References quoted in the XUNDL dataset: 100MO 9BE(109TC,XG):T1/2:XUNDL-14
6 references found.
Clicking on a keynumber will list datasets that reference the given article.
Z.Phys. A274, 327 (1975)
H.Bohn, P.Kienle, D.Proetel, R.L.Hershberger
Structure of Excited States in 100Mo and 102Mo from Spectroscopy Using 18O Induced Reactions
NUCLEAR REACTIONS 100Mo(18O, 18O'γ), (18O, 16O), E=40 MeV; measured recoil distance DSA. 100,102Mo levels deduced T1/2, β, B(λ).
Phys.Rev. C14, 835 (1976)
P.Paradis, G.Lamoureux, R.Lecomte, S.Monaro
Measurement of the Static Quadrupole Moments of the First 2+ States in 94Mo, 96Mo, 98Mo, and 100Mo
NUCLEAR REACTIONS 94,96,98,100Mo(α, α'), E=8.0 MeV; measured σ(Eα', θ). 94,96,98,100Mo(16O, 16O'), E=36 MeV; measured σ(E(16O'), θ). 94,96,98,100Mo levels deduced quadrupole moment, B(E2). Enriched targets.
Nucl.Phys. A441, 534 (1985)
S.J.Mundy, W.Gelletly, J.Lukasiak, W.R.Phillips, B.J.Varley
Collective Transitions in 100Mo and the Mixed Configuration IBM
NUCLEAR STRUCTURE 100Mo calculated levels, B(E2). Interacting boson model.
NUCLEAR REACTIONS 100Mo(16O, 16O'), E=42 MeV; 100Mo(32S, 32S'), E=89 MeV; 100Mo(58Ni, 58Ni'), E=185 MeV; measured σ(E(γ), θ(γ), particle (θ)), T1/2, Coulomb excitation. 100Mo deduced levels, J, B(E2), quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(85)90161-7
Nucl.Phys. A540, 27 (1992)
M.Pignanelli, N.Blasi, S.Micheletti, R.De Leo, L.LaGamba, R.Perrino, J.A.Bordewijk, M.A.Hofstee, J.M.Schippers, S.Y.van der Werf, J.Wesseling, M.N.Harakeh
Hexadecapole Strength Distributions of Vibrational Nuclei in the A = 100 Mass Region
NUCLEAR REACTIONS 94,98,100Mo, 104,106,110Pd, 110,112Cd(p, p'), E=30.7 MeV; 94,98,100Mo, 104,106,110Pd, 110,112Cd(d, d'), E=50.7 MeV; 100Mo, 110Pd(p, p'), E=51 MeV; 112Cd(p, p'), E=60 MeV; measured σ(Ep', θ), σ(Ed', θ). 94,98,100Mo, 104,106,110Pd, 110,112Cd deduced levels, J, π, B(λ). Enriched targets.
doi: 10.1016/0375-9474(92)90192-M
Phys.Rev. C 86, 064305 (2012)
K.Wrzosek-Lipska, L.Prochniak, M.Zielinska, J.Srebrny, K.Hadynska-Klek, J.Iwanicki, M.Kisielinski, M.Kowalczyk, P.J.Napiorkowski, D.Pietak, T.Czosnyka
Electromagnetic properties of 100Mo: Experimental results and theoretical description of quadrupole degrees of freedom
NUCLEAR REACTIONS 100Mo(32S, 32S'), E=76 MeV; measured Eγ, Iγ, γ(θ), (particle)γ-coin using OSIRIS-II array. 100Mo; deduced levels, J, π, E1, E2, E3, M1 reduced matrix elements using GOSIA code, shape deformation parameters, Q2 (quadrupole overall deformation parameter) and cos(3δ) (quadrupole asymmetry parameter). Coulomb excitation. Level and B(E2) systematics of even-even Mo isotopes from N=50-64. Comparison with general quadrupole collective Bohr Hamiltonian (GBH) model.
NUCLEAR STRUCTURE 100Mo; calculated levels, J, π, potential energy surfaces, E2 matrix elements. general quadrupole collective Bohr Hamiltonian (GBH) model.
doi: 10.1103/PhysRevC.86.064305
Phys.Rev. C 95, 034320 (2017)
D.Ralet, for the PreSPEC and AGATA Collaborations
Lifetime measurement of neutron-rich even-even molybdenum isotopes
NUCLEAR REACTIONS 9Be(238U, F)105Nb/106Nb/107Nb/106Mo/107Mo/108Mo/109Mo/108Tc/109Tc/110Tc/, E=600 MeV/nucleon; measured reaction products using FRS separator and Lund-York-Cologne calorimeter (LYCCA) at GSI, Eγ, Iγ, (fragment)γ-coin, level half-lives by a relativistic version of the Doppler-shift-attenuation method using AGATA and HECTOR+ arrays at GSI. 100,102,104,106,108Mo; deduced levels, half-lives for yrast levels, transition quadrupole moments; calculated particle-number projected potential energy surfaces in (β2, γ) plane. Comparison of level half-lives with previous experimental data, and deduced B(E2) values with beyond-mean-field calculations within the symmetry conserving configuration mixing (SCCM) method with Gogny D1S functional.
doi: 10.1103/PhysRevC.95.034320