By O. Kofoed-Hansen, C. J. Christensen (auth.), S. Flügge (eds.)
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39 is the existence of several" unfavoured" transitions with very low loglo It values. These values are hard to distinguish from some of the values attributed to superallowed decays and Table 3. 4. they are classified as unfavoured transitions Transition Spin Decay log" fl merely because they belong to decays of relatively heavy nuclei. The cases of 0+-+1+ Nd140 K 3·7 loglolt<4,4 are summarized in Table 3. 1 these transitions. 4 a rule provided by the decays of (14 and P32. Concluding this section we may remark that the allowed unfavoured transitions show a remarkable spread in loglo It values and that the highest and lowest values are based on extremely reliable experimental information.
3) A neutron is created and is slowed down and diffuses around until it is captured. In the capture the binding energy is emitted as y-rays. These y-rays give rise to electrons which may be detected. The neutron capture occurs delayed relative to the initial events. The y-ray energy is given by the binding energy. This sequence of events is illustrated in Fig. 33 and the instrument used is shown in Fig. 34. The main difficulty is the rarity of. genuine events due to the smallness of the cross section for neutrino absorption.
4°; (3) 175°]. - S G chosen as the one giving the best fit to the experimental polarization results. 46. Curve showing corresponding values of :Ie and y, as defined in Eqs.
Beta Decay / Betazerfall by O. Kofoed-Hansen, C. J. Christensen (auth.), S. Flügge (eds.)