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NSR database version of April 11, 2024.

Search: Author = J.Arruda-Neto

Found 73 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0652.


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
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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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0692.


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
Citations: PlumX Metrics


1999DE35      Eur.Phys.J. A 6, 107 (1999)

A.Deppman, J.D.T.Arruda-Neto

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0617.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0647.


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
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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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0773.


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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0756.


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
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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
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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
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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
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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
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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
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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
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1988AR01      Phys.Rev. C37, 1326 (1988)

J.D.T.Arruda-Neto

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
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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
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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
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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
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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
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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
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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
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1985AR21      Acta Phys.Pol. B16, 963 (1985)

J.D.T.Arruda-Neto

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
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1984AR01      J.Phys.(London) G10, 101 (1984)

J.D.T.Arruda-Neto

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
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1984AR03      Z.Phys. A315, 247 (1984)

J.D.T.Arruda-Neto

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
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1984AR06      Phys.Rev. C29, 1905 (1984)

J.D.T.Arruda-Neto

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
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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
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1984CA34      Phys.Lett. 146B, 179 (1984)

J.R.Calarco, J.Arruda-Neto, K.A.Griffioen, S.S.Hanna, D.H.H.Hoffmann, B.Neyer, R.E.Rand, K.Wienhard, M.R.Yearian

Observation of Monopole Strength in the 12C(e, e'p0)11B Reaction

NUCLEAR REACTIONS 12C(e, e'p), E=86, 118, 126 MeV; measured σ(E(e'), θ(e'), θp), forward, backward asymmetry. 12C deduced possible monopole resonance, EWSR.

doi: 10.1016/0370-2693(84)91012-8
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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
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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
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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
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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
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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
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1980NE06      Nucl.Phys. A349, 483 (1980)

J.D.T.Arruda Neto, B.L.Berman

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
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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
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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0533.


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