Abstract
The absolute intensity of x-rays/RaD disintegration () has been measured to be ±0.02 by argon-filled proportional counter spectrometry on carrier-free RaDEF equilibrium sources, and the relative intensities were found to be . The intensity of x-rays relative to that () of the single, 46.5-kev, pure gamma ray is . Care was taken to avoid error due to wall-effects and the counting techniques were varied and cross-checked so as to eliminate possible systematic errors. The absolute intensity of the gamma ray is from data taken on a 3×3 inch NaI(Tl) scintillation spectrometer. Assuming the number of -shell ionizations/RaD disintegration () to be 0.62, the mean -fluorescence yield () of bismuth is 0.38±0.02, which when combined with the ratio , leads to an experimental value of the total -shell conversion coefficient (), which thus is 13.3±2.0, the major error arising from the correction of for the contribution due to Compton backscattering, which amounts to some 10 to 20% depending on exact conditions of geometry and collimation. The value of the -conversion coefficient interpolated from Rose's tables is 17.85, based on a point-charge nucleus. Better agreement is obtained with a value of about 12.7 from theoretical calculations of Sliv and Listengarten, who included a correction for the finite size of the nucleus.
A new summary of mean -fluorescence yields from nuclear excitation is presented which shows that the mean yields depend strongly upon the relative number of vacancies in the respective subshells.
- Received 26 December 1956
DOI:https://doi.org/10.1103/PhysRev.106.266
©1957 American Physical Society