NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.Lei Found 32 matches. 2023LE12 Phys.Rev. C 108, 034612 (2023) 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
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
2023LI41 Phys.Rev. C 108, 024606 (2023) 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
2023LU10 Phys.Rev. C 108, 024612 (2023) 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
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
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
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
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
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
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
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
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
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
2020LE08 Phys.Rev. C 102, 014608 (2020) 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
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
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
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
2019LE01 Phys.Rev.Lett. 122, 042503 (2019) 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
2019LE17 Phys.Rev.Lett. 123, 232501 (2019) 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
2018LE02 Phys.Rev. C 97, 011601 (2018) 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
2018LE06 Phys.Rev. C 97, 034628 (2018) 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
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
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
2017LE02 Phys.Rev. C 95, 044605 (2017) 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
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
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
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
2016MO13 Few-Body Systems 57, 319 (2016) 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
2015LE15 Phys.Rev. C 92, 044616 (2015) 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
2015LE19 Phys.Rev. C 92, 061602 (2015) 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
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
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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