282 MeV; measured σ(E), σ(E(recoil), θ). Enriched targets.

doi: 10.1016/0375-9474(74)90447-3
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1973BI08      Phys.Rev. C8, 375 (1973)

R.Bimbot, M.F.Rivet

Excitation Functions and Recoil Ranges of Residual Nuclei Produced Through Kr-Induced Transfer Reactions in ²⁰⁹Bi Targets

NUCLEAR REACTIONS ²⁰⁹Bi(⁸⁴Kr, X), E=430-500 MeV; measured σ(E). ²¹¹At, ^210,211Rn deduced production σ, recoil range.

doi: 10.1103/PhysRevC.8.375
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0028.

1972AL09      Phys.Rev. C5, 799 (1972)

J.M.Alexander, R.Bimbot

Search for Spontaneous-Fission Isomerism in Nuclei of Medium Mass

NUCLEAR REACTIONS, Fission ²⁰⁹Bi(p, xF), E=42-135 MeV; Pb(d, xf), E=48, 75 MeV; ²⁰⁹Bi(d, xf), E=48-78 MeV; ¹⁶⁹Tm(¹⁴N, F), E=100, 103, 113 MeV; Ir(¹⁴N, F), E=71-111 MeV; ²⁰⁶Pb(α, xF), E=53-138 MeV; ¹⁵⁴Gd(α, xF), E=96-138 MeV; ²⁰⁹Bi(α, xF), E=53, 101, 138 MeV; ¹⁴¹Pr(¹⁴N, F), E=78, 90, 101, 111 MeV; measured I(recoil); deduced SF production σ, isomeric σ ratio.

doi: 10.1103/PhysRevC.5.799
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1972BI10      Nucl.Phys. A189, 193 (1972)

R.Bimbot, D.Gardes, M.F.Rivet

Recoil Study of Transfer Reactions: Evidence for α and ⁸Be Transfers in ¹²C Reactions with Heavy Nuclei (Au, Bi)

NUCLEAR REACTIONS ¹⁹⁷Au, ²⁰⁹Bi(¹²C, αxn); ¹⁹⁷Au, ²⁰⁹Bi(¹²C, ⁸Bexn), E(¹²C)=60-90 MeV; measured σ(E), σ(θ), recoil ranges.

doi: 10.1016/0375-9474(72)90654-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0126.

1972BI12      Nucl.Phys. A189, 539 (1972)

R.Bimbot, H.Gauvin, Y.Le Beyec, M.Lefort, N.T.Porile, B.Tamain

Reactions de Transfert d'un Grand Nombre de Nucleons Induites par ⁸⁴Kr Sur ²³²Th: Etude des Seuils de Reaction

NUCLEAR REACTIONS ²³²Th(⁸⁴Kr, X), E=450-494 MeV; measured σ(E) for ²²⁶Th, ²²⁵Th, ²²⁴Ac, ²²³Ac formation.

doi: 10.1016/0375-9474(72)90312-0
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1971BI08      J.Phys.(Paris) 32, 243 (1971)

R.Bimbot, Y.Le Beyec

Etude du Mecanisme des Reactions Nucleaires Induites par Particules Alpha de Haute Energie. II. Reactions ²⁰⁸Pb(α, xn)²¹²-x-Po et ^206,208Pb(α, pxn) Bi. Noyau Compose et Mecanismes

NUCLEAR REACTIONS ^206,208Pb(α, pxn), ²⁰⁸Pb(α, xn), E=40-150 MeV; measured σ(E); deduced fusion σ, non-compound contribution.

doi: 10.1051/jphys:01971003204024300
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2013.

1971BI14      Phys.Rev. C4, 2180 (1971)

R.Bimbot, D.Gardes, M.F.Rivet

Excitation Function and Recoil Ranges of ²¹¹At Produced Through ⁴⁰Ar + ²⁰⁹Bi Transfer Reactions

NUCLEAR REACTIONS ²⁰⁹Bi(⁴⁰Ar, X), E=190-270 MeV; measured recoil ranges, σ(E) for ²¹¹At production.

doi: 10.1103/PhysRevC.4.2180
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0034.

1971BI16      C.R.Acad.Sci., Ser.B, 273, 505 (1971)

R.Bimbot, C.Deprun, D.Gardes, H.Gauvin, Y.Le Beyec, M.Lefort, J.Peter, B.Tamain

Experiences Preliminaires sur les Reactions Nucleaires Induites par un Faisceau d'Ions Krypton de 450 a 500 MeV. Premiers Indices en Faveur de la Synthese de Noyaux Superlourds

NUCLEAR REACTIONS ⁷⁴Ge, ¹¹⁶Cd, Th, U(Kr, X), E=450-500 MeV; measured charged particle spectra.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2216.

1971BI22      C.R.Acad.Sci., Ser.B 273, 1054 (1971)

R.Bimbot, H.Gauvin

Reactions de Spallation de Noyaux Legers Induites par des Protons de 50, 100 et 153 MeV

NUCLEAR REACTIONS N, O, ¹⁸O, F, Mg, Al, Si, Cl(p, X), E=50, 100, 153 MeV; measured σ for ⁷Be, ¹¹C, ¹³N, ¹⁸F, ^22,24Na, ^34mCl formation.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2134.

1969BI05      J.Phys.(Paris) 30, 513 (1969)

R.Bimbot, H.Jaffrezic, Y.Le Beyec, M.Lefort, A.Vigny-Simon

Etude du Mecanisme des Reactions Nucleaires Induites par Particules α De Haute Energie. I. Reactions 206-Pb(α, Xn)210-xPo

NUCLEAR REACTIONS ²⁰⁶Pb(α, xn), E = 40-150 MeV; measured σ(E).

doi: 10.1051/jphys:01969003007051300
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2012.