Collectivity and Configuration Mixing in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi>Pb</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>186</mml:mn><mml:mo>,</mml:mo><mml:mn>188</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi>Po</mml:mi><mml:mprescripts/><mml:none/><mml:mn>194</mml:mn></mml:mmultiscripts></mml:math>
T. GrahnDepartment of Physics, University of Jyväskylä, P. O. Box 35, FI-40014 Jyväskylä, FinlandΑ. DewaldInstitut fu r Kernphysik, Universita t zu Ko ln, Zu lpicher Strae 77, 50937 Ko ln, GermanyO. MöllerInstitut fu ¨r Kernphysik, Universita ¨t zu Ko ¨ln, Zu ¨lpicher Straße 77, 50937 Ko ¨ln, GermanyR. JulinDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandC. W. BeausangWright Nuclear Structure Laboratory, Yale University, New Haven, Connecticut 06520, USAStephan ChristenInstitut fu r Kernphysik, Universita t zu Ko ln, Zu lpicher Strae 77, 50937 Ko ln, GermanyI. G. DarbyDepartment of Physics, Oliver Lodge Laboratory, University of Liverpool, Liverpool L69 7ZE, United KingdomS. EeckhaudtDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandP. T. GreenleesDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandA. GörgenK. HelariuttaLaboratory of Radiochemistry, University of Helsinki, P. O. Box 55, FI-00014 Helsinki, FinlandJ. JolieInstitut fu r Kernphysik, Universita t zu Ko ln, Zu lpicher Strae 77, 50937 Ko ln, GermanyPeter G. JonesDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandS. JuutinenDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandH. KettunenDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandT. KröllPhysik-Department E12, TU Mu ¨nchen, 85748 Garching, GermanyR. KrückenPhysik-Department E12, TU Mu ¨nchen, 85748 Garching, GermanyY. Le CozCEA-SACLAY, DSM/DAPNIA/SPhN, F-91191 Gif-sur-Yvette Cedex, FranceM. LeinoDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandA.-P. LeppänenDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandP. MaierbeckPhysik-Department E12, TU Mu ¨nchen, 85748 Garching, GermanyDavid MeyerWright Nuclear Structure Laboratory, Yale University, New Haven, Connecticut 06520, USAB. MelonInstitut fu r Kernphysik, Universita t zu Ko ln, Zu lpicher Strae 77, 50937 Ko ln, GermanyP. NieminenDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandM. NymanDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandR. D. PageDepartment of Physics, Oliver Lodge Laboratory, University of Liverpool, Liverpool L69 7ZE, United KingdomJ. PakarinenDepartment of Physics, Oliver Lodge Laboratory, University of Liverpool, Liverpool L69 7ZE, United KingdomP. PetkovInstitute for Nuclear Research and Nuclear Energy, Sofia, BulgariaP. RahkilaDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandBidhan C. SahaInstitut fu r Kernphysik, Universita t zu Ko ln, Zu lpicher Strae 77, 50937 Ko ln, GermanyM. SandzeliusDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandJ. SarénDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandC. ScholeyDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, FinlandJ. UusitaloDepartment of Physics, University of Jyva ¨skyla ¨, P. O. Box 35, FI-40014 Jyva ¨skyla ¨, Finland
2006lv
ABI
Аннотация
Lifetimes of prolate intruder states in $^{186}\mathrm{Pb}$ and oblate intruder states in $^{194}\mathrm{Po}$ have been determined by employing, for the first time, the recoil-decay tagging technique in recoil distance Doppler-shift lifetime measurements. In addition, lifetime measurements of prolate states in $^{188}\mathrm{Pb}$ up to the ${8}^{+}$ state were carried out using the recoil-gating method. The $B(E2)$ values have been deduced from which deformation parameters $|{\ensuremath{\beta}}_{2}|=0.29(5)$ and $|{\ensuremath{\beta}}_{2}|=0.17(3)$ for the prolate and the oblate bands, respectively, have been extracted. The results also shed new light on the mixing between different shapes.
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