NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = M.N.Martins Found 26 matches. 2019SA44 Phys.Rev. A 100, 022703 (2019) O.C.B.Santos, V.R.Vanin, N.L.Maidana, M.N.Martins, M.H.Tabacniks, C.L.Rodrigues, T.F.Silva, A.D.Santos, S.F.Barros, J.A.Garcia-Alvarez, M.F.Koskinas, J.M.Fernandez-Varea, M.S.Pindzola Experimental and theoretical cross sections for K-shell ionization of 52Te , 73Ta , and 83Bi by electrons with energies up to 100 keV NUCLEAR REACTIONS Te, Ta, Bi(E, E'), E<100keV; measured reaction products, X-rays; deduced σ.
doi: 10.1103/PhysRevA.100.022703
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
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
2001SH03 Phys.Rev. C63, 017602 (2001) V.B.Shostak, G.P.Palkin, N.I.Woloshin, V.P.Likhachev, M.N.Martins, M.T.F.da Cruz 6He Neutron Distribution Radius from 7Li(p, 2p)6He Reaction NUCLEAR REACTIONS 7Li(p, 2p), E=70 MeV; analyzed σ(E, θ). 6He deduced neutron rms radius. Distorted-wave approximation for nonlocal realistic t matrix.
doi: 10.1103/PhysRevC.63.017602
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
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
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
1999TE01 Phys.Rev. C59, 522 (1999) L.A.A.Terremoto, V.P.Likhachev, M.N.Martins, M.T.F.da Cruz, N.Teruya Branching Ratio of the 26Mg(e, e'α0)22Ne Reaction in the Giant Resonance Region NUCLEAR REACTIONS 26Mg(e, e'α), E=14-26 MeV; analyzed data; deduced α0 branching ratios. 26Mg deduced α0 decay branch of GDR.
doi: 10.1103/PhysRevC.59.522
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
1997TE11 Phys.Rev. C56, 2597 (1997) L.A.A.Terremoto, V.P.Likhachev, M.N.Martins, H.J.Emrich, G.Fricke, T.Krohl, K.W.Neff Giant Resonances in the 26Mg(e, e'α0)22Ne Reaction NUCLEAR REACTIONS 26Mg(e, e'α), E=14-26 MeV; measured eα-coin, σ(Eα, Ee, θ(α), θ(e)); deduced multipole components, sum rules. 22Ne deduced resonances.
doi: 10.1103/PhysRevC.56.2597
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
1995AN16 Phys.Rev. C52, 1484 (1995) Two Proton and Two Neutron Photoemission Cross Sections of 63Cu NUCLEAR REACTIONS 63Cu(e, 2p), (e, 2n), E=28-60 MeV; measured electrodisintegration σ; deduced σ(γ, 2p)(Eγ), σ(γ), 2n(Eγ), E2, E1 components.
doi: 10.1103/PhysRevC.52.1484
1993GE03 Phys.Rev. C48, 105 (1993) One Neutron Photoemission Cross Section of 238U NUCLEAR REACTIONS 238U(e, n), E=12-60 MeV; measured σ(θ); deduced E1, E2 components of (γ, n) reaction. DWBA analysis.
doi: 10.1103/PhysRevC.48.105
1990DI07 Phys.Rev. C42, 1559 (1990) H.F.Dias, M.N.Martins, E.Wolynec Proton Emission Cross Sections of Silicon Isotopes NUCLEAR REACTIONS, ICPND 30,29Si(e, p), (e, 2p), E=20-60 MeV; measured σ(E); deduced σ(E) for (γ, p), (γ, 2p). Virtual photon theory.
doi: 10.1103/PhysRevC.42.1559
1988CA12 J.Phys.(London) G14, 779 (1988) M.I.C.Cataldi, E.Wolynec, M.N.Martins, P.Gouffon, Y.Miyao Electrodisintegration of 208Pb, 209Bi and 181Ta NUCLEAR REACTIONS 208Pb, 209Bi, 181Ta(e, xn), E=8-22 MeV; calculated electrodisintegration σ(E). 181Ta, 208Pb, 209Bi deduced isoscalar E2 transition strengths, B(M1). Virtual photon analysis.
doi: 10.1088/0305-4616/14/6/018
1988CA15 J.Phys.(London) G14, 1139 (1988) M.C.A.Campos, E.Wolynec, M.N.Martins M1 Strength in 197Au NUCLEAR REACTIONS 197Au(e, n), E=9-23 MeV; measured σ(E). 197Au deduced E2 and M1 transition strengths. Virtual photon analysis.
doi: 10.1088/0305-4616/14/8/016
1987WO02 J.Phys.(London) G13, 515 (1987) E.Wolynec, V.A.Serrao, M.N.Martins Nuclear Size Effects in Virtual Photon Spectra NUCLEAR REACTIONS 181Ta(e, n), E=9-30 MeV; measured σ(E). 181Ta deduced E2 transition strength. Activation method. Virtual photon analysis.
doi: 10.1088/0305-4616/13/4/015
1985DO15 Phys.Rev. C32, 781 (1985) W.R.Dodge, E.Hayward, M.N.Martins, E.Wolynec (e, p) and (e, α) Reactions in 90Zr and 92Zr NUCLEAR REACTIONS 92,90Zr(e, p), (e, α), E=20-130 MeV; measured σ(θp, Ep), σ(θα, Eα), proton, α yields; deduced σ(γ, p), σ(γ, α). Enriched targets. DWBA, virtual photon spectra.
doi: 10.1103/PhysRevC.32.781
1984MA53 Phys.Rev. C30, 1855 (1984) M.N.Martins, E.Hayward, G.Lamaze, X.K.Maruyama, F.J.Schima, E.Wolynec Experimental Test of the Bremsstrahlung Cross Section NUCLEAR REACTIONS 63Cu(e, n), E=13.5-60 MeV; measured electrodisintegration σ(E); deduced bremsstrahlung σ(E), σ(γ, n). Activation technique, thin Cu, Mo, Ta, Th radiators. Virtual photon theory.
doi: 10.1103/PhysRevC.30.1855
1984WO04 Phys.Rev. C29, 1137 (1984) E.Wolynec, A.R.V.Martinez, P.Gouffon, Y.Miyao, V.A.Serrao, M.N.Martins Comment on Photoneutron Cross Sections NUCLEAR REACTIONS 89Y, 115In, 117,118,120,124Sn, 133Cs, 159Tb, 165Ho, 181Ta, 197Au, 208Pb(γ, n), (γ, 2n), E not given; analyzed data; deduced neutron multiplicity sorting role. Saclay, Livermore data.
doi: 10.1103/PhysRevC.29.1137
1982MA41 Phys.Rev. C26, 1936 (1982) M.N.Martins, E.Wolynec, M.C.A.Campos Electrodisintegration of 63Cu and 65Cu NUCLEAR REACTIONS 65Cu(e, α), 63Cu(e, 2n), E=14-34 MeV; measured σ(E); deduced σ(γ, α), σ(γ, 2n) vs E. DWBA analysis, virtual photons, electrodisintegration.
doi: 10.1103/PhysRevC.26.1936
1977MA19 Phys.Rev. C16, 613 (1977) M.N.Martins, E.Wolynec, G.Moscati Multipolarities of Nuclear Transitions Involved in the One Neutron Disintegration of 238U NUCLEAR REACTIONS 238U(e, en), E=6-25 MeV; measured σ(E). DWBA virtual photon analysis.
doi: 10.1103/PhysRevC.16.613
1976WO06 Phys.Rev.Lett. 37, 585 (1976) E.Wolynec, M.N.Martins, G.Moscati Alpha Decay of the Giant Quadrupole Resonance in 238U NUCLEAR REACTIONS 238U(e, e'α), E=9-24 MeV; measured σ(E). 238U deduced E2 strength, Γ.
doi: 10.1103/PhysRevLett.37.585
1975WO04 Phys.Rev. C11, 1083 (1975) E.Wolynec, G.Moscati, J.R.Moreira, O.D.Goncalves, M.N.Martins Disintegration of 12C, 19F, 35Cl, 63Cu, and 65Cu by Real and Virtual Radiation NUCLEAR REACTIONS 12C, 19F, 35Cl, 65Cu(γ, n), (e, e'n), 63Cu(γ, 2n), (e, e'2n), E=16-39 MeV; measured σ(Eγ)/σ(Ee); deduced photoabsorption.
doi: 10.1103/PhysRevC.11.1083
1975WO07 Nucl.Phys. A244, 205 (1975) E.Wolynec, G.Moscati, O.D.Goncalves, M.N.Martins An Analysis of Electrodisintegration of Nuclei Using E1 Virtual Radiation Spectra Evaluated with Coulomb Distorted Waves NUCLEAR REACTIONS 12C, 63Cu, 64Zn, 109Ag, 181Ta, 197Au(e, e'n), (γ, n), E=12-36 MeV; calculated photo/electro disintegration.
doi: 10.1016/0375-9474(75)90056-1
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