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For a variety of radionuclides which decay via $beta^{-}$ and a weak $beta^{+}$-channel the electron-capture (EC) is not observed yet. As the interest of exact decay characteristica increased again, not least with the need of reliable data for experiments on investigation of the neutrinoless double-beta-decay, an experiment for the investigation of the $^{76}$As-EC was performed. The first time observation of the EC of $^{76}$As by this experiment resulted in a total branching-ratio for the EC / $beta^{+}$-channel of $p_mathrm{EC} = 0.0269 pm left(0.0080(mathrm{stat.}) pm 0.0029(mathrm{sys.}) right)$ and $p_mathrm{EC} = 0.0263 pm left(0.0077(mathrm{stat.}) pm 0.0047(mathrm{sys.}) right)$ according to two different methods. For the branching of this decay-channel into the first excited- and the ground state of gess a limit was obtained.
Two-neutrino double electron capture ($2 u$ECEC) is a second-order Weak process with predicted half-lives that surpass the age of the Universe by many orders of magnitude. Until now, indications for $2 u$ECEC decays have only been seen for two isotop
The photon spectrum accompanying the orbital K-electron capture in the first forbidden unique decay of 81Kr was measured. The total radiation intensity for the photon energies larger than 50 keV was found to be 1.47(6) x 10^{-4} per K-capture. Both t
We report the first observation of the parity-violating 2.2 MeV gamma-ray asymmetry $A^{np}_gamma$ in neutron-proton capture using polarized cold neutrons incident on a liquid parahydrogen target at the Spallation Neutron Source at Oak Ridge National
Neutrino accompanied double beta-decay of Ge-76 can populate the ground state and the excited states of Se-76. While the decay to the ground state has been observed with a half-life of 1.74 +0.18 -0.16 10^21 years, decays to the excited states have n
The lifetimes of the first 2$^{+}$ states in the neutron-deficient $^{76,78}$Sr isotopes were measured using a unique combination of the $gamma$-ray line-shape method and two-step nucleon exchange reactions at intermediate energies. The transition ra