NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.Andrade Found 26 matches. 2023MA46 Universe 9, 438 (2023) J.Mas Ruiz, K.G.Zayas-Bazan, P.G.Zayas-Bazan, A.Huerta, J.Sastre-Hernandez, D.J.Marin-Lambarri, Lui.Acosta, E.Andrade, C.Solis, E.R.Chavez Lomeli Probing the Elastic Scattering Differential Cross Section for Al + p at Backward Angles in a Low Energy Regime NUCLEAR REACTIONS 27Al(p, p), E=0.8-2.1 MeV; measured reaction products; deduced σ(θ). Comparison with optical model calculations. The ion beam analysis of materials (IBA), IBANDL database. The 1 MV tandem accelerator facility model 4110Bo of the Accelerator Mass Spectrometry Laboratory (LEMA) located at the Physics Institute of the National Autonomous University of Mexico (IFUNAM).
doi: 10.3390/universe9100438
2023PA16 Phys.Rev. C 107, 064613 (2023) K.Palli, A.Pakou, A.M.Moro, P.D.O'Malley, L.Acosta, A.M.Sanchez-Benitez, G.Souliotis, E.F.Aguilera, E.Andrade, D.Godos, O.Sgouros, V.Soukeras, C.Agodi, T.L.Bailey, D.W.Bardayan, C.Boomershine, M.Brodeur, F.Cappuzzello, S.Carmichael, M.Cavallaro, S.Dede, J.A.Duenas, J.Henning, K.Lee, W.S.Porter, F.Rivero, W.von Seeger Quasielastic scattering of 7Be + natZr at sub- and near-barrier energies NUCLEAR REACTIONS Zr(7Be, X), E=20.6, 22.1, 23.7, 28.2 MeV; measured reaction product, charged particles, angular distributions; deduced quasielastic scattering σ(θ), total σ(E), optical model parameters. Optical model analysis. Comparison to phenomenological predictions and Continuum-Discretized Coupled-Channel (CDCC) calculations. Systematics of total fusion cross-sections for 7Li+59Co, 7Li+64Ni, 7Li+124Sn, 7Be+90Zr. Setup consisting of 4 silicon DSSD telescopes at Notre Dame FN tandem accelerator.
doi: 10.1103/PhysRevC.107.064613
2022CH34 Nucl.Instrum.Methods Phys.Res. B526, 77 (2022) E.Chavez, V.Araujo-Escalona, J.Mas-Ruiz, L.Acosta, E.Andrade, L.Barron-Palos, R.J.R.Gleason, A.Huerta, M.Rodriguez-Ceja, D.J.Marin-Lambarri, C.G.Mendez, S.Padilla, C.Solis, A.O.Valdez-Guerrero Accelerator Mass Spectrometry, an ultrasensitive tool to measure cross sections for stellar nucleosynthesis NUCLEAR REACTIONS 28Si(d, α), E=1-5 MeV; measured reaction products. 26Al, 10B, 14C; deduced the activation-AMS method. 5.5 MV CN-Van de Graaff accelerator at IFUNAM, the EN-Tandem accelerator at ININ.
doi: 10.1016/j.nimb.2022.06.016
2020AB10 Eur.Phys.J.Plus 135, 845 (2020) M.Abbasi, H.Panjeh, R.Perez, A.Deppman, E.Andrade II, F.Velasco, F.Guzman Heavy-ion-induced fission of 181Ta and 209Bi at intermediate energies by CRISP model NUCLEAR REACTIONS 181Ta, 209Bi(11B, X), E=125.7, 245.4, 146 MeV; analalyzed available data; calculated σ, mass-yield distributions using the CRISP code.
doi: 10.1140/epjp/s13360-020-00828-4
2019BA34 Phys.Rev. C 100, 024616 (2019) A.R.Balabekyan, G.S.Karapetyan, E.Andrade II, A.Deppman, S.V.Gaginyan, E.Melyan, J.R.Drnoyan, V.I.Zhemenik, J.Adam, L.Zavorka, A.A.Solnyshkin, V.M.Tsoupko-Sitnikov, J.Khushvaktov, E.B.Hernandez Fragment production in proton-induced reaction on 209Bi target at intermediate energy range NUCLEAR REACTIONS 209Bi(p, X)24Na/28Mg/42K/46Sc/47Ca/52Mn/56Co/57Ni/59Fe/65Zn/66Ga/69Ge/72Zn/72Ga/74As/75Se/76Br/88Y/89Zr/90Nb/93mMo/96Nb/96Tc/100Rh/106mAg/110mAg/113Sn/118mSb/119Te/119mTe/120mSb/121Te/121mTe/124Sb/127Sb/127Xe/131mTe/140La/148mPm/154Tb/169Lu/170Lu/172Lu/175Ta/185Ir/194Au/203Bi/205Bi/206Bi, E=660 MeV; measured reaction products, Eγ, Iγ, mass-yield distribution; deduced cross-sections, fissility as function of Z2/A, contribution of symmetric fission to total fission cross section as function of the total number of emitted neutrons, cross section ratios of residues from 660 and 600 MeV proton-induced reactions. Comparison with previous experimental data, and with theoretical model calculations using the CRISP code. Measurement performed at the phasotron of the Laboratory of Nuclear Problems at the Joint Institute of Nuclear Research (JINR, Dubna).
doi: 10.1103/PhysRevC.100.024616
2018AN03 J.Phys.(London) G45, 015105 (2018) E.Andrade, Jr., G.S.Karapetyan, A.Deppman, J.L.Bernal-Castillo, V.Guimaraes, A.R.Balabekyan, J.Adam, F.Garcia, F.Guzman Systematic study of fission modes in the proton-induced fission of actinide and pre-actinide NUCLEAR REACTIONS 241Am, 237Np, 238U(p, X), E=26.5, 62.9, 660 MeV; 232Th(p, X), E=6.5, 62.9, 190 MeV; 208Pb(p, X), E=190, 500, 1000 MeV; 197Au(p, X), E=190, 800 MeV; analyzed available data in the framework of the Random Neck Rupture Model; deduced the roles of the neutron excess and of the so called fissility parameter.
doi: 10.1088/1361-6471/aa9a0c
2018TU10 J.Phys.(London) G45, 115103 (2018) O.Tumbarell, F.Guzman, F.G.Velasco, J.L.Bernal-Castillo, O.Rodriguez, A.Samana, E.Andrade II, A.Deppman Calculation of the Coulomb barrier and the level density parameter at the fission saddle point in spallation nuclear reactions NUCLEAR REACTIONS 208Pb, 238U(p, X), E=1 GeV; calculated average values of the number of emitted particles as a function of the excitation energy of the initial residual nuclei, kinetic energy distribution of the emitted particles, considering fission.
doi: 10.1088/1361-6471/aae3d7
2017VA26 Phys.Rev. C 96, 054606 (2017) D.Vargas, A.R.Samana, F.G.Velasco, O.R.Hoyos, F.Guzman, J.L.Bernal-Castillo, E.Andrade II, R.Perez, A.Deppman, C.A.Barbero, A.E.Mariano Nuclear medium effects in muonic neutrino interactions with energies from 0.2 to 1.5 GeV NUCLEAR REACTIONS 2H, 12C, 16O, 27Al, 40Ar, 56Fe, 208Pb(ν, X), E=0.2-1.5 GeV; calculated σ(E) data, energy distributions for π+ and μ- spectra in the framework of Monte Carlo calculation in the intranuclear cascade model. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.054606
2015AN16 Phys.Rev. C 92, 064903 (2015) E.Andrade II, I.Gonzalez, A.Deppman, C.A.Bertulani Evidence of subnucleonic degrees of freedom in J/ψ photoproduction in ultraperipheral collisions at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.92.064903
2013DE14 Phys.Rev. C 87, 054604 (2013) A.Deppman, E.Andrade, II, V.Guimaraes, G.S.Karapetyan, N.A.Demekhina Photofission of 232Th and 238U at intermediate energies NUCLEAR REACTIONS 232Th, 238U(γ, F), E=50, 3500 MeV; measured Eγ, Iγ; deduced yield, charge and mass distributions of fragments, fissility parameter. Data for fission fragment distributions analyzed by Monte Carlo calculations using CRISP code.
doi: 10.1103/PhysRevC.87.054604
2013DE25 Phys.Rev. C 88, 024608 (2013) A.Deppman, E.Andrade, II, V.Guimaraes, G.S.Karapetyan, A.R.Balabekyan, N.A.Demekhina Proton-induced fission on 241Am, 238U, and 237Np at intermediate energies NUCLEAR REACTIONS 237Np, 238U, 241Am(p, F), E=660 MeV; calculated fission σ vs fragment mass, fissility, number of nucleons evaporated by the nuclei before and after fission. Intermediate energy proton-induced fission. Monte-Carlo method using computer code CRISP and Bohr-Wheeler model. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.024608
2013DE37 Phys.Rev. C 88, 064609 (2013) A.Deppman, E.Andrade, II, V.Guimaraes, G.S.Karapetyan, O.A.P.Tavares, A.R.Balabekyan, N.A.Demekhina, J.Adam, F.Garcia, K.Katovsky Superasymmetric fission of heavy nuclei induced by intermediate-energy protons NUCLEAR REACTIONS 237Np, 238U(p, F)28Mg/34mCl/38S/38Cl/39Cl/41Ar/42K/43K/43Sc/44Ar/44K/44Sc/44mSc/45K/46Sc/46mSc/47Ca/47Sc/48Sc/48V/48Cr/49Cr/51Cr/52Mn/52mMn/52Fe/54Mn/55Co/56Mn/56Co/56Ni/57Co/57Ni/58Co/58mCo/59Fe/60Co/60mCo/60Cu/61Cu/65Ni/65Zn/65Ga/66Ni/66Ga/66Ge/67Cu/67Ga/69mZn/69Ge, E=660 MeV; measured Eγ, Iγ, production σ of intermediate-mass fragments (IMF) by induced activation method at LNR Phasotron-JINR cyclotron facility. A total of 93 isotopes in A=30-200 range identified with high precision. Comparison with simulation code CRISP for multimodal fission. Discussed superasymmetric fragment production mechanism.
doi: 10.1103/PhysRevC.88.064609
2011AN29 J.Phys.:Conf.Ser. 312, 082010 (2011) E.Andrade, II, J.C.M.Menezes, S.B.Duarte, F.Garcia, P.C.R.Rossi, O.A.P.Tavares, A.Deppman Fragment mass distributions for heavy nuclei fission induced by intermediate energy probes NUCLEAR REACTIONS 237Np, 241Am(p, F), E=660 MeV;238U(γ, F), E=0-50 MeV; calculated mass distribution from bremsstrahlung reaction using Monte Carlo for nuclear cascade followed by competition between fission and particle emission. Compared with data and other calculations.
doi: 10.1088/1742-6596/312/4/082010
1996MC09 Nucl.Instrum.Methods Phys.Res. B118, 219 (1996) L.C.McIntyre, Jr., J.A.Leavitt, M.D.Ashbaugh, J.Borgardt, E.Andrade, J.Rickards, A.Oliver Cross Section Measurements for the (3He, p) Nuclear Reaction on B and N between 2 and 4 MeV NUCLEAR REACTIONS 10,11B, 14N(3He, p), E=2-4 MeV; measured σ(Ep, θ).
doi: 10.1016/0168-583X(95)01074-2
1991AP02 Nucl.Instrum.Methods Phys.Res. B56/57, 799 (1991); see 1991Ap03 L.M.Apatiga, E.Andrade, J.Rickards, E.Belmont, F.Alba A Nuclear Reaction Study of Nitrogen Diffusion into Titanium and Its Relation to Microhardness
doi: 10.1016/0168-583X(91)95031-8
1991AP03 Nucl.Instrum.Methods Phys.Res. B56/57, 799 (1991) L.M.Apatiga, E.Andrade, J.Rickards, E.Belmont, F.Alba A Nuclear Reaction Study of Nitrogen Diffusion Into Titanium and Its Relation to Microhardness NUCLEAR REACTIONS 14N(d, α), E=2.6 MeV; measured σ(θ=170°); deduced N diffusion into Ti. Commercial drill coated with TiN.
doi: 10.1016/0168-583X(91)95031-8
1988PA22 Phys.Rev. C38, 2716 (1988) P.V.Pancella, G.S.Mutchler, S.D.Baker, J.W.Kruk, I.M.Duck, M.D.Corcoran, G.C.Phillips, J.M.Clement, J.A.Buchanan, B.W.Mayes, L.S.Pinsky, W.von Witsch, E.Andrade, H.Garcilazo, J.M.Laget Measurement of π+d → Δ++n at Intermediate Energy NUCLEAR REACTIONS 2H(π+, π+p), E at 312-600 MeV/c; measured σ(θ(π), θ(p)) vs pion momentum; deduced σ(θ) for reaction 2H(π+, Δ++).
doi: 10.1103/PhysRevC.38.2716
1980AN06 Nucl.Phys. A337, 365 (1980) E.Andrade, D.Miljanic, G.C.Phillips Analysis of Angular Distribution of Proton-Neutron FSI in the Reaction 2H(p, pn)1H at E = 12.5 MeV NUCLEAR REACTIONS 2H(p, pn), E=12.5 MeV; measured pn-coin; deduced angular dependence of final state interaction. Watson-Migdal, exact three-body models.
doi: 10.1016/0375-9474(80)90148-7
1980OR03 Phys.Rev. C22, 1104 (1980) M.E.Ortiz, E.Andrade, M.Cardenas, A.Dacal, A.Menchaca-Rocha, J.L.C.Ford, Jr., J.G.del Campo, R.L.Robinson, D.Shapira, E.Aguilera Nonstatistical Effects in the 12C(15N, α) Reaction NUCLEAR REACTIONS 12C(15N, α), E=21.4-39 MeV; 12C(15N, 15N), E=22-31.8 MEV; measured σ(E, θ); deduced nonstatistical effects. 27Al deduced high-spin resonances. Hauser-Feshbach formalism, fluctuation, single-level analysis.
doi: 10.1103/PhysRevC.22.1104
1978GO06 Nucl.Phys. A297, 125 (1978) J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, M.E.Ortiz, A.Dacal, E.Andrade Coherence Widths in 27Al Measured with the 12C(15N, α) Reaction NUCLEAR REACTIONS 12C(15N, α), E=21.4-39.0 MeV; measured σ(E) at θ=7°. 27Al deduced coherence widths, effective moment of inertia. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(78)90202-6
1977GO08 Phys.Lett. 69B, 415 (1977) J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, M.E.Ortiz, A.Dacal, E.Andrade Yrast Levels in 27Al Suggested by Resonance Structure in the 12C(15N, α) Reaction NUCLEAR REACTIONS 12C(15N, α), E=21.4-39.0 MeV; measured σ(E, Eα). 27Al deduced resonances.
doi: 10.1016/0370-2693(77)90833-4
1977MI13 Nucl.Phys. A290, 27 (1977) D.Miljanic, E.Andrade, J.Hudomalj-Gabitzsch, G.S.Mutchler, G.C.Phillips Mechanisms in d + 6Li Three-Body Reactions at Low Bombarding Energies NUCLEAR REACTIONS 6Li(d, 2d), (d, dα), (d, pt), (d, pα), (d, tα), E=7.5, 9, 10, 10.5 MeV; measured (E;E1, E2, θ1, θ2); deduced reaction mechanisms. Enriched target.
doi: 10.1016/0375-9474(77)90662-5
1974MI10 Phys.Lett. 50B, 330 (1974) D.Miljanic, J.Hudomalj, G.S.Mutchler, E.Andrade, G.C.Phillips Quasi-Free Contributions in the d + 6Li Reactions at Low Energies NUCLEAR REACTIONS 6Li(d, 2d), (d, αd), (d, tp), E=7.5-10.5 MeV; measured σ, deduced reaction mechanism.
doi: 10.1016/0370-2693(74)90682-0
1973AN25 Nucl.Instrum.Methods 113, 93 (1973) E.Andrade, D.Rendic, V.A.Otte, G.C.Phillips Charged Particle Mass Identification by Energy-Time-of-Flight Technique NUCLEAR REACTIONS 12C(d, X), E=12 MeV; measured σ(E(X), mass(X)).
doi: 10.1016/0029-554X(73)90483-7
1972AN02 Nucl.Phys. A183, 145 (1972) E.Andrade, V.Valkovic, D.Rendic, G.C.Phillips Angular Distributions of Quasi-Free Scattering Contributions in Deuteron Break-up by Protons and Deuterons NUCLEAR REACTIONS 2H(p, pn), E=12.5 MeV; 2H(d, pn), E=12.5 MeV; measured σ(E(p1), E(p2), Ep, En, θ(1)=-θ(2)=15-60°), (Ed, Ep, Ed, En, θ(1)=-θ(2)=15-40°).
doi: 10.1016/0375-9474(72)90935-9
1971VA28 Phys.Rev. C4, 2289 (1971) V.Valkovic, I.M.Duck, W.E.Sweeney, Jr., E.Andrade, G.C.Phillips Nuclear-Deuteron Quasifree Scattering in the Reaction d + d → d + p + n at Low Bombarding Energies NUCLEAR REACTIONS 2H(d, np), E=6-13 MeV; measured σ(E;Ed, En, θ(d), θ(n)), σ(E;Ed, Ep, θ(d), θ(p)).
doi: 10.1103/PhysRevC.4.2289
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