Abstract
The ratio P of the probability of exciting the K shell of copper by direct cathode-ray impact to the probability of exciting the same shell by fluorescence in a thick target, is measured with normally emergent rays over a range of voltages extending from 2 to 17.4 times the K excitation voltage. P is found to vary from 6.63 at U=2 to 7.2 at U=17.4, where U is the ratio of tube voltage to K excitation voltage. The ratio Q of the probability of a cathode ray ionizing the K shell directly to the probability of a cathode ray exciting a continuous quantum of frequency greater than the K-limit frequency is found to be very nearly constant at 3.5 for the same voltage range. The variation of P with Z is examined theoretically and compared with experiment showing a lack of good agreement.

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