References quoted in the XUNDL dataset: 104CD 92MO(106CD,104CDG):T:XUNDL-9
4 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. C64, 014305 (2001)
G.A.Muller, A.Jungclaus, O.Yordanov, E.Galindo, M.Hausmann, D.Kast, K.P.Lieb, S.Brant, V.Krstic, D.Vretenar, A.Algora, F.Brandolini, G.de Angelis, M.De Poli, C.Fahlander, A.Gadea, T.Martinez, D.R.Napoli, A.Dewald, R.Peusquens, H.Tiesler, M.Gorska, H.Grawe, P.G.Bizzeti
High-Spin Structure and Electromagnetic Transition Strengths in 104Cd
NUCLEAR REACTIONS 58Ni(50Cr, 4p), E=200, 205 MeV; measured Eγ, Iγ, γγ-coin, DSA. 104Cd deduced high-spin levels, J, π, T1/2, B(E2), B(M1). GASP array, lineshape and recoil-distance measurements. Comparison with interacting-boson-plus-broken-pair model calculations.
doi: 10.1103/PhysRevC.64.014305
Phys.Rev. C 75, 054311 (2007); Erratum Phys.Rev. C 77, 019901 (2008)
N.Boelaert, A.Dewald, C.Fransen, J.Jolie, A.Linnemann, B.Melon, O.Moller, N.Smirnova, K.Heyde
Low-spin electromagnetic transition probabilities in 102, 104Cd
NUCLEAR REACTIONS 92Mo(12C, 2n), E=41 MeV; 94Mo(12C, 2n), E=42 MeV; measured Eγ, Iγ and lifetimes for low lying states using recoil distance Doppler shift technique. Deduced B(E2).
doi: 10.1103/PhysRevC.75.054311
Phys.Rev. C 80, 054302 (2009)
A.Ekstrom, J.Cederkall, D.D.DiJulio, C.Fahlander, M.Hjorth-Jensen, A.Blazhev, B.Bruyneel, P.A.Butler, T.Davinson, J.Eberth, C.Fransen, K.Geibel, H.Hess, O.Ivanov, J.Iwanicki, O.Kester, J.Kownacki, U.Koster, B.A.Marsh, P.Reiter, M.Scheck, B.Siebeck, S.Siem, I.Stefanescu, H.K.Toft, G.M.Tveten, J.Van de Walle, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, K.Wrzosek, M.Zielinska
Electric quadrupole moments of the 2+1 states in 100, 102, 104Cd
NUCLEAR REACTIONS 109Ag(100Cd, 100Cd'), E=287.0 MeV; 64Zn, 109Ag(102Cd, 102Cd'), E=292.7 MeV; 64Zn, 109Ag(104Cd, 104Cd'), E=298.7 MeV; measured Eγ, Iγ, γ(particle)-coin, and γ-ray yields using REX-ISOLDE facility. 64Zn, 100,102,104Cd, 109Ag; deduced levels, J, π, E2 matrix elements, electric quadrupole moments. Comparison with shell model calculations.
NUCLEAR MOMENTS 100,102,104Cd; measured electric quadrupole moments of first 2+ states using reorientation method in Coulomb excitation. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.80.054302
Phys.Rev. C 104, 034320 (2021)
M.Siciliano, J.J.Valiente-Dobon, A.Goasduff, T.R.Rodriguez, D.Bazzacco, G.Benzoni, T.Braunroth, N.Cieplicka-Orynczak, E.Clement, F.C.L.Crespi, G.de France, M.Doncel, S.Erturk, C.Fransen, A.Gadea, G.Georgiev, A.Goldkuhle, U.Jakobsson, G.Jaworski, P.R.John, I.Kuti, A.Lemasson, H.Li, A.Lopez-Martens, T.Marchi, D.Mengoni, C.Michelagnoli, T.Mijatovic, C.Muller-Gatermann, D.R.Napoli, J.Nyberg, M.Palacz, R.M.Perez-Vidal, B.Saygi, D.Sohler, S.Szilner, D.Testov
Lifetime measurements in the even-even 102-108Cd isotopes
NUCLEAR REACTIONS 92Mo(106Cd, 106Cd'), E=770 MeV; measured Eγ, Iγ, γγ-coin, level T1/2 by recoil-distance Doppler-shift (RDDS) method using the AGATA γ-ray spectrometer, VAMOS++ magnetic spectrometer, and Cologne plunger device at the GANIL facility. 102,104,106,108Cd; deduced levels, J, π, B(E2), B(M1). Comparison with beyond-mean-field calculations, and with previous experimental results for level half-lives. Systematics of the experimental B(E2) values for the first 2+ states in even-mass Cd and Sn isotopes.
NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Cd; calculated energies and B(E2) of the first 2+ and 4+ states, potential energy surfaces (PES) in (β2, γ) plane using particle-number variation-after-projection (PNVAP) method, and collective wave functions (CWFs) contours for the first 2+ and 4+ states in (β2, γ) plane. 106Cd; calculated levels, J, π, collective wave functions (CWFs) contours in (β2, γ) plane. State-of-the-art beyond mean-field calculations using the symmetry-conserving configuration-mixing (SCCM) approach, and Gogny-D1S interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.034320