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NSR database version of April 26, 2024.

Search: Author = B.Bouriquet

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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, T_1/2. 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, 238}U 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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