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Program - Brookhaven National Laboratory

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Materials and Measurements, Retieseweg 111, B-2440 Geel, Belgium. A.Klix, Institute for Neutron<br />

Physics and Reactor Technology, Karlsruhe Institute of Technology, D-76344 Eggenstein-Leopoldshafen,<br />

Germany. A. Buffler, D. Geduld, Department of Physics, University of Cape Town, Private Bag,<br />

Rondebosch 7701, South Africa. F. D. Smit, C. Vermeulen, P. Maleka, R. T. Newman, iThemba LABS, P<br />

O Box 722, Somerset West, 7129, South Africa. R. Nolte, Physikalisch-Technische Bundesanstalt,<br />

Bundesallee 100, D-38116 Braunschweig, Germany. A. Wallner, Faculty of Physics, Univ. of Vienna,<br />

VERA <strong>Laboratory</strong>, Waehringer Strasse 17, A-1090 Vienna, Austria.<br />

The process of neutrinoless double beta decay (0νββ) plays a key role in modern neutrino physics. The<br />

experiments on the 76 Ge-0νββ-decay using germanium-semiconductors are at the forefront in this field. Due<br />

to the extremely low count rates expected for this rare decay, any kind of background event in the detector,<br />

especially at energies close to Qββ = 2039 keV has to be avoided. Therefore, a careful investigation on the<br />

neutron-induced background was carried out. In this contribution the results of the search for a potentially<br />

existing 2040.7 keV gamma-ray, which occurs due to de-excitation of the 69 th excited state of 76 Ge, will<br />

be presented. In order to verify the existence of this weak transition the gamma rays occurring due to the<br />

β-decay of the short living 76 Ga (T 1/2 = 32.6 s) into 76 Ge was studied. Therefore, the 14 MeV high-flux DT<br />

neutron generator of the TU Dresden, equipped with an automatic pneumatic sample transport system,<br />

was employed. Furthermore, first and new results on cross sections for inelastic neutron scattering into the<br />

69 th excited state of 76 Ge, measured at the GAINS setup of the IRMM in Geel, will be shown. The decay<br />

of 68 Ge is a major source of intrinsic background nuclides in germanium semiconductor detectors. This<br />

nuclide is produced from other germanium isotopes in x Ge(n,jn) 68 Ge reactions induced by cosmogenic<br />

neutrons. First measurements for the production cross section of 68 Ge with fast quasi monoenergetic<br />

neutrons (En > 20 MeV) were performed at iThemba LABS using the activation foil method. Within<br />

these studies on 76 Ge, the electron capture of 76 As has been observed for the first time, whose results will<br />

be presented.<br />

HD 7 5:30 PM<br />

Gamma-ray Spectroscopy of 30 P<br />

Elaine McNeice, Kiana Setoodehnia, Balraj Singh, Alan A. Chen, Jun Chen<br />

Department of Physics and Astronomy, McMaster University, Canada<br />

Yasuyuki Abe, Shota Fukuoka, Yoko Ishibashi, Tetsuro Komatsubara, Daisuke Nagae, Akira Ozawa<br />

Division of Physics, the University of Tsukuba, Japan<br />

Takehito Hayakawa<br />

Japan Atomic Energy Agency, Japan<br />

David Kahl, Shigeru Kubono, Hiroshi Suzuki, Hidetoshi Yamaguchi<br />

Nishina Center, the University of Tokyo, Wako Branch at RIKEN, Japan<br />

30 P is an N=Z=15 odd-odd nuclide whose level density is reasonably high (34 proton-bound excited states,<br />

S(p)=5594.5 keV). Also states with isospin T=0 and T=1 coexist from the ground state upwards. Therefore<br />

30 P spectroscopy provides an experimental test of the effect of isospin symmetry breaking on level structure.<br />

Moreover, the proton-resonance structure of 30 P determines the 29 Si(p,γ) 30 P reaction rate at a temperature<br />

characteristic of explosive hydrogen burning in supernovae type Ia. The 29 Si(p,γ) 30 P reaction has recently<br />

[1] been identified as one of top ten proton-capture reactions important for supernova nucleosynthesis.<br />

We have studied 30 P levels up to 7.2 MeV via in-beam γ-ray spectroscopy using the 28 Si( 3 He,pγ) 30 P<br />

reaction at the University of Tsukuba Tandem Accelerator Complex in Japan. An energy level scheme was<br />

deduced from γ-γ coincidence measurements. Furthermore, spin assignments based on measurements of<br />

γ-ray angular distributions and γ-γ directional correlation of oriented nuclei (DCO ratios) were made for<br />

124

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