JOSHI, P.; JENKINS, D.G.; RADDON, P.M.; SIMONS, A.J.; WADSWORTH, R.; WILKINSON, A.R.; FOSSAN, D.B.; KOIKE, T.; STAROSTA, K.; VAMAN, C.; TIMAR, J.; DOMBRADI, Zs.; KRASZNAHORKAY, A.; MOLNAR, J.; SOHLER, D.; ZOLNAI, L.; ALGORA, A.; PAUL, E.S.; RAINOVSKI, G.; GIZON, A.; GIZON, J.; BEDNARCZYK, P.; CURIEN, D.; DUCHENE, G.; SCHEURER, J.N.

doi:10.1016/j.physletb.2004.05.066

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Physics Letters B. 2004, vol. 595, p. 135-142

Elsevier

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136 P. Joshi et al. / Physics Letters B 595 (2004) 135–142AbstractThe nucleus 106Rh was populated using the reaction 96Zr(13C, p2n) at a beam energy of 51 MeV. γ -ray transitions wereidentified using the EUROBALL-IV γ -ray spectrometer and the DIAMANT charged particle array. The yrast band, which isbased upon a πg−19/2 ⊗ νh11/2 configuration, has been extended to I π = (22−). A new I = 1 band has been identified whichresides ∼ 300 keV above the yrast band. Core–quasiparticle coupling model calculations show reasonably good agreement withthe data. The properties of the two pairs of strongly coupled bands are consistent with a chiral interpretation for these states. 2004 Elsevier B.V< Leer menos

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Stability of chiral geometry in the odd-odd Rh isotopes: spectroscopy of $^{106}$Rh

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