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NSR database version of May 10, 2024.

Search: Author = J.Lei

Found 33 matches.

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2024SP03      Nuovo Cim. C 47, 34 (2024)

R.Sparta, A.DiPietro, P.Figuera, O.Tengblad, A.M.Moro, J.Lei, I.Martel, J.P.Fernandez Garcia, L.Acosta, M.J.G.Borge, J.Cederkall, T.Davinson, B.Diana, J.Diaz Ovejas, L.M.Fraile, D.Galaviz, J.Halkjaer Jensen, B.Jonson, M.La Cognata, M.Lattuada, A.Perea, A.M.Sanchez Benitez, N.Soic, S.Vinal Onses

8B reaction dynamics researched at HIE-ISOLDE

NUCLEAR REACTIONS 64Zn(8B, X), E=4.5 MeV/nucleon; measured reaction products. 8B; deduced σ, halo structure of the light nucleus impact on reaction dynamics. Comparison with continuum discretised coupled channel (CDCC) calculations. HIE-ISOLDE at CERN.

doi: 10.1393/ncc/i2024-24034-y
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2023LE12      Phys.Rev. C 108, 034612 (2023)

J.Lei, A.M.Moro

Advancing the Ichimura-Austern-Vincent model with continuum-discretized coupled-channels wave functions for realistic descriptions of two-body projectile breakup

doi: 10.1103/PhysRevC.108.034612
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2023LI36      Phys.Rev. C 108, 014617 (2023)

H.Liu, S.Nakayama, J.Lei, Z.Ren

Comparison of Ichimura-Austern-Vincent and Glauber models for the deuteron-induced inclusive breakup reaction in light and medium-mass nuclei

NUCLEAR REACTIONS 12C, 58Ni(d, pX), (d, nX), E=56, 100 MeV; calculated σ(θ, E) as a function of emitted particle angle and energy, nonelastic breakup σ(θ, E). Calculations utilizing model of Ichimura, Austern, and Vincent (IAV) and the Glauber model with the quantum S matrix. Comparison to experimental data.

doi: 10.1103/PhysRevC.108.014617
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2023LI41      Phys.Rev. C 108, 024606 (2023)

J.Liu, J.Lei, Z.Ren

Testing the validity of the surface approximation for reactions induced by weakly bound nuclei with a fully quantum-mechanical model

NUCLEAR REACTIONS 28Si(d, pX), (6Li, αX), E=5-100 MeV; 208Pb(d, pX), (6Li, αX), E=20-100 MeV; calculated nonelastic breakup σ(E), dependence of σ(E) on radial cut-offs to scattering waves. Calculations in the frame of full y quantum mechanical model from Ichimura, Austern and Vincent(IAV).

doi: 10.1103/PhysRevC.108.024606
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2023LU10      Phys.Rev. C 108, 024612 (2023)

Y.Lu, J.Lei, Z.Ren

Systematic single-folding optical potential for 6Li and 7Li based on KD02 potentials

NUCLEAR REACTIONS 24,25,26Mg, 27Al, 28Si, 39K, 40Ca, 58Ni, 89Y, 90,91,92,94,96Zr, 112,116,120,124Sn, 208Pb, 209Bi(6Li, 6Li), E=31-240 MeV;24,26Mg, 28Si, 40,44,48Ca, 54,56Fe, 58,60Ni, 89Y, 90Zr, 116,118Sn, 142Nd, 144Sm, 208Pb(7Li, 7Li), E=33-350 MeV; analyzed experimental data of nucleus-nucleus elastic scattering and σ energy dependence; deduced optical potential parameters; calculated σ(θ), σ(E). 116Sn, 208Pb(6Li, X), E=5-300 MeV; 28Si, 64Zn, 116Sn, 208Pb(7Li, X), E=5-360 MeV; calculated σ(E). Energy-dependent systematic optical potential on the KD02 optical potential within the framework of the single-folding model. Comparison to experimental data and calculations performed with Cook's systematic optical potential.

doi: 10.1103/PhysRevC.108.024612
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2023SA13      Eur.Phys.J. A 59, 48 (2023)

O.C.B.Santos, R.Lichtenthaler, A.M.Moro, K.C.C.Pires, U.Umbelino, A.S.Serra, E.O.N.Zevallo, A.L.de Lara, V.Scarduelli, J.Alcantara-Nunez, A.Lepine-Szily, J.Lei, S.Appannababu, M.Assuncao

One-neutron stripping from 8Li projectiles to 9Be target nuclei

NUCLEAR REACTIONS 9Be(8Li, 7Li), E=23.8 MeV; measured reaction products; deduced σ(θ), σ(θ, E). Comparison with optical model calculations using standard Woods-Saxon potentials. The RIBRAS (Radioactive Ion Beams in Brasil) facility.

doi: 10.1140/epja/s10050-023-00959-z
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2022DU05      Phys.Rev. C 105, 034602 (2022)

F.F.Duan, Y.Y.Yang, J.Lei, K.Wang, Z.Y.Sun, D.Y.Pang, J.S.Wang, X.Liu, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Hu, Z.H.Gao, X.X.Xu, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, G.Yang, S.Y.Jin, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Elastic scattering and breakup reactions of neutron-rich nucleus 11Be on 208Pb at 210 MeV

NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, 10Be), E=210 MeV; measured reaction products; deduced σ(θ), σ. Comparison with CDCC calculations and experimental results for other reaction systems including tightly- and weakly-bound projectiles impinging on medium to heavy mass targets. Beam by Heavy-Ion Research Facility in Lanzhou (HIRFL, China).

doi: 10.1103/PhysRevC.105.034602
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2022WA16      Phys.Rev. C 105, 054616 (2022)

K.Wang, Y.Y.Yang, V.Guimaraes, D.Y.Pang, F.F.Duan, Z.Y.Sun, J.Lei, G.Yang, S.W.Xu, J.B.Ma, Q.Liu, Z.Bai, H.J.Ong, B.F.Lv, S.Guo, X.H.Wang, R.H.Li, M.Kumar Raju, Z.G.Hu, H.S.Xu

Elastic scattering investigation of radioactive 13B and 13O projectiles on a 208Pb target at intermediate energies

NUCLEAR REACTIONS 208Pb(13B, 13B), E=254 MeV; 208Pb(13O, 13O), E=413 MeV; measured reaction products, time-of-flight, magnetic rigidity, angular distributions; deduced σ(θ). 13B, 13O; deduced proton, neutron and matter rms radii. Optical model analysis with Sao Paulo and Pang global potentials. Comparison to continuum discretized coupled channels (CDCC) calculations. Beams were produced by fragmentation of a primary 59.54 MeV/nucleon 16O beam delivered by the Heavy-Ion Research Facility in Lanzhou (HIRFL).

doi: 10.1103/PhysRevC.105.054616
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021GO05      Eur.Phys.J. A 57, 57 (2021)

M.Gomez-Ramos, J.Gomez-Camacho, J.Lei, A.M.Moro

The Hussein-McVoy formula for inclusive breakup revisited

NUCLEAR REACTIONS 9Be(14O, 13N), E=80 MeV/nucleon; 9Be(14O, 13O), E=53 MeV/nucleon; calculated integrated nonelastic breakup σ.

doi: 10.1140/epja/s10050-021-00376-0
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2021SA25      Phys.Rev. C 103, 064601 (2021)

O.C.B.Santos, R.Lichtenthaler, K.C.C.Pires, U.Umbelino, E.O.N.Zevallos, A.L.de Lara, A.S.Serra, V.Scarduelli, J.Alcantara-Nunez, V.Guimaraes, A.Lepine-Szily, J.C.Zamora, A.M.Moro, S.Appannababu, M.Assuncao, A.Barioni, R.Linares, V.A.B.Zagatto, P.N.de Faria, M.C.Morais, V.Morcelle, J.M.B.Shorto, J.Lei

Evidence of the effect of strong stripping channels on the dynamics of the 8Li + 58Ni reaction

NUCLEAR REACTIONS 58Ni(8Li, 8Li), (8Li, 8Li'), (8Li, 7Li), E=23.9, 26.1, 28.7, 30 MeV, [secondary 8Li beam produced in 9Be(7Li, 8Li), E=26-32 MeV using the RIBRAS facility at the 8-UD Pelletron accelerator of the University of Sao Paulo]; measured reaction products, two-dimensional ΔE-E particle spectra, elastic σ(θ). Comparison with optical model and continuum discretized coupled channels (CDCC) calculations for the elastic and nonelastic breakup or particle-transfer processes.

doi: 10.1103/PhysRevC.103.064601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD1004.


2021SP06      Phys.Lett. B 820, 136477 (2021)

R.Sparta, A.Di Pietro, P.Figuera, O.Tengblad, A.M.Moro, I.Martel, J.P.Fernandez-Garcia, J.Lei, L.Acosta, M.J.G.Borge, G.Bruni, J.Cederkall, T.Davinson, J.D.Ovejas, L.M.Fraile, D.Galaviz, J.H.Jensen, B.Jonson, M.La Cognata, A.Perea, A.M.Sanchez-Benitez, N.Soic, S.Vinals

Probing proton halo effects in the 8B+64Zn collision around the Coulomb barrier

NUCLEAR REACTIONS 64Zn(8B, 8B), (8B, X)7Be, E=4.9 MeV/nucleon; measured reaction products. 8B; deduced σ(θ, E). Comparison with continuum-discretized coupled-channels (CDCC) calculations.

doi: 10.1016/j.physletb.2021.136477
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2021WA12      Phys.Rev. C 103, 024606 (2021)

K.Wang, Y.Y.Yang, A.M.Moro, V.Guimaraes, J.Lei, D.Y.Pang, F.F.Duan, J.L.Lou, J.C.Zamora, J.S.Wang, Z.Y.Sun, H.J.Ong, X.Liu, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Hu, X.X.Xu, Z.H.Gao, G.Yang, S.Y.Jin, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu, for the RIBLL Collaboration

Elastic scattering and breakup reactions of the proton drip-line nucleus 8B on 208Pb at 238 MeV

NUCLEAR REACTIONS 208Pb(3He, 3He), E=55 MeV; 208Pb(8B, 8B), (8B, X), E=238 MeV; 208Pb(7Be, 7Be), (7Be, X), E=175 MeV, [3He, 7Be and 8B secondary beams from 9Be(12C, X), E=59.7 MeV primary reaction followed by ΔE-E particle identification of fragments at RIBLL-HIRFL-Lanzhou facility]; measured reaction products, particle spectra, using double-sided silicon strip detectors (DSSDs) and a CsI(Tl) crystal array; deduced σ(θ) for elastic scattering and inelastic breakup (NEB) of 8B and 7Be, no significant Coulomb rainbow suppression. Comparison with optical model and continuum discretized coupled channels (CDCC) calculations.

doi: 10.1103/PhysRevC.103.024606
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0265.


2021YA01      Phys.Lett. B 813, 136045 (2021)

L.Yang, C.J.Lin, H.Yamaguchi, J.Lei, P.W.Wen, M.Mazzocco, N.R.Ma, L.J.Sun, D.X.Wang, G.X.Zhang, K.Abe, S.M.Cha, K.Y.Chae, A.Diaz-Torres, J.L.Ferreira, S.Hayakawa, H.M.Jia, D.Kahl, A.Kim, M.S.Kwag, M.La Commara, R.Navarro-Perez, C.Parascandolo, D.Pierroutsakou, J.Rangel, Y.Sakaguchi, C.Signorini, E.Strano, X.X.Xu, F.Yang, Y.Y.Yang, G.L.Zhang, F.P.Zhong, J.Lubian

Insight into the reaction dynamics of proton drip-line nuclear system 17F+58Ni at near-barrier energies

NUCLEAR REACTIONS 58Ni(17F, 17F), (17F, X), E=43.6, 47.5, 55.7, 63.1 MeV; measured reaction products, Eα, Iα, Ep, Ip. 16O, 17F; deduced σ, σ(θ) quasielastic scattering and fusion.

doi: 10.1016/j.physletb.2020.136045
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2687.


2020DU18      Phys.Lett. B 811, 135942 (2020)

F.F.Duan, Y.Y.Yang, K.Wang, A.M.Moro, V.Guimaraes, D.Y.Pang, J.S.Wang, Z.Y.Sun, J.Lei, A.Di Pietro, X.Liu, G.Yang, J.B.Ma, P.Ma, S.W.Xu, Z.Bai, X.X.Sun, Q.Hu, J.L.Lou, X.X.Xu, H.X.Li, S.Y.Jin, H.J.Ong, Q.Liu, J.S.Yao, H.K.Qi, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Scattering of the halo nucleus 11Be from a lead target at 3.5 times the Coulomb barrier energy

NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, X), E=140 MeV; 208Pb(10Be, X), (10Be, X), E=127 MeV; 208Pb(9Be, 9Be), (9Be, X), E=88 MeV; measured reaction products. 9,10,11Be; deduced σ(θ), σ(E), σ. Comparison with continuum discretized coupled channel (CDCC) as well as by the XCDCC calculations.

doi: 10.1016/j.physletb.2020.135942
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0235.


2020LE08      Phys.Rev. C 102, 014608 (2020)

J.Lei, P.Descouvemont

Lagrange-mesh R-matrix method for inhomogeneous equations

NUCLEAR REACTIONS 93Nb(d, pX), E=25.5 MeV; calculated double differential σ(E, θ), real and imaginary parts of the source term function for an outgoing proton using Lagrange-mesh R-matrix method. Comparisons with Green's function and Numerov methods.

doi: 10.1103/PhysRevC.102.014608
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2019DI11      Phys.Lett. B 798, 134954 (2019)

A.Di Pietro, A.M.Moro, J.Lei, R.de Diego

Insights into the dynamics of breakup of the halo nucleus 11Be on a 64Zn target

NUCLEAR REACTIONS 64Zn(11Be, X)10Be, E=28.7 MeV; analyzed available data; deduced quasielastic and breakup σ(θ), σ(θ, E) using CDCC and extended CDCC (XCDCC) calculations.

doi: 10.1016/j.physletb.2019.134954
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1856.


2019FE05      Phys.Rev. C 99, 054605 (2019)

J.P.Fernandez-Garcia, A.Di Pietro, P.Figuera, J.Gomez-Camacho, M.Lattuada, J.Lei, A.M.Moro, M.Rodriguez-Gallardo, V.Scuderi

Breakup mechanisms in the 6He + 64Zn reaction at near-barrier energies

NUCLEAR REACTIONS 64Zn(α, α), E=17.4 MeV; measured scattered α particles, differential σ(θ) using LEDA-type detectors and single-sided silicon strip detectors for particle detection at the Louvain la Neuve (Belgium) cyclotron facility; analyzed present data and previous experimental data at E(α)=13.2 MeV by optical model calculations based on the Sao Paulo potential. 64Zn(6He, 6He), (6He, α), E=14.85, 17.9 MeV; measured scattered particles, differential σ(θ) for outgoing 6He and α particles, the latter from 2n transfer process; analyzed present data and previous experimental data at E(6He)=9.8 and 13.5 MeV by optical model calculations, coupled-reaction-channel (CRC), continuum-discretized coupled channel (CDCC), and DWBA inclusive-breakup models.

doi: 10.1103/PhysRevC.99.054605
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2458.


2019HL01      Phys.Rev. C 100, 034609 (2019)

L.Hlophe, J.Lei, Ch.Elster, A.Nogga, F.M.Nunes, D.Jurciukonis, A.Deltuva

Deuteron-α scattering: Separable versus nonseparable Faddeev approach

NUCLEAR REACTIONS 4He(d, d), (d, np), E=10, 20, 50 MeV; calculated differential σ(E) for elastic and breakup reactions using the momentum-space Faddeev Alt-Grassberger-Sandhas (AGS) framework.

doi: 10.1103/PhysRevC.100.034609
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2019LE01      Phys.Rev.Lett. 122, 042503 (2019)

J.Lei, A.M.Moro

Puzzle of Complete Fusion Suppression in Weakly Bound Nuclei: A Trojan Horse Effect?

NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E<50 MeV; calculated σ, σ(E); deduced a new method to compute complete fusion σ in collisions involving weakly bound nuclei.

doi: 10.1103/PhysRevLett.122.042503
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2019LE17      Phys.Rev.Lett. 123, 232501 (2019)

J.Lei, A.M.Moro

Unraveling the Reaction Mechanisms Leading to Partial Fusion of Weakly Bound Nuclei

NUCLEAR REACTIONS 209Bi(6Li, α), E<40 MeV; calculated σ(θ). Comparison with available data.

doi: 10.1103/PhysRevLett.123.232501
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2018LE02      Phys.Rev. C 97, 011601 (2018)

J.Lei, A.M.Moro

Post-prior equivalence for transfer reactions with complex potentials

NUCLEAR REACTIONS 58Ni(d, p), E=80 MeV; calculated angle-integrated proton energy spectra in inclusive transfer and breakup reactions; analyzed post-, and prior equivalence using model of Ichimura, Austern and Vincent (IAV) for post-forms and that of Udagawa and Tamura (UT) for prior-forms.

doi: 10.1103/PhysRevC.97.011601
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2018LE06      Phys.Rev. C 97, 034628 (2018)

J.Lei

Inclusive breakup calculations in angular momentum basis: Application to 7Li + 58Ni

NUCLEAR REACTIONS 58Ni(7Li, 7Li), (7Li, αX), E=14.22, 16.25, 18.28, 20.31 MeV; calculated differential σ(θ, E), α(θ, E) for elastic breakup (EBU) and nonelastic breakup (NEB); deduced inclusive breakup cross sections for arbitrary values of orbital angular momentum. 58Ni(6Li, X), (7Li, X), E(cm)/VB=0.6-1.4; calculated ratios of elastic breakup (EBU)/total breakup (TBU), and nonelastic breakup (NEB) cross sections. Angular momentum basis method within the model proposed by Ichimura, Austern, and Vincent (IAV), and within the closed-form DWBA model. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.034628
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2018LE16      Phys.Rev. C 98, 051001 (2018)

J.Lei, L.Hlophe, Ch.Elster, A.Nogga, F.M.Nunes, D.R.Phillips

Few-body universality in the deuteron-α system

NUCLEAR STRUCTURE 6Li; calculated d-α S-wave scattering length and absolute value of the n-p-α three body separation energy using variety of phase-shift equivalent nucleon-nucleon and α-nucleon interactions; interpreted as a deuteron or two-nucleon halo nucleus from dα and 6Li correlation.

doi: 10.1103/PhysRevC.98.051001
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2017HL02      Phys.Rev. C 96, 064003 (2017)

L.Hlophe, J.Lei, C.Elster, A.Nogga, F.M.Nunes

6Li in a three-body model with realistic Forces: Separable versus nonseparable approach

NUCLEAR STRUCTURE 6Li; calculated three-body binding energies for the ground state, momentum distributions of different pairs in the ground state of 6Li, by solving momentum-space Faddeev equations using separable interactions based on the Ernst-Shakin-Thaler (EST) scheme, and with CD-Bonn interaction for the np pair and Bang potential for the n(p)-α subsystems.

doi: 10.1103/PhysRevC.96.064003
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2017LE02      Phys.Rev. C 95, 044605 (2017)

J.Lei, A.M.Moro

Comprehensive analysis of large α yields observed in6Li-induced reactions

NUCLEAR REACTIONS 208Pb(6Li, αX), E=29, 33, 35, 39 MeV; 144Sm(6Li, 6Li), E=22.1, 35.1 MeV; 159Tb(6Li, αX), E=23, 25, 27, 30, 35 MeV; 118Sn(6Li, 6Li), (6Li, αX), E=18, 19, 20, 21, 22.5, 24 MeV; 59Co(6Li, 6Li), E=18 MeV; 59Co(6Li, αX), E=21.5 MeV; 58Ni(6Li, 6Li), (6Li, αX), E=12, 14, 16, 18, 20 MeV; 209Bi(6Li, αX); analyzed σ(θ) data for α particles and elastic reactions; deduced elastic breakup (EBU) and nonelastic breakup (NEB) components of the inclusive breakup cross sections using continuum-discretized coupled-channels (CDCC) method.

doi: 10.1103/PhysRevC.95.044605
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2017PO13      Eur.Phys.J. A 53, 178 (2017)

G.Potel, G.Perdikakis, B.V.Carlson, M.C.Atkinson, W.H.Dickhoff, J.E.Escher, M.S.Hussein, J.Lei, W.Li, A.O.Macchiavelli, A.M.Moro, F.M.Nunes, S.D.Pain, J.Rotureau

Toward a complete theory for predicting inclusive deuteron breakup away from stability

NUCLEAR REACTIONS 93Nb(d, pn), E=10, 25.5 MeV; calculated σ(ln), σ(θn) assuming both elastic and nonelastic breakup. Compared with published calculations. 40,48,60Ca(d, pn), E=20, 40 MeV; calculated σ(Ep) vs En and vs ln using both elastic and nonelastic breakup and using Hussein-McVoy theory.

doi: 10.1140/epja/i2017-12371-9
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2016DU18      Phys.Rev. C 94, 024614 (2016)

Q.Ducasse, B.Jurado, M.Aiche, P.Marini, L.Mathieu, A.Gorgen, M.Guttormsen, A.C.Larsen, T.Tornyi, J.N.Wilson, G.Barreau, G.Boutoux, S.Czajkowski, F.Giacoppo, F.Gunsing, T.W.Hagen, M.Lebois, J.Lei, V.Meot, B.Morillon, A.M.Moro, T.Renstrom, O.Roig, S.J.Rose, O.Serot, S.Siem, I.Tsekhanovich, G.M.Tveten, M.Wiedeking

Investigation of the 238U (d, p) surrogate reaction via the simultaneous measurement of γ-decay and fission probabilities

NUCLEAR REACTIONS 238U(d, p)239U*, E=15 MeV; measured particle spectra Eγ, Iγ, (proton)γ- and (proton)(fission events)-coin using ΔE/E silicon telescope SiRi for particles and CACTUS array for γ rays at Oslo Cyclotron Laboratory; corrected data using continuum-discretized coupled channels calculations for elastic breakup, and DWBA for inelastic breakup; deduced excitation energy of 239U versus detected γ-ray energy, ratio between the γ-coincidence and the singles spectra, average angular momentum, γ-decay and fission probabilities as function of excitation energy and compared with JENDL 4.0, ENDF-B/VII.1 and JEFF 3.2 evaluated libraries, and corresponding neutron-induced data; calculated contributions to the total deuteron breakup process (TB) as a function of the excitation energy of 239U. Statistical model calculations for decay probabilities and average angular momentum.

doi: 10.1103/PhysRevC.94.024614
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2016MO06      Acta Phys.Pol. B47, 821 (2016)

A.M.Moro, J.Lei, M.Gomez-Ramos, J.M.Arias, R.de Diego, J.Gomez-Camacho, J.A.Lay

Recent Developments for the Calculation of Elastic and Non-elastic Breakup of Weakly-bound Nuclei

doi: 10.5506/APhysPolB.47.821
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2016MO13      Few-Body Systems 57, 319 (2016)

A.M.Moro, J.Lei

Recent Advances in Nuclear Reaction Theories for Weakly Bound Nuclei: Reexamining the Problem of Inclusive Breakup

NUCLEAR REACTIONS 209Bi(6Li, 6Li), (6Li, α), E=30, 38 MeV; analyzed available σ data; deduced Elastic (EBU), non-elastic (NEB) and total breakup (TBU=EBU+NEB) and complete fusion (CF) σ, Eα, Iα. Comparison with available data.

doi: 10.1007/s00601-016-1085-1
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2015LE15      Phys.Rev. C 92, 044616 (2015)

J.Lei, A.M.Moro

Reexamining closed-form formulae for inclusive breakup: Application to deuteron- and 6Li-induced reactions

NUCLEAR REACTIONS 93Nb(d, pX), E=25.5 MeV; 58Ni(d, pX), E=80, 100 MeV; 209Bi(6Li, 6Li), (6Li, αX), E=24-50 MeV; calculated σ(θ) distributions, angle integrated proton differential σ(Ep) and double-differential σ(Ep), σ(θ) for α particles in 6Li+209Bi reactions, inclusive breakup σ. Comparison with experimental data. DWBA version of the coupled-channels optical theorem for the nonelastic breakup and continuum-discretized coupled-channels (CDCC) framework for the elastic breakup (EBU).

doi: 10.1103/PhysRevC.92.044616
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2015LE19      Phys.Rev. C 92, 061602 (2015)

J.Lei, A.M.Moro

Numerical assessment of post-prior equivalence for inclusive breakup reactions

NUCLEAR REACTIONS 62Ni(d, pX), E=25.5 MeV; calculated angle-integrated energy differential σ(Ep), double differential σ as a function of the proton energy. 209Bi(6Li, αX), E=36 MeV; calculated angle-integrated energy differential σ(Eα), σ(θ) for α using several models under the general distorted-wave Born approximation (DWBA) approach. Comparison of results from different models, and with experimental data. Post-prior equivalence in the calculation of nonelastic breakup (NEB) cross sections.

doi: 10.1103/PhysRevC.92.061602
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2012LE15      Phys.Rev. C 86, 057602 (2012)

J.Lei, J.S.Wang, S.Mukherjee, Q.Wang, R.Wada, Y.Y.Yang, J.B.Chen, J.L.Hang, M.R.Huang, Z.Bai, P.Ma, S.L.Jin, J.B.Ma, Y.Li, M.H.Zhao

Quarter-point angle for light, weakly bound projectiles

NUCLEAR REACTIONS 208Pb(6He, 6He), E(cm)=19-40 MeV; 208Pb(7Li, 7Li), E(cm)=30-44 MeV; 208Pb(12C, 12C), E(cm)=60-200 MeV; 64Zn, 90Zr, 112,116Sn(6Li, 6Li), 58Ni(8B, 8B), 116Sn(7Li, 7Li), 209Bi(9Be, 9Be)181Ta, 208Pb(16O, 16O), E not given; calculated values of quarter-point angles; analyzed threshold anomaly. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.057602
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2012LE16      Phys.Rev. C 86, 057603 (2012)

J.Lei, J.S.Wang, S.Mukherjee, Q.Wang, R.Wada

Phenomenological formula of total reaction cross sections for low-energy systems

NUCLEAR REACTIONS 11B(12C, X), E=344.5 MeV; 12C(12C, X), E=180 MeV; 12C(12C, X), E=300 MeV; 12C(12C, X), E=360 MeV; 12C(16O, X), E=62 MeV; 16O(16O, X), E=75 MeV; 28Si(12C, X), E=65 MeV; 40Ca(12C, X), E=180 MeV; 28Si(13C, X), E=60 MeV; 28Si(16O, X), E=75 MeV; 58Ni(12C, X), E=344.5 MeV; 197Au(12C, X), E=344.5 MeV; 90Zr(12C, X), E=120 MeV; 58Ni(16O, X), E=40 MeV; 60Ni(16O, X), E=56 MeV; 62Ni(16O, X), E=70 MeV; 64Ni(16O, X), E=70 MeV; 208Pb(12C, X), E=96 MeV; 208Pb(16O, X), E=129.5 MeV; 27Al(6He, X), E=12 MeV; 58Ni(6He, X), E=9 MeV; 65Cu(6He, X), E=22.6 MeV; 27Al(6Li, X), E=10 MeV; 27Al(7Li, X), E=18 MeV; 27Al(9Be, X), E=32 MeV; 58Ni(6Li, X), E=14 MeV; 59Co(6Li, X), E=29.6 MeV; 64Zn(6Li, X), E=22 MeV; 58Ni(7Be, X), E=21.4 MeV; 64Zn(7Li, X), E=20 MeV; 120Sn(6He, X), E=17.4 MeV; 112Sn(6Li, X), E=25 MeV; 116Sn(6Li, X), E=26 MeV; 208Pb(6Li, X), E=35 MeV; 209Bi(6Li, X), E=36.9 MeV; 58Ni(8B, X), E=25.3 MeV; 197Au(6He, X), E=27 MeV; 208Pb(6He, X), E=27 MeV; analyzed total reaction cross sections. Presented phenomenological formula of total reaction cross sections. Wong formula.

doi: 10.1103/PhysRevC.86.057603
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