NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = M.Montoya

Found 13 matches.

Back to query form

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)

M.Montoya

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)

M.Montoya

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 T_1/2; deduced SF(T_1/2) limit, branching ratio. ²⁵⁶Rf(SF) [from ²⁶⁰Sg(α-decay)]; measured T_1/2. ²⁶⁰Sg, ²⁵⁶Rf deduced mass excess.

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

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

M.Montoya

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)

M.Montoya

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