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NSR database version of May 24, 2024.

Search: Author = E.Andrade

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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1410.


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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1232.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0229.


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
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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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0651.


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
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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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1049.


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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