Absolute E1 and E2 transition rates in $^{110}$Cd

L.K. Kostov; W. Andrejtscheff; L.G. Kostova; L. Käubler; H. Prade; R. Schwengner

doi:doi:10.1007/s100500050119

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2018 Impact factor 2.481

Hadrons and Nuclei

Eur. Phys. J. A 2, 269-273

Absolute E1 and E2 transition rates in ¹¹⁰Cd

L.K. Kostov¹ - W. Andrejtscheff¹ - L.G. Kostova¹ - L. Käubler² - H. Prade² - R. Schwengner²

¹ Bulgarian Academy of Sciences, Institute for Nuclear Research and Nuclear Energy, Tzarigradsko Chaussée 72, BG-1784 Sofia, Bulgaria
² Institute of Nuclear and Hadronic Physics of FZR, D-01314 Dresden, Germany

Received: 4 December 1997 / Revised version: 15 April 1998 Communicated by D. Schwalm

Abstract
The lifetimes of several states in ¹¹⁰Cd have been determined by means of the generalized centroid-shift method. The reaction ¹⁰⁸Pd( $\alpha$ ,2n) has been used and the following results were obtained: T_1/2(2879 keV) = 0.60 $\pm$ 0.10 ns, T_1/2(3029 keV) = 0.30 $\pm$ 0.10 ns, T_1/2(3056 keV) = 2.25 $\pm$ 0.10 ns, T_1/2(3611 keV) = 0.45 $\pm$ 0.10 ns. Electric dipole and quadrupole transitions are discussed in terms of octupole and quadrupole collectivity. The odd-spin sequence of the semi-aligned structure $\nu$ (h_11/2d_5/2) has been established with the band-head at J $^{\pi}$ = 7^-₂ identified as a new two-quasiparticle isomer, the lower-lying 5^-_1,2 states being of two-quasiproton character.
to 0ptNuclear Reaction: ¹⁰⁸Pd( $\alpha$ ,2n), E = 27 MeV,; measured E $_{\gamma}$ , I $_{\gamma}$ , $\gamma$ -r.f. Deduced: T_1/2, B( $\alpha$ L) in ¹¹⁰Cd. Ge detectors. Generalized centroid-shift analysis.