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Search: Author = D.Boilley

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2021AB02      Prog.Theor.Exp.Phys. 2021, 021D01 (2021)

Y.Abe, D.Boilley, Q.Hourdille, C.Shen

A dynamical study of fusion hindrance with the Nakajima-Zwanzig projection method

doi: 10.1093/ptep/ptab005
Citations: PlumX Metrics

2021HO12      Eur.Phys.J. A 57, 162 (2021)

Q.Hourdille, Y.Lallouet, D.Boilley

Bayesian analysis of the uncertainty in decay lifetimes in the case of poor statistics

RADIOACTIVITY 278Nh(α), 262Db(SF); analyzed available data; deduced a Bayesian T1/2.

doi: 10.1140/epja/s10050-021-00473-0
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2019BR06      Phys.Rev. C 99, 024614 (2019)

R.Briselet, Ch.Theisen, M.Vandebrouck, A.Marchix, M.Airiau, K.Auranen, H.Badran, D.Boilley, T.Calverley, D.Cox, F.Dechery, F.Defranchi Bisso, A.Drouart, B.Gall, T.Goigoux, T.Grahn, P.T.Greenlees, K.Hauschild, A.Herzan, R.D.Herzberg, U.Jakobsson, R.Julin, S.Juutinen, J.Konki, M.Leino, A.Lightfoot, A.Lopez-Martens, A.Mistry, P.Nieminen, J.Pakarinen, P.Papadakis, J.Partanen, P.Peura, P.Rahkila, J.Rubert, P.Ruotsalainen, M.Sandzelius, J.Saren, C.Scholey, J.Sorri, S.Stolze, B.Sulignano, J.Uusitalo, A.Ward, M.Zielinska

Production cross section and decay study of 243Es and 249Md

NUCLEAR REACTIONS 197Au(48Ca, 2n)243Es, E=208, 210 MeV; 203Tl(48Ca, 2n)249Md, E=212.7, 214.3 MeV; measured reaction products, Eα, Iα, (recoil)α-coin, (recoil)αα-correlations, production σ(E) using RITU separator for recoils at the University of Jyvaskyla. Comparison of measured production σ(E) with calculations using the KEWPIE2 statistical fusion-evaporation code. Systematics of fusion-evaporation σ in the 2n channel.

RADIOACTIVITY 243Es(α)[from 197Au(48Ca, 2n), E=208, 210 MeV followed by separation of fragments using RITU separator at the Accelerator Laboratory of the University of Jyvaskyla (JYFL); 249Md(α)[from 203Tl(48Ca, 2n), E=212.7, 214.3 MeV]; 245Es(α)[α daughter of 249Md decay]; measured Eα, Iα, recoils, (recoils)α-correlations, half-lives and α-decay branching ratios for α decays of ground states of 243,245Es, 249Md. Comparison with previously measured values, and with theoretical predictions.

doi: 10.1103/PhysRevC.99.024614
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0923. Data from this article have been entered in the XUNDL database. For more information, click here.

2018CA19      Phys.Rev. C 98, 024305 (2018)

B.Cauchois, H.Lu, D.Boilley, G.Royer

Uncertainty analysis of the nuclear liquid drop model

ATOMIC MASSES Z=10-110, N=10-160; calculated uncertainties in the predicted binding energies from nuclear liquid-drop model, correlations between the theoretical binding energies and Q(α) of 208Pb and the binding energies for 2315 nuclei using standard regression analysis including a statistical treatment of the errors of the model.

doi: 10.1103/PhysRevC.98.024305
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2018CA26      Eur.Phys.J. A 54, 202 (2018)

B.Cauchois, D.Boilley

Constraining the shell correction energies of super-heavy nuclei - Uncertainty analysis

NUCLEAR STRUCTURE 257No, 261,267Rf, 265,271Sg, 269,275Hs, 273,279Ds, 277,283Cn, 287Fl, 291Lv; calculated Qα, mass excess, microscopic correction energy (SCE), mass excess correlation matrix for two α-decay chains (starting with 291Lv and 277Cn); deduced LDM (Liquid Drop Model) correlation matrix parameters.

doi: 10.1140/epja/i2018-12640-1
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2016LU08      Phys.Rev. C 94, 034616 (2016)

H.Lu, D.Boilley, Y.Abe, C.Shen

Synthesis of superheavy elements: Uncertainty analysis to improve the predictive power of reaction models

NUCLEAR REACTIONS 208Pb(58Fe, n)265Hs, E not given; calculated distribution of the empirical formation probability. Z=102-114; calculated cross sections for evaporation residues (ER) for one-neutron evaporation from compound nuclei with Z=102-114, formation and survival probabilities using uncertainty analysis for experimental data and theoretical parameters to constrain fusion models.

doi: 10.1103/PhysRevC.94.034616
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2014HE32      Phys.Rev.Lett. 113, 262505 (2014)

G.Henning, T.L.Khoo, A.Lopez-Martens, D.Seweryniak, M.Alcorta, M.Asai, B.B.Back, P.F.Bertone, D.Boilley, M.P.Carpenter, C.J.Chiara, P.Chowdhury, B.Gall, P.T.Greenlees, G.Gurdal, K.Hauschild, A.Heinz, C.R.Hoffman, R.V.F.Janssens, A.V.Karpov, B.P.Kay, F.G.Kondev, S.Lakshmi, T.Lauritsen, C.J.Lister, E.A.McCutchan, C.Nair, J.Piot, D.Potterveld, P.Reiter, A.M.Rogers, N.Rowley, S.Zhu

Fission Barrier of Superheavy Nuclei and Persistence of Shell Effects at High Spin: Cases of 254No and 220Th

NUCLEAR REACTIONS 208Pb(48Ca, 2n), E=217, 220.5 MeV; 176Yb(48Ca, 4n), E=219 MeV; measured reaction products, Eγ, Iγ; deduced fission barrier heights. Comparisons with theoretical fission barriers test theories that predict properties of superheavy elements.

doi: 10.1103/PhysRevLett.113.262505
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2011BO27      Phys.Rev. C 84, 054608 (2011)

D.Boilley, H.Lu, C.Shen, Y.Abe, B.G.Giraud

Fusion hindrance of heavy ions: Role of the neck

NUCLEAR REACTIONS 100Mo(100Mo, X), 110Pd(110Pd, X), E not given; calculated liquid drop model potential energy, neck distribution, LDM potential contour plots, fusion probability.

doi: 10.1103/PhysRevC.84.054608
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2011SH19      Phys.Rev. C 83, 054620 (2011)

C.Shen, D.Boilley, Q.Li, J.Shen, Y.Abe

Fusion hindrance in reactions with very heavy ions: Border between normal and hindered fusion

NUCLEAR REACTIONS 208Pb(86Kr, X), 110Pd(110Pd, X), 100Mo(100Mo, X), 90Zr(90Zr, X), E not given; calculated LDM potential, fusion hindrance. Two-center liquid drop model.

doi: 10.1103/PhysRevC.83.054620
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2010AB19      Nucl.Phys. A834, 349c (2010)

Y.Abe, C.Shen, D.Boilley, B.G.Giraud, G.Kosenko

Mechanism of Fusion Hindrance and Predictions of SHE Production

NUCLEAR REACTIONS 249Bk, 249Cf(48Ca, xn), E*=20-55 MeV; calculated σ, reaction mechanism features.

doi: 10.1016/j.nuclphysa.2010.01.037
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2010GO18      Eur.Phys.J. A 43, 251 (2010)

C.Golabek, S.Heinz, W.Mittig, F.Rejmund, A.C.C.Villari, S.Bhattacharyva, D.Boilley, G.De France, A.Drouart, L.Gaudefroy, L.Giot, V.Maslov, M.Morjean, G.Mukherjee, Yu.Penionzkevich, P.Roussel-Chomaz, C.Stodel

Investigation of deep inelastic reactions in 238U + 238U at Coulomb barrier energies

NUCLEAR REACTIONS 238U(238U, X), E=6.09-7.35 MeV/nucleon; measured reaction product yields, mass and energy distributions, σ(θ) using VAMOS detector; deduced reaction mechanism features, di-nuclear system formation. Comparison with data and models.

doi: 10.1140/epja/i2010-10911-5
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2009AB28      Int.J.Mod.Phys. E18, 2169 (2009)

Y.Abe, C.Shen, D.Boilley, B.G.Giraud

From di-nucleus to mono-nucleus: Neck evolution in fusion of massive systems

NUCLEAR REACTIONS 100Mo(100Mo, X), E not given; calculated the neck degree of freedom during fusioning process between heavy ions, average trajectory, over-passing probability and the current at the top of the barrier.

doi: 10.1142/S0218301309014494
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2008AB26      Int.J.Mod.Phys. E17, 2214 (2008)

Y.Abe, C.Shen, G.Kosenko, D.Boilley, B.G.Giraud

Di-nucleus dynamics toward fusion of heavy nuclei

doi: 10.1142/S0218301308011367
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2008BO34      Int.J.Mod.Phys. E17, 1681 (2008)

D.Boilley, A.Marchix, D.Wilgenbus, Y.Lallouet, F.Gimbert, Y.Abe

What can we learn from the fission time of the super-heavy elements?

doi: 10.1142/S0218301308010696
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2008GO33      Int.J.Mod.Phys. E17, 2235 (2008)

C.Golabek, A.C.C.Villari, S.Heinz, W.Mittig, S.Bhattacharyya, D.Boilley, G.De France, A.Drouart, L.Gaudefroy, L.Giot, A.Marchix, V.Maslov, M.Morjean, G.Mukherjee, A.Navin, Yu.Penionzkevich, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, C.Stodel

Search for a long living giant system in 238U + 238U collisions near the coulomb barrier

NUCLEAR REACTIONS 238U(238U, X), E=6.09-7.35 MeV/nucleon; measured mass spectra; deduced total kinetic energy loss, production yields, σ(θ).

doi: 10.1142/S0218301308011409
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2008SH26      Int.J.Mod.Phys. E17, Supplement 1, 66 (2008)

C.W.Shen, Y.Abe, D.Boilley, G.Kosenko, E.Zhao

Isospin dependence of reactions 48Ca+243-251Bk

NUCLEAR REACTIONS 243,244,245,246,247,248,249,250,251Bk(48Ca, X), E(cm)=203.3 MeV; calculated fusion σ. Two-step model, KEWPIE code.

doi: 10.1142/S0218301308011768
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2007AB08      Int.J.Mod.Phys. E16, 491 (2007)

Y.Abe, A.Marchix, C.Shen, B.Yilmaz, G.Kosenko, D.Boilley, B.G.Giraud

Dynamics of massive systems and synthesis of superheavy elements

NUCLEAR REACTIONS 208Pb(58Fe, n), E(cm)=210-235 MeV; 132Sn, 160Gd(132Sn, n), (132Sn, 2n), (132Sn, 3n), (132Sn, 4n), E(cm)=265-295 MeV; calculated fusion and evaporation residue σ.

doi: 10.1142/S0218301307005922
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2007BO37      Eur.Phys.J. A 33, 47 (2007)

D.Boilley, A.Marchix, B.Jurado, K.-H.Schmidt

A new formula for the saddle-to-scission time

doi: 10.1140/epja/i2007-10415-5
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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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2004AB25      Acta Phys.Hung.N.S. 19, 77 (2004)

Y.Abe, D.Boilley, B.Giraud, G.Kosenko, C.Shen

Fusion Theory for Synthesis of the Superheavy Elements

NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm) ≈ 180-250 MeV; calculated fusion excitation functions. Fluctuation-dissipation dynamics, comparison with data.

doi: 10.1556/APH.19.2004.1-2.11
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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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2003AB17      Yad.Fiz. 66, 1093 (2003); Phys.Atomic Nuclei 66, 1057 (2003)

Y.Abe, C.W.Shen, G.I.Kosenko, D.Boilley

Theory of Fusion for Superheavy Elements

NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm) ≈ 180-240 MeV; calculated fusion σ, maximum evaporation residue σ. Two-step model, comparison with data.

doi: 10.1134/1.1586418
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2003AB33      Acta Phys.Pol. B34, 2091 (2003)

Y.Abe, D.Boilley, G.Kosenko, C.Shen

Reaction mechanisms for synthesis of superheavy elements

NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm)=180-250 MeV; calculated fusion σ. Two-step mechanism, shape evolution. Comparison with data.

2003BO42      Eur.Phys.J. A 18, 627 (2003)

D.Boilley, Y.Abe, J.-D.Bao

Inverse Kramers formula and fusion dynamics of heavy ions

doi: 10.1140/epja/i2003-10088-0
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2002AB28      Prog.Theor.Phys.(Kyoto), Suppl. 146, 104 (2002)

Y.Abe, D.Boilley, G.Kosenko, J.D.Bao, C.W.Shen, B.Giraud, T.Wada

Fusion Dynamics of Massive Heavy-Ion Systems

NUCLEAR REACTIONS 244Pu(48Ca, X), E ≈ threshold; calculated fusion probability, related features. Two-step model.

doi: 10.1143/PTPS.146.104
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2002BA76      Nucl.Phys. A707, 47 (2002)

J.-D.Bao, D.Boilley

Quantum Propagator Approach to Heavy-Ion Fusion

NUCLEAR REACTIONS 100Mo(100Mo, X), 123Sb(86Kr, X), 124Sn(96Zr, X), E(cm) ≈ 190-270 MeV; calculated fusion probability. Quantum propagator approach, comparison with data.

doi: 10.1016/S0375-9474(02)00751-0
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1994BO37      Z.Phys. A349, 119 (1994)

D.Boilley, Y.Abe, S.Ayik, E.Suraud

A Bohr-Mottelson Model of Nuclei at Finite Temperature

doi: 10.1007/BF01291169
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1993BO19      Nucl.Phys. A556, 67 (1993)

D.Boilley, E.Suraud, Y.Abe, S.Ayik

Nuclear Fission with a Langevin Equation

NUCLEAR REACTIONS 205At, 248Cf(n, F), E=thermal; calculated fission rate vs temperature, time. Langevin equation.

doi: 10.1016/0375-9474(93)90238-S
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1992AY01      Phys.Lett. 276B, 263 (1992)

S.Ayik, D.Boilley

Damping of Collective Vibrations in a Memory-Dependent Transport Model

NUCLEAR STRUCTURE A ≤ 200; calculated GDR, GQR damping width. 108Sn; calculated giant dipole resonance damping width vs excitations. Memory dependent transport model.

doi: 10.1016/0370-2693(92)90315-U
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1992AY03      Nucl.Phys. A545, 35c (1992)

S.Ayik, E.Suraud, M.Belkacem, D.Boilley

The Boltzmann-Langevin Model for Nuclear Collisions

NUCLEAR REACTIONS 12C(12C, 12C), E=40-100 MeV/nucleon; calculated total quadrupole momentum distribution associated collision rate, diffusion coeffient, mean value, variance time evolutions. 12C(12C, K+X), E ≈ 400-1400 MeV/nucleon; calculated K+ production σ(E). Boltzmann-Langevin model.

doi: 10.1016/0375-9474(92)90444-O
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1989SU10      Nucl.Phys. A495, 73c (1989)

E.Suraud, D.Cussol, Ch.Gregoire, D.Boilley, M.Pi, P.Schuck, B.Remaud, F.Sebille

Explosions in Landau Vlasov Dynamics

NUCLEAR REACTIONS 40Ca(40Ca, X), E=20-100 MeV/nucleon; 50Ti(40Ar, X), E=20, 44 MeV/nucleon; 197Au(40Ar, X), E=60 MeV/nucleon; calculated average density time evolution. Landau-Vlasov simulations.

doi: 10.1016/0375-9474(89)90309-6
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