NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = D.Boilley Found 31 matches. 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
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
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
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
2018CA26 Eur.Phys.J. A 54, 202 (2018) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
2004BO11 Comput.Phys.Commun. 159, 1 (2004) 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
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
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) Inverse Kramers formula and fusion dynamics of heavy ions
doi: 10.1140/epja/i2003-10088-0
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
2002BA76 Nucl.Phys. A707, 47 (2002) 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
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
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
1992AY01 Phys.Lett. 276B, 263 (1992) 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
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
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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