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NSR database version of May 24, 2024.

Search: Author = M.Montoya

Found 13 matches.

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2000VA10      Phys.Lett. 480B, 239 (2000)

E.Vardaci, M.Kaplan, W.E.Parker, D.J.Moses, J.T.Boger, G.J.Gilfoyle, M.A.McMahan, M.Montoya

Search for Ternary Fragmentation in the Reaction 856 MeV 98Mo + 51V: Kinematic probing of intermediate-mass-fragment emissions

NUCLEAR REACTIONS 51V(98Mo, X), E=856 MeV; measured intermediate mass fragment, fission fragment spectra, angular correlations; deduced no three-body breakup.

doi: 10.1016/S0370-2693(00)00407-X
Citations: PlumX Metrics

1991BO15      Z.Phys. A338, 369 (1991)

B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, D.Gardes, F.Hanappe, D.Jouan, M.Montoya

Excitation Energy Partition in Deeply Inelastic Collisions between 40Ar and Ag at 27 MeV Per Nucleon

NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured fragment particle evaporation; deduced excitation energy partition features.

doi: 10.1007/BF01288204
Citations: PlumX Metrics

1991GO03      Z.Phys. A338, 51 (1991)

U.Gollerthan, T.Brohm, H.-G.Clerc, E.Hanelt, M.Horz, W.Morawek, W.Schwab, K.-H.Schmidt, F.P.Hessberger, G.Munzenberg, V.Ninov, R.S.Simon, J.P.Dufour, M.Montoya

Decay of the Compound Nucleus 179Au Formed in the Cold Fusion Reaction 90Zr + 89Y

NUCLEAR REACTIONS 89Y(90Zr, X), E=4.02 MeV/nucleon; measured (light charged particle)(evaporation residue)-coin, σ(Ep, θp), σ(Eα, θα), γ(light charged particle)-coin; deduced σ, different channels. Cold fusion, statistical model analysis.

doi: 10.1007/BF01279114
Citations: PlumX Metrics

1991JO12      Z.Phys. A340, 63 (1991)

D.Jouan, B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, H.Gauvin, C.Gregoire, F.Hanappe, D.Gardes, M.Montoya, B.Remaud, F.Sebille

Dynamics and Thermalization in Violent Collisions between 40Ar and Ag at 27 MeV/nucleon

NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured (fragment)(fragment)-coin; deduced reaction mechanism.

doi: 10.1007/BF01284482
Citations: PlumX Metrics

1988BO13      Phys.Lett. 205B, 26 (1988)

B.Borderie, M.Montoya, M.F.Rivet, D.Jouan, C.Cabot, H.Fuchs, D.Gardes, H.Gauvin, D.Jacquet, F.Monnet, F.Hanappe

Deeply Inelastic Collisions as a Source of Intermediate Mass Fragments at E/A = 27 MeV

NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured fragment σ(θ1, θ2); deduced reaction mechanism.

doi: 10.1016/0370-2693(88)90393-0
Citations: PlumX Metrics

1988GO03      Phys.Lett. 201B, 206 (1988)

U.Gollerthan, H.-G.Clerc, E.Hanelt, W.Morawek, V.Ninov, W.Schwab, K.-H.Schmidt, F.-P.Hessberger, G.Munzenberg, R.S.Simon, J.-P.Dufour, M.Montoya

Observation of Enhanced Low-Energy Charged-Particle Emission in the Cold Fusion Reaction 90Zr + 89Y

NUCLEAR REACTIONS 89Y(90Zr, pα), E=362 MeV; measured σ(Ep, θp), σ(Eα, θα), p(residue)-, α(residue)-coin. Detector telescopes. Statistical model calculations.

doi: 10.1016/0370-2693(88)90213-4
Citations: PlumX Metrics

1987MO31      J.Phys.(Paris), Colloq.C-2, 353 (1987)


What Odd Even Effects Mean in Low Energy Fission ( Question )

NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; calculated fission fragment mass, charge, kinetic energy distribution; deduced proton, neutron odd-even effects. Statistical pair breaking mechanism.

1986MO08      Radiat.Eff. 93, 9 (1986)


Shell and Coulomb Effects in Thermal Neutron Induced Cold Fission of U-233, U-235, and Pu-239

NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; measured fission fragment mass, kinetic energy distribution; deduced Coulomb, shell effects role. Static scission model.

doi: 10.1080/00337578608207417
Citations: PlumX Metrics

1986MO23      Z.Phys. A325, 357 (1986)

M.Montoya, R.W.Hasse, P.Koczon

Coulomb Effects in Low Energy Fission

NUCLEAR REACTIONS 234,236U(n, F), E=low; analyzed cold fission fragment charge, total kinetic energy distributions, yield data; deduced Coulomb effects role in fission. Static scission model.

1985HO29      Nucl.Phys. A447, 335c (1985)

S.Hofmann, P.Armbruster, G.Munzenberg, W.Reisdorf, K.-H.Schmidt, H.G.Burkhard, F.P.Hessberger, H.-J.Schott, Y.K.Agarwal, G.Berthes, U.Gollerthan, H.Folger, R.Hingmann, J.G.Keller, M.E.Leino, P.Lemmertz, M.Montoya, K.Poppensieker, B.Quint, I.Zychor

The Influence of the Surprising Decay Properties of Element 108 on Search Experiments for New Elements

RADIOACTIVITY 260Sg(α) [from 208Pb(54Cr, 2n), E=4.92 MeV/nucleon]; measured T1/2; deduced SF(T1/2) limit, branching ratio. 256Rf(SF) [from 260Sg(α-decay)]; measured T1/2. 260Sg, 256Rf deduced mass excess.

doi: 10.1016/0375-9474(86)90615-9
Citations: PlumX Metrics

1984MO26      Z.Phys. A319, 219 (1984)


Mass and Kinetic Energy Distribution in Cold Fission of 233U, 235U and 239Pu Induced by Thermal Neutrons

NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; measured fission fragment yield vs mass, kinetic energy distributions. Static scission configuration model.

doi: 10.1007/BF01415636
Citations: PlumX Metrics

1983MO12      J.Phys.(Paris) 44, 785 (1983)


Nucleon Pair Breaking in the Thermal Neutron Induced Fission of 233U and 235U

NUCLEAR REACTIONS 233,235U(n, F), E=thermal; analyzed fission fragment mass yield data; deduced nucleon pair breaking during saddle to scission transition.

doi: 10.1051/jphys:01983004407078500
Citations: PlumX Metrics

1981SI12      J.Phys.(Paris), Lett. 42, L-437 (1981)

C.Signarbieux, M.Montoya, M.Ribrag, C.Mazur, C.Guet, P.Perrin, M.Maurel

Evidence for Nucleon Pair Breaking Even in the Coldest Scission Configurations of 234U and 236U

NUCLEAR REACTIONS, Fission 233,235U(n, F), E=thermal; measured σ(fragment mass) vs kinetic energy release; deduced nucleon pair breaking effects.

doi: 10.1051/jphyslet:019810042019043700
Citations: PlumX Metrics

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