NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.D.Arruda-Neto Found 72 matches. 2012RO28 Phys.Rev. C 86, 037601 (2012) T.E.Rodrigues, J.D.T.Arruda-Neto Forward-angle incoherent photoproduction of pseudoscalar mesons off nuclei
doi: 10.1103/PhysRevC.86.037601
2011RO34 Phys.Rev. C 84, 021601 (2011) T.E.Rodrigues, J.D.T.Arruda-Neto Attenuation of ω mesons in cold nuclear matter
doi: 10.1103/PhysRevC.84.021601
2010RO24 Phys.Rev. C 82, 024608 (2010) T.E.Rodrigues, J.D.T.Arruda-Neto, J.Mesa, C.Garcia, K.Shtejer, D.Dale, I.Nakagawa, P.L.Cole Nuclear incoherent photoproduction of π0 and η from 4 to 12 GeV
doi: 10.1103/PhysRevC.82.024608
2007RO02 Phys.Rev. C 75, 014605 (2007) T.E.Rodrigues, M.N.Martins, C.Garcia, J.D.T.Arruda-Neto, J.Mesa, K.Shtejer, F.Garcia Photon-induced multiple particle emissions of 90Zr and natZr from 10 to 140 MeV NUCLEAR REACTIONS Zr, 90Zr(γ, xnyp), E=10-140 MeV; calculated photoabsorption σ, particle emission branching ratios, giant resonance and quasideuteron contributions. Multicollisional Monte Carlo approach, comparisons with data.
doi: 10.1103/PhysRevC.75.014605
2006AR17 Phys.Rev. C 74, 034324 (2006) J.D.T.Arruda-Neto, J.Mesa, F.Garcia, O.Rodriguez, L.P.Geraldo, C.Garcia, T.E.Rodrigues, K.Shtejer, R.Semmler, F.Guzman Role of transitional levels in 237Np(γ, f): Perspectives for studying highly deformed systems NUCLEAR REACTIONS 237Np(γ, F), E ≈ 5-7 MeV; analyzed photofission σ; calculated fission barrier surfaces, transition levels. Semimicroscopic combined method.
doi: 10.1103/PhysRevC.74.034324
2005RO13 Phys.Rev. C 71, 051603 (2005) T.E.Rodrigues, J.D.T.Arruda-Neto, J.Mesa, C.Garcia, K.Shtejer, D.Dale, I.Nakagawa Incoherent π0 photoproduction from complex nuclei NUCLEAR REACTIONS 12C, 208Pb(γ, π0X), E=0.33, 5.0, 5.5, 6.0 GeV; calculated σ(θ), in-medium effects. Muticollisional intranuclear cascade framework, comparisons with data.
doi: 10.1103/PhysRevC.71.051603
2004LI78 Braz.J.Phys. 34, 753 (2004) V.P.Likhachev, J.D.T.Arruda-Neto, M.T.F.da Cruz, H.Dias, S.B.Duarte, W.R.Carvalho, Jr., M.S.Hussein, A.C.S.Lima, L.F.R.Macedo, J.Mesa, S.A.Pashchuk, T.E.Rodrigues, G.Silva, H.R.Schelin, O.A.P.Tavares Residual Nucleus Excitation Energy in (e, e'p)- Reaction
doi: 10.1590/S0103-97332004000500012
2004RO22 Phys.Rev. C 69, 064611 (2004) T.E.Rodrigues, J.D.T.Arruda-Neto, A.Deppman, V.P.Likhachev, J.Mesa, C.Garcia, K.Shtejer, G.Silva, S.B.Duarte, O.A.P.Tavares Photonuclear reactions at intermediate energies investigated via the Monte Carlo multicollisional intranuclear cascade model NUCLEAR REACTIONS Sn, Ce, Ta, Pb(γ, X), E=20-140 MeV; calculated total photoabsorption σ, neutron multiplicities. Monte Carlo multicollisional intranuclear cascade model, comparison with data.
doi: 10.1103/PhysRevC.69.064611
2003DE20 Nucl.Instrum.Methods Phys.Res. B211, 15 (2003) A.Deppman, O.A.P.Tavares, S.B.Duarte, J.D.T.Arruda-Neto, M.Goncalves, V.P.Likhachev, J.Mesa, E.C.de Oliveira, S.R.de Pina, O.Rodriguez A Monte Carlo method for nuclear evaporation and fission at intermediate energies NUCLEAR STRUCTURE 237Np, 238U, 232Th; calculated fissility vs excitation energy, competition with evaporation channels. Monte Carlo approach.
doi: 10.1016/S0168-583X(03)01265-5
2003LI01 Nucl.Phys. A713, 24 (2003) V.P.Likhachev, J.Mesa, J.D.T.Arruda-Neto, B.V.Carlson, W.R.Carvalho, Jr., L.C.Chamon, A.Deppman, H.Dias, M.S.Hussein Quasi-free 238U(e, e'f) cross section in macroscopic-microscopic approach NUCLEAR REACTIONS 238U(e, e'X), E=720 MeV; calculated quasifree electrofission σ(E, θ). Comparison with data. NUCLEAR STRUCTURE 238U; calculated single-particle level energies. 237,238U, 237Pa; calculated fissility vs excitation energy.
doi: 10.1016/S0375-9474(02)01302-7
2003LI25 Phys.Rev. C 68, 014615 (2003) V.P.Likhachev, J.D.T.Arruda-Neto, W.R.Carvalho, Jr., A.Deppman, I.G.Evseev, F.Garcia, M.S.Hussein, L.F.R.Macedo, A.Margaryan, J.Mesa, V.O.Nesterenko, O.Rodriguez, S.A.Pashchuk, H.R.Schelin, M.S.Vaudeluci Inclusive quasifree electrofission cross section for 238U NUCLEAR STRUCTURE 237,238U, 237Pa; calculated fissility vs excitation energy. NUCLEAR REACTIONS 238U(e, e'p), (e, e'), E=300 MeV; calculated σ(E, θ). 238U(e, F), E=100-250 MeV; measured fission σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.68.014615
2003ME28 Phys.Rev. C 68, 054608 (2003) J.Mesa, J.D.T.Arruda-Neto, A.Deppman, V.P.Likhachev, M.V.Manso, C.E.Garcia, O.Rodriguez, F.Guzman, F.Garcia New calculation for the neutron-induced fission cross section of 233Pa between 1.0 and 3.0 MeV NUCLEAR REACTIONS 233Pa(n, F), E=1-3 MeV; calculated fission σ. Comparison with data. NUCLEAR STRUCTURE 234Pa; calculated potential energy surfaces, level densities.
doi: 10.1103/PhysRevC.68.054608
2003NE06 J.Phys.(London) G29, L37 (2003) V.O.Nesterenko, V.P.Likhachev, P.-G.Reinhard, J.Mesa, W.Kleinig, J.D.T.Arruda-Neto, A.Deppman Deformation effects in low-momentum distributions of heavy nuclei NUCLEAR STRUCTURE 238U; calculated momentum distributions of deep hole proton states, ground-state quadrupole moments. Comparison of Woods-Saxon and Skyrme-Hartree-Fock approaches.
doi: 10.1088/0954-3899/29/4/101
2003RO12 Phys.Rev. C 68, 014618 (2003) T.E.Rodrigues, J.D.T.Arruda-Neto, Z.Carvalheiro, J.Mesa, A.Deppman, V.P.Likhachev, M.N.Martins Statistical and direct aspects of 64Zn(γ, n) and (γ, np) decay channels in the giant dipole resonance and quasideuteron energy regions NUCLEAR REACTIONS 64Zn(e, n), (e, np), E=12.5-60 MeV; measured σ. 64Zn(γ, n), (γ, np), E=10-60 MeV; deduced σ. Comparison with previous results.
doi: 10.1103/PhysRevC.68.014618
2002DE35 J.Phys.(London) G28, 2259 (2002) S.R.de Pina, J.Mesa, A.Deppman, J.D.T.Arruda-Neto, S.B.Duarte, E.C.de Oliveira, O.A.P.Tavares, E.L.Medeiros, M.Goncalves, E.de Paiva Nucleon Effective Mass Effects on the Pauli-Blocking Function
doi: 10.1088/0954-3899/28/8/311
2002DE60 Phys.Rev. C 66, 067601 (2002) A.Deppman, O.A.P.Tavares, S.B.Duarte, J.D.T.Arruda-Neto, M.Goncalves, V.P.Likhachev, E. C.de Oliveira Photofissility of heavy nuclei at intermediate energies NUCLEAR REACTIONS 209Bi, 232Th, 238U, 237Np, 243Am(γ, F), E=200-1000 MeV; calculated fissility. 209Bi, 243Am(γ, F), E=200-1000 MeV; calculated photofission σ. Monte Carlo approach.
doi: 10.1103/PhysRevC.66.067601
2002LI23 Phys.Rev. C65, 044611 (2002) V.P.Likhachev, J.Mesa, J.D.T.Arruda-Neto, B.V.Carlson, A.Deppman, M.S.Hussein, V.O.Nesterenko, F.Garcia, O.Rodriguez Quasifree Electrofission of 238U NUCLEAR REACTIONS 238U(e, e'p), E=2 GeV; calculated σ(E, θ), residual nucleus fissility.
doi: 10.1103/PhysRevC.65.044611
2001DE41 Phys.Rev.Lett. 87, 182701 (2001) A.Deppman, O.A.P.Tavares, S.B.Duarte, E.C.de Oliveira, J.D.T.Arruda-Neto, S.R.de Pina, V.P.Likhachev, O.Rodriguez, J.Mesa, M.Goncalves Photofissility of Actinide Nuclei at Intermediate Energies NUCLEAR REACTIONS 237Np, 238U, 232Th(γ, F), E ≈ 200-1000 MeV; analyzed fissility; deduced role of proton and α evaporation. Monte Carlo approach.
doi: 10.1103/PhysRevLett.87.182701
2001GA70 Eur.Phys.J. A 12, 487 (2001) V.B.Gavrikov, V.P.Likhachev, J.D.T.Arruda-Neto, A.L.Bonini Incoherent X-Radiation Produced by Relativistic Electrons in Crystals
doi: 10.1007/s10050-001-8671-3
2001RO18 Comput.Phys.Commun. 137, 405 (2001) O.Rodriguez, F.Garcia, H.Dias, J.Mesa, J.D.T.Arruda-Neto, E.Garrote, F.Guzman LINDEN: Code for level density calculations of deformed nuclei using Lipkin-Nogami projectors in the BCS approach NUCLEAR STRUCTURE 233U; calculated levels, J, π. Lipkin-Nogami pairing model, comparison with data.
2001SH46 Braz.J.Phys. 31, 327 (2001) V.B.Shostak, G.P.Palkin, N.I.Woloshin, V.P.Likhachev, J.D.T.Arruda-Neto, M.T.F.da Cruz, M.N.Martins Analysis of the Ratio of (p, pn) to (p, 2p) Reaction Cross Sections NUCLEAR REACTIONS 7Li(p, 2p), (p, np), E=70 MeV; analyzed σ(E, θ), final-state interactions and off-shell effects. Distorted-wave approximation, non-local realistic t-matrix.
doi: 10.1590/s0103-97332001000200028
2000GE17 Nucl.Sci.Eng. 136, 357 (2000) L.P.Geraldo, R.Semmler, O.L.Goncalez, J.Mesa, J.D.T.Arruda-Neto, F.Garcia, O.Rodriguez Photofission Cross Sections for 237Np in the Energy Interval from 5.27 to 10.83 MeV NUCLEAR REACTIONS 237Np(γ, F), E=5.27-10.83 MeV; measured photofission σ. Comparison with previous data, model predictions.
doi: 10.13182/NSE00-A2164
2000SH01 Phys.Rev. C61, 024601 (2000) V.B.Shostak, G.P.Palkin, N.I.Voloshin, V.P.Likhachev, M.N.Martins, J.D.T.Arruda-Neto Study of 9Be(p, pn) and 9Be(p, 2p) Reactions at 70 MeV NUCLEAR REACTIONS 9Be(p, np), (p, 2p), E=70 MeV; measured proton spectra, neutron spectra, pp-, np-coin, σ(E, θ); deduced 1s and 1p shell contributions. 8Be deduced radius. Comparisons with neighboring nuclides.
doi: 10.1103/PhysRevC.61.024601
1999DE35 Eur.Phys.J. A 6, 107 (1999) Investigation of Low Energy Pion-Nucleus Interaction using Electrofission Data for Heavy Nuclei at the Pion Threshold NUCLEAR REACTIONS 182W(e, F), (γ, F), E=100-200 MeV; calculated fission σ; deduced two-, three-nucleon pion reabsorption contributions, sensitivity to pion mean free path.
doi: 10.1007/s100500050323
1999GA40 Eur.Phys.J. A 6, 49 (1999) F.Garcia, E.Garrote, M.-L.Yoneama, J.D.T.Arruda-Neto, J.Mesa, F.Bringas, J.F.Dias, V.P.Likhachev, O.Rodriguez, F.Guzman Woods-Saxon Potential Parametrization at Large Deformations for Plutonium Odd Isotopes NUCLEAR STRUCTURE 237,239,241Pu; calculated single-particle levels, J, π, deformation; deduced spin-orbit parameterization. Woods-Saxon potential.
doi: 10.1007/s100500050316
1999GA50 Phys.Rev. C60, 064311 (1999); Erratum Phys.Rev. C 80, 039903 (2009) F.Garcia, O.Rodriguez, F.Guzman, H.Dias, J.D.T.Arruda-Neto, M.S.Hussein, A.K.Kerman Particle-Hole Level Densities in Deformed Nuclei NUCLEAR STRUCTURE 233Th, 239U; calculated potential energy surfaces, particle-hole level densities; deduced deformation effects. Microscopic combinatorial approach.
doi: 10.1103/PhysRevC.60.064311
1999LI02 Phys.Rev. C59, 525 (1999) V.P.Likhachev, M.N.Martins, M.T.F.da Cruz, J.D.T.Arruda-Neto, L.P.Geraldo, R.Semmler, J.F.Dias Triton Angular Distributions from the 7Li(γ, t)α Reaction Near Threshold NUCLEAR REACTIONS 7Li(γ, t), E=6.4-6.7, 8.5-9.0 MeV; measured tritons σ(E, θ). Comparison with binary cluster model.
doi: 10.1103/PhysRevC.59.525
1998AR13 Nucl.Phys. A638, 701 (1998) J.D.T.Arruda-Neto, S.Simionatto, V.P.Likhachev, F.Garcia, J.Mesa, A.Deppman, O.Rodriguez, F.Guzman Photoneutron Multiplicities of Preactinide Nuclei at Energies Above the Pion Threshold NUCLEAR REACTIONS Ce, Sn, Pb, Ta, 197Au, 182W(γ, X), E < 250 MeV; analyzed average neutron multiplicities; deduced pion reabsorption role.
doi: 10.1016/S0375-9474(98)00215-2
1998LI07 Nucl.Phys. A628, 597 (1998) V.P.Likhachev, M.N.Martins, Yu.A.Kasatkin, M.T.F.da Cruz, J.D.T.Arruda-Neto, V.B.Shostak, V.V.Denyak, I.G.Evseev, S.A.Paschuk, V.M.Khvastunov Disintegration of the Deuteron by Linearly Polarized Photons at Low Energies NUCLEAR REACTIONS 2H(polarized γ, p), E=5-10 MeV bremsstrahlung; measured σ(θ), asymmetry following disintegration. Model comparison.
doi: 10.1016/S0375-9474(97)00620-9
1998SH33 Nucl.Phys. A643, 3 (1998) V.B.Shostak, G.P.Palkin, N.I.Voloshin, V.P.Likhachev, J.D.T.Arruda-Neto, M.T.F.da Cruz, M.N.Martins Study of 7Li(p, pn) and 7Li(p, 2p) Reactions at 70 MeV NUCLEAR REACTIONS 7Li(p, 2p), (p, np), E=70 MeV; measured σ(Ep, θ(1), θ(2)); deduced off-shell, final state interaction effects. Distorted wave approximation, realistic T-matrix.
doi: 10.1016/S0375-9474(98)00551-X
1997AR09 Phys.Rev. C55, 2471 (1997) J.D.T.Arruda-Neto, M.-L.Yoneama, J.F.Dias, F.Garcia, M.A.V.Reigota, V.P.Likhachev, F.Guzman, O.Rodriguez, J.Mesa Electrofission of 239Pu in the Energy Range 7-12 MeV NUCLEAR REACTIONS 239Pu(e, F), E=7-12 MeV; measured fission σ(E). 239Pu deduced levels M1 fission strength. Enriched target. DWBA, virtual phonon analyses.
doi: 10.1103/PhysRevC.55.2471
1997DE52 Nucl.Instrum.Methods Phys.Res. A384, 516 (1997) A.Deppman, J.D.T.Arruda-Neto, M.V.Tavares A New and Simple Method to Unfold Electroexcitation Cross Sections at Intermediate Energies NUCLEAR REACTIONS 182W(e, F), E=130-160 MeV; analyzed σ. Deconvolution method, DWBA.
doi: 10.1016/S0168-9002(96)00841-8
1996AR14 Phys.Rev. C54, 3294 (1996) J.D.T.Arruda-Neto, T.Saito, M.Sugawara, T.Tamae, H.Miyase, K.Abe, O.Konno, M.Oikawa, S.Simionatto, M.L.Yoneama, J.F.Dias, A.Deppman, B.S.Bhandari, V.P.Likhachev, A.C.S.Lima Photoexcitation Mechanisms Investigated Through the Fission Channel NUCLEAR REACTIONS 182W, 197Au, Ta(e, F), E not given; analyzed fission data; deduced σ(γ, F), compound nucleus excitation energy delineation related features.
doi: 10.1103/PhysRevC.54.3294
1996DE59 Nuovo Cim. 109A, 1197 (1996) A.Deppman, J.D.T.Arruda-Neto, E.De Sanctis, N.Bianchi Clustering-Related Aspects in the Compound Nucleus Formation NUCLEAR STRUCTURE 238U, 232Th; analyzed photofissility data; deduced cluster preformation probability. Intranuclear cascade with preformed clusters incorporated.
doi: 10.1007/BF02798822
1996LI59 Nucl.Instrum.Methods Phys.Res. A376, 455 (1996) V.P.Likhachev, J.F.Dias, M.-L.Yoneama, M.N.Martins, J.D.T.Arruda-Neto, C.C.Bueno, V.Perevertailo, O.Frolov Silicon Strip Detectors for Fission RADIOACTIVITY 252Cf(SF); measured fission fragment spectra. 241Am(α); measured α-spectra; deduced silicon strip detector performance characteristics.
doi: 10.1016/0168-9002(96)00275-6
1996YO04 Nucl.Phys. A604, 263 (1996) M.-L.Yoneama, E.Jacobs, J.D.T.Arruda-Neto, B.S.Bhandari, D.De Frenne, S.Pomme, K.Persyn, K.Govaert Study of the 232Th Fission Barrier by Electron-Induced Fission NUCLEAR REACTIONS 232Th(e, F), E=4.5-7.9 MeV; measured electron induced σ, α(θ); deduced photofission σ for (1-, 0), (1-, 1), (2+0) channels, isomer fission, fission barrier.
doi: 10.1016/0375-9474(96)00159-5
1995AR03 Phys.Rev. C51, R452 (1995) J.D.T.Arruda-Neto, T.Saito, M.Sugawara, T.Tamae, H.Miyase, K.Abe, O.Konno, M.Oikawa, A.Deppman, S.Simionatto, E.M.L.Macedo, B.S.Bhandari Photofission of 182W following Reabsorption of Photopions NUCLEAR REACTIONS 182W(e, F), E=80-180 MeV; measured fission σ(E); deduced σ(γ, F), pion reabsorption σ. Enriched targets.
doi: 10.1103/PhysRevC.51.R452
1995AR04 Phys.Rev. C51, 751 (1995) J.D.T.Arruda-Neto, A.Deppman, N.Bianchi, E.De Sanctis Nuclear Photofissility at Intermediate and High Energies NUCLEAR REACTIONS 232Th, 238U(γ, F), E=300-1200 MeV; analyzed fission data. 232Th deduced fissility nonsaturation features. Intranuclear cascade Monte Carlo, statistical models.
doi: 10.1103/PhysRevC.51.751
1994AR01 J.Phys.(London) G20, 197 (1994) J.D.T.Arruda-Neto, T.Saito, M.Sugawara, T.Tamae, H.Miyase, K.Abe, K.Takahisa, O.Konno, M.Oikawa, S.Simionatto Observation of Fine Thermalization Effects in the Electrofission of Preactinde Nuclei NUCLEAR REACTIONS 197Au, Ta(e, F), E=40-250 MeV; measured fission σ; deduced photofission σ, thermalization process features.
doi: 10.1088/0954-3899/20/1/019
1994AR12 Phys.Rev. C50, 282 (1994) J.D.T.Arruda-Neto, T.Saito, M.Sugawara, T.Tamae, H.Miyase, K.Abe, K.Takahisa, O.Konno, M.Oikawa, A.Deppman, S.Simionatto Thermalizatioon Related Effects in the Electrofission of Preactinide Nuclei NUCLEAR REACTIONS 197Au, Ta(e, F), E=40-250 MeV; measured fission σ(E); deduced photofission σ. Intranuclear cascade model analysis.
doi: 10.1103/PhysRevC.50.282
1993AR10 Phys.Rev. C48, 1594 (1993) J.D.T.Arruda-Neto, T.Saito, M.Sugawara, T.Tamae, H.Miyase, K.Abe, K.Takahisa, O.Konno, M.Oikawa, S.Simionatto Observation of Pion-Related Effects in the Photofission of Preactinide Nuclei NUCLEAR REACTIONS 197Au, Ta(e, F), E=25-180 MeV; measured absolute fission σ(E); deduced photofission σ, photofissility. Natural targets.
doi: 10.1103/PhysRevC.48.1594
1993BI16 Phys.Rev. C48, 1785 (1993) N.Bianchi, A.Deppman, E.De Sanctis, A.Fantoni, P.Levi Sandri, V.Lucherini, V.Muccifora, E.Polli, A.R.Reolon, P.Rossi, A.S.Iljinov, M.V.Mebel, J.D.T.Arruda-Neto, M.Anghinolfi, P.Corvisiero, G.Gervino, L.Mazzaschi, V.Mokeev, G.Ricco, M.Ripani, M.Sanzone, M.Taiuti, A.Zucchiatti, R.Bergere, P.Carlos, P.Garganne, A.Lepretre Photofissility of 232Th Measured with Tagged Photons from 250 to 1200 MeV NUCLEAR REACTIONS 232Th(γ, F), E=250-1200 MeV; measured photofission σ(E). 232Th deduced photofissility. Tagged photons, parallel plate avalanche detector.
doi: 10.1103/PhysRevC.48.1785
1991MI02 Phys.Rev. C43, 1677 (1991) R.A.Miskimen, E.A.Ammons, J.D.T.Arruda-Neto, G.O.Bolme, L.S.Cardman, P.L.Cole, J.R.Deininger, S.M.Dolfini, A.J.Linzey, J.B.Mandeville, B.L.Miller, P.E.Mueller, C.N.Papanicolas, A.Serdarevic, S.E.Williamson Use of the (e, e'n) Reaction to Study the Giant Multipole Resonances in 116Sn NUCLEAR REACTIONS 116Sn(e, e'n), E=68.3, 68.4, 99.4 MeV; measured σ(θn, En). 116Sn deduced giant multipole resonance EWSR strengths. Open-shell, continuum RPA.
doi: 10.1103/PhysRevC.43.1677
1990AR01 Phys.Rev. C41, 354 (1990) J.D.T.Arruda-Neto, M.Sugawara, H.Miyase, T.Kobayashi, T.Tamae, K.Abe, M.Nomura, H.Matsuyama, H.Kawahara, K.Namai, M.L.Yoneama, S.Simionatto Electrofission of 208Pb in the Intermediate Energy Region NUCLEAR REACTIONS 208Pb(e, F), E=35-250 MeV; measured fission σ(E); deduced σ(γ, F). Intranuclear cascade model, thermalization process.
doi: 10.1103/PhysRevC.41.354
1990AR22 Phys.Lett. 248B, 34 (1990) J.D.T.Arruda-Neto, E.Jacobs, D.De Frenne, S.Pomme Evidence for Isomeric Electron Induced Fission of 232Th NUCLEAR REACTIONS 232Th(e, F), E=4.54-6.64 MeV; measured fission fragment σ(θ), σ(E). 232Th deduced inner barrier height, fission isomer evidence.
doi: 10.1016/0370-2693(90)90010-4
1990MI03 Phys.Lett. 236B, 251 (1990) R.A.Miskimen, E.A.Ammons, J.D.T.Arruda-Neto, L.S.Cardman, P.L.Cole, J.R.Deininger, S.M.Dolfini, A.J.Linzey, J.B.Mandeville, B.L.Miller, P.E.Mueller, C.N.Papanicolas, A.Serdarevic, S.E.Williamson Coincidence Studies of the Giant Multipole Resonances in 116Sn Using the (e, e'n) Reaction NUCLEAR REACTIONS 116Sn(e, e'n), E ≤ 100 MeV; measured σ(θn) for fixed E, θ(e'). 116Sn deduced transition strengths in giant resonance region.
doi: 10.1016/0370-2693(90)90977-E
1989AR12 J.Phys.(London) G15, L215 (1989) J.D.T.Arruda-Neto, M.Sugawara, H.Miyase, T.Kobayashi, T.Tamae, K.Abe, M.Nomura, H.Matsuyama, H.Kawahara, K.Namai, M.L.Yoneama, S.Simionatto Electron-Induced Fission Decay from (Jπ, K) = (2+, 0) States in 208Pb NUCLEAR REACTIONS 208Pb(e, e'F), E=35 MeV; measured fission fragment σ(θ). 208Pb level deduced fission decay features.
doi: 10.1088/0954-3899/15/10/004
1989AR19 Phys.Scr. 40, 735 (1989) J.D.T.Arruda-Neto, S.Simionatto, S.B.Herdade, Z.Carvalheiro, M.L.Yoneama, B.L.Berman Electrofission of 233U NUCLEAR REACTIONS 233U(e, F), E=5.75-31 MeV; measured fission σ(E); deduced E2 photofission σ(E). 233U deduced M1 transition strength.
doi: 10.1088/0031-8949/40/6/006
1989DI02 Phys.Rev. C39, 564 (1989) H.Dias, J.D.T.Arruda-Neto, B.V.Carlson, M.S.Hussein Statistical Calculation of Fission Decay Probabilities of Nuclear Giant Multipole Resonances NUCLEAR STRUCTURE 236U; calculated giant resonance fission probabilities. Hauser-Feshbach model.
doi: 10.1103/PhysRevC.39.564
1988AR01 Phys.Rev. C37, 1326 (1988) E2(T = 0) Photofission of 236U and Statistical Calculations NUCLEAR REACTIONS 236U(γ, F), E=5.5-8 MeV; calculated isoscalar quadrupole fission σ(E).
doi: 10.1103/PhysRevC.37.1326
1988AR02 J.Phys.(London) G14, 373 (1988) J.D.T.Arruda-Neto, S.L.Paschoal, S.B.Herdade Electrofission of 237Np in the Energy Range 6-60 MeV NUCLEAR REACTIONS 237Np(e, F), E=6-60 MeV; measured fission σ(E). 237Np deduced E2, M1 fission strengths.
doi: 10.1088/0305-4616/14/3/013
1987AR10 Phys.Scr. 35, 427 (1987) J.D.T.Arruda-Neto, W.Rigolon, S.B.Herdade Evidence for the Statistical Fission Decay of the Giant Quadrupole Resonance of 232Th NUCLEAR REACTIONS 232Th(e, F), E=5.6-32 MeV; measured fission σ(E). 232Th deduced GQR fission decay characteristics. Mica foils.
doi: 10.1088/0031-8949/35/4/003
1986AR02 J.Phys.(London) G12, 105 (1986) J.D.T.Arruda-Neto, S.B.Herdade, B.L.Berman Observation of M1 Strength in the Photofission of Actinide Nuclei NUCLEAR REACTIONS 234,236,238U(e, F), E=5-7 MeV; measured fission σ(θ). 234,236,238U deduced photofission M1 transition strengths, parameters. Virtual photon formalism.
doi: 10.1088/0305-4616/12/2/009
1986AR11 Phys.Rev. C34, 935 (1986) J.D.T.Arruda-Neto, M.Sugawara, T.Tamae, O.Sasaki, H.Ogino, H.Miyase, K.Abe Photoexcitation Mechanisms and Fission of 209Bi from Threshold to the Δ Region NUCLEAR REACTIONS 209Bi(e, F), E=43-250 MeV; measured absolute fission σ(E); deduced photon induced fission σ(E). 209Bi deduced relative fission probability. Natural target.
doi: 10.1103/PhysRevC.34.935
1985AR04 J.Phys.(London) G11, 649 (1985) J.D.T.Arruda-Neto, S.B.Herdade, Z.Carvalheiro, S.Simionatto, B.L.Berman Non-Electric-Dipole Photofission of 235U NUCLEAR REACTIONS 235U(e, F), E=5.8-22 MeV; measured fission σ(E). 235U deduced non-E1 multipole component role in fission.
doi: 10.1088/0305-4616/11/5/011
1985AR08 Phys.Rev. C31, 2321 (1985) J.D.T.Arruda-Neto, M.Sugawara, T.Tamae, O.Sasaki, H.Ogino, H.Miyase, K.Abe Photoexcitation Mechanisms and the Fission Process of 209Bi from Threshold to the Δ Region NUCLEAR REACTIONS 209Bi(e, F), E=43-250 MeV; measured fission σ(E); deduced σ(γ, F). 209Pb deduced relative fission probability. 209Bi deduced fission process, photoexcitation mechanism. Natural target.
doi: 10.1103/PhysRevC.31.2321
1985AR21 Acta Phys.Pol. B16, 963 (1985) E2-Fission Decay of 232Th NUCLEAR REACTIONS 232Th(α, α'F), E not given; analyzed fission. 232Th deduced isoscalar GQR decay inconsistencies. Other reaction data input.
1985WO03 Phys.Lett. 153B, 226 (1985) J.G.Woodworth, D.Rowley, J.D.T.Arruda-Neto, P.J.Countryman, K.A.Griffioen, D.H.H.Hoffmann, K.T.Knopfle, K.Van Bibber, M.R.Yearian, J.R.Calarco The Inclusive Electrofission of 238U at Incident Energies Between 45 and 120 MeV NUCLEAR REACTIONS 238U(e, e'F), E=47.6-119.1 MeV; measured fission fragment (e')-coin, σ(E).
doi: 10.1016/0370-2693(85)90536-2
1984AR01 J.Phys.(London) G10, 101 (1984) Coincident-Inclusive Electrofission Angular Correlations NUCLEAR REACTIONS 238U(e, e'F), E=9.5 MeV; calculated fission (fragment)(e)(θ), σ(fragment θ, E(e')) vs virtual photon energy.
doi: 10.1088/0305-4616/10/1/015
1984AR03 Z.Phys. A315, 247 (1984) Observation of E2-Fission Decay for 232Th from Electro- and Photoinduced Reactions NUCLEAR REACTIONS 232Th(e, e'F), E=5-7 MeV; 232Th(γ, F), E=5.3-7 MeV; analyzed fission σ(E) data. 232Th deduced GQR transition strength.
doi: 10.1007/BF01419386
1984AR06 Phys.Rev. C29, 1905 (1984) Splitting of Isoscalar Giant Resonances in Actinide Nuclei NUCLEAR REACTIONS 238U(α, α'), E=100, 172 MeV; 238U(e, F), E=5-30 MeV; 232Th, 238U(γ, F), E=5-7 MeV; 232Th(e, F), E=5-8 MeV; analyzed inelastic σ(θ), σ(E), fission data. 238U deduced B(E2), GQR energy distribution, near barrier E2 fission strength. 232Th deduced near barrier fission strength. Natural targets.
doi: 10.1103/PhysRevC.29.1905
1984AR11 Phys.Rev. C29, 2399 (1984) J.D.T.Arruda-Neto, W.Rigolon, S.B.Herdade, H.L.Riette Photofission of 232Th NUCLEAR REACTIONS 232Th(e, F), E=20-32 MeV; measured bremstrahlung induced fission σ(E); deduced photon induced fission σ(E). Comparison with other data.
doi: 10.1103/PhysRevC.29.2399
1982AR05 Phys.Rev. C25, 1689 (1982) J.D.T.Arruda-Neto, M.F.B.M.Vannucci, S.B.Herdade, A.Vannucci, I.C.Nascimento Concentration of E2 Strength near the Fission Barrier of 232Th NUCLEAR REACTIONS, Fission 232Th(e, F), E=5.5-7 MeV; measured σ(fragment θ). 232Th deduced E2 fission probability, EWSR. Natural target.
doi: 10.1103/PhysRevC.25.1689
1982AR14 Nucl.Phys. A389, 378 (1982) J.D.T.Arruda-Neto, S.B.Herdade, I.C.Nascimento, B.L.Berman Electrofission of 234U, 236U and 238U: Angular distributions and E2 strength functions NUCLEAR REACTIONS 234U(e, F), E=5.5-25 MeV; measured fission σ(fragment θ). 234,236,238U deduced dominant fission channel K, multipolarity, E2 fission strength functions, GQR role.
doi: 10.1016/0375-9474(82)90525-5
1982AR15 Acta Phys.Pol. B13, 157 (1982) J.D.T.Arruda-Neto, S.B.Herdade Comment on Electrofission of 237Np in the Energy Range 10-34 MeV NUCLEAR REACTIONS 237Np(e, F), E=10-34 MeV; analyzed published fission data inconsistensies.
1981AR09 Phys.Rev. C23, 2595 (1981) J.D.T.Arruda-Neto, B.L.Berman, S.B.Herdade, I.C.Nascimento Fission Decay of the Giant Quadrupole Resonance for 234U NUCLEAR REACTIONS, Fission 234U(e, F), E=5.5-25.4 MeV; measured σ(fission, E); deduced photofission σ(E). 234U deduced GQR fission decay parameters, EWSR. Enriched, thin targets.
doi: 10.1103/PhysRevC.23.2595
1980AR03 Nucl.Phys. A334, 297 (1980) J.D.T.Arruda Neto, S.B.Herdade, I.C.Nascimento Formalism and Applications of Electrofission and Photofission Fragment Angular Distributions NUCLEAR REACTIONS 238U(e, e'F), E=5.5-9 MeV; measured fission fragment σ(θ). 238U deduced low-lying fissioning levels. Natural target.
doi: 10.1016/0375-9474(80)90070-6
1980AR13 Phys.Rev. C22, 1996 (1980) J.D.T.Arruda-Neto, S.B.Herdade, B.L.Berman, I.C.Nascimento E2 Giant Resonances and an M1 Component in the Photofission of 236U NUCLEAR REACTIONS, Fission 236U(e, F), E=5.5-33 MeV; measured fission-fragment yields, σ(fragment θ). 236U deduced GQR, first chance fission decay.
doi: 10.1103/PhysRevC.22.1996
1980NE06 Nucl.Phys. A349, 483 (1980) Study of Electrofission and Hadron-Induced Fission Decay of the Giant Quadrupole Resonance of 238U NUCLEAR REACTIONS, Fission 238U(e, F), E=10-500 MeV; analyzed σ(E); 238U(α, α'F), E=120 MeV; 238U(6Li, 6Li'F), E=150 MeV; analyzed fission decay probabilities. 238U deduced GQR decay characteristics, first-, second-chance fission components, relative GDR contributions.
doi: 10.1016/0375-9474(80)90302-4
1979AR12 Lett.Nuovo Cim. 26, 487 (1979) J.D.T.Arruda Neto, B.L.Berman, S.B.Herdade, I.C.Nascimento Determination of the Giant E2 Isoscalar Resonance for 236U NUCLEAR REACTIONS 236U(e, F), E=5-27 MeV; 236U(γ, F), E=11-19 MeV bremsstrahlung; measured yields. 236U deduced T=0, GQR, width, energy-weighted sum rule, possible GMR. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0080. 1978AR09 Phys.Rev. C18, 863 (1978) J.D.T.Arruda Neto, S.B.Herdade, B.S.Bhandari, I.C.Nascimento Electric Quadrupole Giant Resonance in the Photofission of 238U NUCLEAR REACTIONS 238U(e, F), E=5.5-28.3 MeV; measured yield, σ(fragment, θ); deduced E2 σ. 238U deduced E2 isoscalar giant resonance parameters.
doi: 10.1103/PhysRevC.18.863
1976AR08 Phys.Rev. C14, 1499 (1976) J.D.T.Arruda Neto, S.B.Herdade, B.S.Bhandari, I.C.Nascimento Electrofission and Photofission of 238U in the Energy Range 6-60 MeV NUCLEAR REACTIONS 238U(e, F), E=6-60 MeV; measured measured σ(E); deduced E1 contribution to fission process.
doi: 10.1103/PhysRevC.14.1499
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