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NSR database version of May 24, 2024.

Search: Author = B.Bouriquet

Found 15 matches.

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2010DA04      Phys.Rev. C 81, 024608 (2010)

M.Dasgupta, D.J.Hinde, S.L.Sheehy, B.Bouriquet

Suppression of fusion by breakup: Resolving the discrepancy between the reactions of 9Be with 208Pb and 209Bi

NUCLEAR REACTIONS 208Pb, 209Bi(9Be, xn)211Rn/212Rn/213Rn/214Rn/212Fr/213Fr/214Fr/215Fr/216Fr, E=44.0, 50.0, 60.0 MeV; measured α and fragment spectra; deduced complete fusion σ. Discussed discrepancies in previous cross section data for similar reactions.

doi: 10.1103/PhysRevC.81.024608
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1840.

2006AB33      Phys.Atomic Nuclei 69, 1101 (2006)

Y.Abe, G.I.Kosenko, C.W.Shen, B.Bouriquet, A.Marchix, D.Boilley, B.Giraud

Fusion Hindrance and Synthesis of Superheavy Elements

NUCLEAR REACTIONS 208Pb(58Ni, X), (64Ni, X), (70Zn, X), (71Ga, X), (76Ge, X), E(cm) ≈ 210-310 MeV; 209Bi(70Zn, X), E(cm) ≈ 260-300 MeV; 160Gd(132Sn, X), E(cm) ≈ 325-350 MeV; calculated fusion excitation functions. 208Pb(58Fe, n), (64Ni, n), (70Zn, n), (71Ga, n), (76Ge, n), E(cm) ≈ 215-285 MeV; 209Bi(64Ni, n), (70Zn, n), E(cm) ≈ 235-275 MeV; 160Gd(132Sn, γ), (132Sn, n), (132Sn, 2n), (132Sn, 3n), E(cm) ≈ 325-350 MeV; calculated σ. Fusion hindrance mechanism discussed.

doi: 10.1134/S1063778806070027
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2006CH52      Eur.Phys.J. A 30, 397 (2006)

A.Chatillon, Ch.Theisen, P.T.Greenlees, G.Auger, J.E.Bastin, E.Bouchez, B.Bouriquet, J.M.Casandjian, R.Cee, E.Clement, R.Dayras, G.de France, R.de Tourreil, S.Eeckhaudt, A.Gorgen, T.Grahn, S.Grevy, K.Hauschild, R.-D.Herzberg, P.J.C.Ikin, G.D.Jones, P.Jones, R.Julin, S.Juutinen, H.Kettunen, A.Korichi, W.Korten, Y.Le Coz, M.Leino, A.Lopez-Martens, S.M.Lukyanov, Yu.E.Penionzhkevich, J.Perkowski, A.Pritchard, P.Rahkila, M.Rejmund, J.Saren, C.Scholey, S.Siem, M.G.Saint-Laurent, C.Simenel, Yu.G.Sobolev, Ch.Stodel, J.Uusitalo, A.Villari, M.Bender, P.Bonche, P.-H.Heenen

Spectroscopy and single-particle structure of the odd-Z heavy elements 255Lr, 251Md and 247Es

RADIOACTIVITY 255Lr, 251Md(α) [from 209Bi(48Ca, 2n) and subsequent decay]; measured Eα, Eγ, E(ce), αγ-, α(ce)-coin, Qα, T1/2. 255Lr, 251Md, 247Es deduced levels, J, π, configurations.

doi: 10.1140/epja/i2006-10134-5
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Data from this article have been entered in the XUNDL database. For more information, click here.

2006TA04      Nucl.Phys. A764, 371 (2006)

G.Tabacaru, M.F.Rivet, B.Borderie, M.Parlog, B.Bouriquet, A.Chbihi, J.D.Frankland, J.P.Wieleczko, E.Bonnet, R.Bougault, R.Dayras, E.Galichet, D.Guinet, P.Lautesse, N.Le Neindre, O.Lopez, L.Manduci, L.Nalpas, P.Pawlowski, E.Rosato, R.Roy, S.Salou, B.Tamain, E.Vient, M.Vigilante, C.Volant, and the INDRA Collaboration

Multifragmentation of very heavy nuclear systems (III): Fragment velocity correlations and event topology at freeze-out

NUCLEAR REACTIONS Sn(129Xe, X), E=32 MeV/nucleon; U(155Gd, X), E=36 MeV/nucleon; measured fragments energy and charge distributions, yields, velocity correlations for central collisions; deduced freeze-out parameters. Comparison to stochastic mean-field calculation.

doi: 10.1016/j.nuclphysa.2005.08.019
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2005YA10      Phys.Rev. C 71, 041602 (2005)

R.Yanez, D.J.Hinde, B.Bouriquet, D.Duniec

Fission mass widths in 19F + 232Th, 16O + 235, 238U reactions at near-barrier energies

NUCLEAR REACTIONS 232Th(19F, X), 235,238U(16O, X), E ≈ 80-100 MeV; measured fission fragment mass distributions; deduced no anomalous mass ratio widths.

doi: 10.1103/PhysRevC.71.041602
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2004AB07      Nucl.Phys. A734, 168 (2004)

Y.Abe, B.Bouriquet, G.Kosenko, C.Shen

Theoretical Predictions of Residue Cross Sections for Superheavy Elements

NUCLEAR REACTIONS 208Pb(64Ni, n), (70Zn, n), (71Ga, n), (76Ge, n), E(cm) ≈ 230-290 MeV; 209Bi(64Ni, n), (70Zn, n), E(cm) ≈ 230-270 MeV; calculated excitation functions. Two-step model, comparison with data.

doi: 10.1016/j.nuclphysa.2004.01.026
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2004BO11      Comput.Phys.Commun. 159, 1 (2004)

B.Bouriquet, Y.Abe, D.Boilley

KEWPIE: A dynamical cascade code for decaying exited compound nuclei

NUCLEAR REACTIONS 246Cm(12C, xn), 242Pu(16O, xn), 236U(22Ne, xn), 232Th(26Mg, xn), E* ≈ 30-70 MeV; calculated evaporation residue σ. 208Pb(48Ca, xn), E*=5-50 MeV; calculated fusion and evaporation residue σ. Dynamical cascade code, comparisons with data.

doi: 10.1016/j.cpc.2003.10.002
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2004BO31      Prog.Theor.Phys.(Kyoto), Suppl. 154, 425 (2004)

B.Bouriquet, G.Kosenko, Y.Abe

Theoretical Predictions of Cross-Sections of the Super-Heavy Elements

NUCLEAR REACTIONS 208Pb, 209Bi(64Ni, n), (70Zn, n), 208Pb(58Fe, n), (71Ga, n), (76Ge, n), E(cm) ≈ 200-290 MeV; calculated σ. Two-step model, comparisons with data.

doi: 10.1143/PTPS.154.425
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2004BO40      Eur.Phys.J. A 22, 9 (2004)

B.Bouriquet, Y.Abe, G.Kosenko

Predictions of the residue cross-sections for the elements Z = 113 and Z = 114

NUCLEAR REACTIONS 208Pb(58Fe, X), (64Ni, X), (70Zn, X), (71Ga, X), (76Ge, X), 209Bi(70Zn, X), E(cm) ≈ 200-320 MeV; calculated fusion σ. 208Pb(58Fe, n), (71Ga, n), (76Ge, n), 208Pb, 209Bi(64Ni, n), (70Zn, n), E(cm) ≈ 220-290 MeV; calculated evaporation residue σ. Two-step model, comparisons with data.

doi: 10.1140/epja/i2004-10058-0
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2003AB29      Nucl.Phys. A722, 241c (2003); Erratum Nucl.Phys. A733, 351 (2004)

Y.Abe, B.Bouriquet, C.Shen, G.Kosenko

Theory of fusion hindrance and synthesis of the superheavy elements

NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm)=180-250 MeV; calculated fusion excitation functions. 238U, 244Pu, 248Cm, 252Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E* ≈ 20-50 MeV; calculated evaporation residue σ. Two-step model, comparisons with data.

doi: 10.1016/S0375-9474(03)01372-1
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2003AB34      Acta Phys.Pol. B34, 1927 (2003)

Y.Abe, B.Bouriquet

On theoretical problems in synthesis of superheavy elements

NUCLEAR REACTIONS 238U, 244Pu, 248Cm(48Ca, X), E(cm)=180-250 MeV; calculated fusion excitation functions. 208Pb, 244Pu(48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E* ≈ 5-50 MeV; calculated fusion, evaporation residue σ. Comparisons with data.

2003CO09      Phys.Rev. C 67, 064603 (2003)

J.Colin, D.Cussol, J.Normand, N.Bellaize, R.Bougault, A.M.Buta, D.Durand, O.Lopez, L.Manduci, J.Marie, J.C.Steckmeyer, B.Tamain, A.Van Lauwe, E.Vient, B.Borderie, F.Lavaud, N.Le Neindre, P.Pawlowski, E.Plagnol, M.F.Rivet, B.Bouriquet, A.Chbihi, J.D.Frankland, D.Guinet, B.Guiot, S.Hudan, J.P.Wieleczko, J.L.Charvet, R.Dayras, E.Galichet, P.Lautesse, L.Nalpas, M.Parlog, E.Rosato, R.Roy, M.Vigilante, C.Volant, and the INDRA Collaboration

Dynamical effects in multifragmentation at intermediate energies

NUCLEAR REACTIONS Ni(Ni, X), E=52, 90 MeV/nucleon; Sn(Xe, X), E=39-50 MeV/nucleon; Au, U(Ta, X), E=33, 39 MeV/nucleon; U(U, X), E=24 MeV/nucleon; measured fragments charge, mass, parallel velocity distributions; deduced entrance channel effects, other reaction mechanism features.

doi: 10.1103/PhysRevC.67.064603
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2003TA27      Eur.Phys.J. A 18, 103 (2003)

G.Tabacaru, B.Borderie, P.Desesquelles, M.Parlog, M.F.Rivet, R.Bougault, B.Bouriquet, A.M.Buta, E.Galichet, B.Guiot, P.Lautesse, N.Le Neindre, L.Manduci, E.Rosato, B.Tamain, M.Vigilante, J.P.Wieleczko

Fragment charge correlations and spinodal decomposition in finite nuclear systems

NUCLEAR REACTIONS Sn(129Xe, X), E=32, 39, 45, 50 MeV/nucleon; measured fragment charge and multiplicity distributions, charge correlations; deduced spinodal instabilities.

doi: 10.1140/epja/i2003-10066-9
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2003TR03      Nucl.Instrum.Methods Phys.Res. A501, 367 (2003)

A.Trzcinski, J.Lukasik, W.F.J.Muller, W.Trautmann, B.Zwieglinski, G.Auger, Ch.O.Bacri, M.L.Begemann-Blaich, N.Bellaize, R.Bittiger, F.Bocage, B.Borderie, R.Bougault, B.Bouriquet, Ph.Buchet, J.L.Charvet, A.Chbihi, R.Dayras, D.Dore, D.Durand, J.D.Frankland, E.Galichet, D.Gourio, D.Guinet, S.Hudan, B.Hurst, P.Lautesse, F.Lavaud, J.L.Laville, C.Leduc, A.LeFevre, R.Legrain, O.Lopez, U.Lynen, L.Nalpas, H.Orth, E.Plagnol, E.Rosato, A.Saija, C.Schwarz, C.Sfienti, J.C.Steckmeyer, G.Tabacaru, B.Tamain, K.Turzo, E.Vient, M.Vigilante, C.Volant

Energy calibration for the INDRA multidetector using recoil protons from 12C + 1H scattering

NUCLEAR REACTIONS 1H(12C, X), E=30 MeV/nucleon; measured particle spectra. 1H(12C, 12C), E=30 MeV/nucleon; measured recoil proton spectra, (carbon)(proton)-coin.

doi: 10.1016/S0168-9002(03)00623-5
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2002BE69      Nucl.Phys. A709, 367 (2002)

N.Bellaize, O.Lopez, J.P.Wieleczko, D.Cussol, G.Auger, Ch.O.Bacri, F.Bocage, B.Borderie, R.Bougault, B.Bouriquet, R.Brou, P.Buchet, A.M.Buta, J.L.Charvet, A.Chbihi, J.Colin, R.Dayras, N.De Cesare, A.Demeyer, D.Dore, D.Durand, J.D.Frankland, E.Galichet, E.Genouin-Duhamel, E.Gerlic, B.Guiot, D.Guinet, S.Hudan, G.Lanzalone, P.Lautesse, F.Lavaud, J.L.Laville, J.F.Lecolley, R.Legrain, N.Le Neindre, L.Manduci, J.Marie, L.Nalpas, J.Normand, M.Parlog, P.Pawlowski, E.Plagnol, M.F.Rivet, E.Rosato, R.Roy, F.Saint-Laurent, J.C.Steckmeyer, G.Tabacaru, B.Tamain, E.van Lauwe, L.Tassan-Got, E.Vient, M.Vigilante, C.Volant

Multifragmentation Process for Different Mass Asymmetry in the Entrance Channel Around the Fermi Energy

NUCLEAR REACTIONS 197Au(58Ni, X), E=32, 52, 90 MeV/nucleon; Sn(129Xe, X), E=50 MeV/nucleon; measured light, intermediate fragments multiplicity, charge distributions, correlations, kinetic energy and angular distributions; deduced multifragmentation mechanism features. Statistical multifragmentation model.

doi: 10.1016/S0375-9474(02)00988-0
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