NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Kildir Found 22 matches. 2007GH06 Phys.Rev. C 75, 044308 (2007) M.Gholami, M.Kildir, A.N.Behkami Microscopic study of spin cut-off factors of nuclear level densities NUCLEAR STRUCTURE A=20-251; calculated spin cut-off parameters using the BCS theory, from the Gilbert and Cameron expression, and from rigid body calculations, compared results from microscopic calculations to their corresponding macroscopic values.
doi: 10.1103/PhysRevC.75.044308
2006BU22 Phys.Rev. C 74, 054613 (2006) Monte Carlo calculation of the de-excitation of fission fragments of 252Cf(sf) within multimodal random neck rupture model RADIOACTIVITY 252Cf(SF); calculated fission fragment yields, neutron and γ-ray multiplicities. Monte Carlo approach, multimodal random neck rupture model, comparisons with data.
doi: 10.1103/PhysRevC.74.054613
2002OZ06 J.Nucl.Radiochem.Sci. 3, No 1, 95 (2002) I.Ozkan, Z.Buyukmumcu, H.Sokmen, M.Kildir Multi-modal Study of Angular Momentum Distribution of Fission Fragments as a Result of Bending Modes NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated fission fragments average angular momenta vs mass. Multimodal fission model. RADIOACTIVITY 252Cf, 248Cm(SF); calculated fission fragments average angular momenta vs mass. Multimodal fission model.
1996BR25 Phys.Rev. C54, 1749 (1996) A.Brondi, M.Kildir, G.La Rana, R.Moro, E.Vardaci, S.Pirrone, F.Porto, S.Sambataro, G.Politi, P.Figuera Reaction Mechanism Coexistence in the 123 MeV 19F + 56Fe Reaction NUCLEAR REACTIONS 56Fe(19F, X), (19F, 19F), E=123 MeV; measured σ(fragment θ) for x=11B to 22Ne, elastic σ(θ); deduced deep inelastic, incomplete fusion processes contributions, angular momentum localization. Extended Wilczynski sum rule model.
doi: 10.1103/PhysRevC.54.1749
1996BU54 J.Radioanal.Nucl.Chem. 204, 275 (1996) Z.Buyukmumcu, M.Kildir, N.K.Aras Determination of Pre-Scission Kinetic Energy in Low Energy Fission using Isotonic Charge Distribution Model NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; analyzed fission products charge distributions; deduced parameters, global odd-even effect, pre-scission kinetic energies.
1995KI02 Phys.Rev. C51, 1873 (1995) M.Kildir, G.La Rana, R.Moro, A.Brondi, E.Vardaci, A.D'Onofrio, D.Fessas, E.Perillo, V.Roca, M.Romano, F.Terrasi, G.Nebbia, G.Viesti, G.Prete Ingoing-Wave Boundary Condition Versus Optical Model Transmission Coefficients: A systemactic comparison with particle emission data NUCLEAR REACTIONS C(28Si, X), E=150 MeV; 103Rh(14N, X), E=81, 121 MeV; 77Se(40Ar, X), E=146, 201 MeV; 64,58Ni(19F, X), E=120 MeV; 58Ni(28Si, X), E=150 MeV; 91Zr(32S, X), E=180 MeV; measured evaporation spectra, yields for 1,2,3H, 4He. Statistical model analysis, ingoing-wave boundary-condition versus optical model transmission coefficients.
doi: 10.1103/PhysRevC.51.1873
1992KI22 Phys.Rev. C46, 2264 (1992) M.Kildir, G.La Rana, R.Moro, A.Brondi, A.D'Onofrio, E.Perillo, V.Roca, M.Romano, F.Terrasi, G.Nebbia, G.Viesti, G.Prete 1,2,3H, 4He Emission from 96Ru Nuclei (E(*) ≈ 113 MeV): Test for transmission coefficients in the evaporation model NUCLEAR REACTIONS 64Ni(32S, xp), (32S, xd), (32S, xt), (32S, xα), E=180 MeV; measured σ(E, θ); deduced transmission coefficients effect. Optical, ingoing wave boundary condition model, fusion systematics.
doi: 10.1103/PhysRevC.46.2264
1989PE01 Phys.Rev. C39, 488 (1989) G.F.Peaslee, N.N.Ajitanand, J.M.Alexander, R.Lacey, L.C.Vaz, M.Kaplan, M.Kildir, D.J.Moses, D.Logan, M.S.Zisman Particle-Particle Coincidence Measurements for 1,2,3H and 4He in the Reaction 480 MeV 56Fe + (nat)Ag NUCLEAR REACTIONS Ag(56Fe, pX), (56Fe, dX), (56Fe, tX), (56Fe, αX), E=480 MeV; measured (particle)(particle)-coin; deduced average particle multiplicities, energy removed, effective emission barriers.
doi: 10.1103/PhysRevC.39.488
1988LA12 Phys.Rev. C37, 2540 (1988) R.Lacey, N.N.Ajitanand, J.M.Alexander, D.M.de Castro Rizzo, G.F.Peaslee, L.C.Vaz, M.Kaplan, M.Kildir, G.La Rana, D.J.Moses, W.E.Parker, D.Logan, M.S.Zisman, P.DeYoung, L.Kowalski Mechanisms for Light Charged Particle Emission in the Reactions 247 and 337 MeV 40Ar + (nat)Ag NUCLEAR REACTIONS Ag(40Ar, pX), (40Ar, dX), (40Ar, tX), (40Ar, αX), (40Ar, X), E=247, 337 MeV; measured σ(θ), σ(Eα, θα); deduced pre-, post scission emission multiplicities. Deformed emitters.
doi: 10.1103/PhysRevC.37.2540
1988LA13 Phys.Rev. C37, 2561 (1988) R.Lacey, N.N.Ajitanand, J.M.Alexander, D.M.de Castro Rizzo, G.F.Peaslee, L.C.Vaz, M.Kaplan, M.Kildir, G.La Rana, D.J.Moses, W.E.Parker, D.Logan, M.S.Zisman, P.DeYoung, L.Kowalski Large-Angle Correlations between 4He and 1,2,3H or 4He in the Reactions 247 and 337 MeV 40Ar + (nat)Ag: Unexpected properties of the nuclear stratosphere NUCLEAR REACTIONS Ag(40Ar, αX), E=247, 337 MeV; measured α(light fragment)-coin, energy correlations; deduced emission source properties, mechanism.
doi: 10.1103/PhysRevC.37.2561
1988PE16 Phys.Rev. C38, 1730 (1988) G.F.Peaslee, N.N.Ajitanand, J.M.Alexander, D.Guerreau, R.Lacey, L.C.Vaz, M.Kaplan, M.Kildir, D.J.Moses, D.Logan, M.S.Zisman Sources of Light-Charged-Particle Emission in the Reaction 480 MeV 56Fe + (nat)Ag NUCLEAR REACTIONS Ag(56Fe, pX), (56Fe, dX), (56Fe, tX), (56Fe, αX), E=480 MeV; measured σ(fragment θ), σ(E(X), θ(X)) for X=p, d, t, α; deduced reaction, particle emission mechanisms.
doi: 10.1103/PhysRevC.38.1730
1987MO05 Nucl.Phys. A465, 339 (1987) D.J.Moses, M.Kaplan, M.Kildir, D.R.G.Logan, G.La Rana, W.E.Parker, R.Lacey, G.F.Peaslee, J.M.Alexander, N.N.Ajitanand, L.C.Vaz, M.S.Zisman Light Charged Particle Emission in 485 MeV 56Fe + 197Au Reactions: Correlations with heavy fragments and relationships to spin and lifetime NUCLEAR REACTIONS 197Au(56Fe, X), (56Fe, F), E=485 MeV; measured σ(Eα, θα, fragment θ), σ(Ep), σ(Eα), σ(Ep, θp, fragment θ) following fission, deep inelastic scattering; deduced evaporative light-particle multiplicities for each emission source. 252Db deduced T1/2.
doi: 10.1016/0375-9474(87)90438-6
1985MO04 Z.Phys. A320, 229 (1985) D.J.Moses, M.Kaplan, J.M.Alexander, D.Logan, M.Kildir, L.C.Vaz, N.N.Ajitanand, E.Duek, M.S.Zisman Particle Spectra from Reversed Kinematics: Powerful probes of hot rotating nuclei NUCLEAR REACTIONS 12C(40Ar, pX), (40Ar, αX), (56Fe, pX), (56Fe, αX), (86Kr, pX), (86Kr, αX), E=8.5 MeV/nucleon; measured inclusive σ(θ, Ep), σ(θ, Eα); deduced effective evaporation emission, fusion barriers. Hot spot, moving source model.
doi: 10.1007/BF01881270
1984AJ02 Z.Phys. A316, 169 (1984) N.N.Ajitanand, J.M.Alexander, H.Delagrange, E.Duek, D.O.Eriksen, D.Guerreau, M.Kaplan, M.Kildir, L.Kowalski, R.Lacey, D.Logan, D.J.Moses, G.F.Peaslee, L.C.Vaz, M.S.Zisman Multiplicities for Evaporative 4He Emission in Heavy Ion Reactions: Relationships to spin and lifetime expectancy of the composite nucleus NUCLEAR REACTIONS Ag, 238U(40Ar, αX), (56Fe, αX), (40Ar, αF), (56Fe, αF), E=8.5 MeV/nucleon; measured σ(fragment θ, θα, Eα), fission-fusion, projectile-like fragment-coin; deduced reaction mechanism, hot nucleus thermodynamic properties.
doi: 10.1007/BF01412259
1984DU09 Z.Phys. A317, 83 (1984) E.Duek, N.N.Ajitanand, J.M.Alexander, D.Logan, M.Kildir, L.Kowalski, L.C.Vaz, D.Guerreau, M.S.Zisman, M.Kaplan, D.J.Moses Mechanisms for Emission of 4He in the Reactions of 334 MeV 40Ar with 238U NUCLEAR REACTIONS 238U(40Ar, αF), E=334 MeV; measured fission (fragment)(fragment)(α)-coin, σ(θα, Eα); deduced fission, α-emission mechanisms.
doi: 10.1007/BF01420452
1984KI07 Z.Phys. A317, 291 (1984) M.Kildir, D.Logan, D.O.Eriksen, D.J.Moses, M.Kaplan, E.Duek, L.C.Vaz, N.N.Ajitanand, J.M.Alexander, M.S.Zisman Fission Reactions of 468-MeV 56Fe + 238U: Detection of 4He/1H Emission from Pre- and Post-Fission Sources NUCLEAR REACTIONS 238U(56Fe, pF), (56Fe, αF), E=469 MeV; measured fission (fragment)(fragment)(θ), σ(θp, Ep, fragment θ), σ(θα, Eα, fragment θ), proton, α differential multiplicities, σ(θα, Eα); deduced light particle emission mechanism.
doi: 10.1007/BF01438361
1983DU14 Phys.Lett. 131B, 297 (1983) E.Duek, N.N.Ajitanand, J.M.Alexander, D.Logan, M.Kildir, L.Kowalski, L.C.Vaz, D.Guerreau, M.S.Zisman, M.Kaplan New Probe of Interediate Reaction Times: Near-Scission Emission of 4He for 334 MeV 40Ar + 238U NUCLEAR REACTIONS 238U(40Ar, αX), (40Ar, αF), E= 334 MeV; measured α(fragment)-coin following fusion, fission; deduced fragment, composite nucleus evaporation upper limit, near scission role.
doi: 10.1016/0370-2693(83)90502-6
1983KA16 Z.Phys. A313, 31 (1983) M.Kaplan, D.J.Moses, D.O.Eriksen, M.Kildir, D.R.G.Logan, M.S.Zisman, R.J.McDonald Light Charged Particle Emission and Fission in 238U + 238U Collisions at 1, 740 MeV NUCLEAR REACTIONS 197Au, 238U(238U, pX), (238U, αX), E=7.31 MeV/nucleon; measured p(fragment)-, α(fragment)-coin, σ(θp, Ep), σ(θα, Eα); deduced reaction mechanism, target, projectile sequential fission.
doi: 10.1007/BF02115840
1982KI01 Phys.Rev. C25, 365 (1982) Monte Carlo Calculation of the Deexcitation of Fission Fragments in the Spontaneous Fission of 252Cf RADIOACTIVITY, Fission 252Cf(SF); calculated prompt neutron yields vs fragment mass, Z, multiplicity distribution, total Eγ vs fragment Z, fractional yield vs Z for A=136, 138, 139, secondary fragment yield vs mass. Monte Carlo method.
doi: 10.1103/PhysRevC.25.365
1982KI06 Z.Phys. A306, 323 (1982) M.Kildir, D.Logan, M.Kaplan, M.S.Zisman, D.Guerreau, J.M.Alexander, L.C.Vaz Studies of 4He Emission in Both Fusion-Like and Inelastic Reactions of 340-MeV 40Ar + 238U NUCLEAR REACTIONS 238U(40Ar, αF), E=340 MeV; measured σ(θα, Eα), (fragment)(fragment)α-coin; deduced fusion-fission, sequential fission induced direct, evaporation α emission.
doi: 10.1007/BF01432373
1980KI05 Nucl.Phys. A340, 117 (1980) Isospin Dependence of the Nuclear Level Width in the Compound Nucleus 30P NUCLEAR REACTIONS 29Si(p, α), E=13.5-15.5 MeV; measured σ(E). 30P levels deduced widths, densities for T < , T > isospin states.
doi: 10.1016/0375-9474(80)90326-7
1973KI10 Phys.Rev. C8, 1965 (1973) Isospin Dependence of the Nuclear Level Width NUCLEAR REACTIONS 31P(p, α), (p, p'), E=8.5-10.0 MeV, measured σ(E;θ). 32S deduced level widths, level densities for isospin states at 17.8 MeV.
doi: 10.1103/PhysRevC.8.1965
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