Abstract
Critical radiation potentials for iron, determined photo-electrically.—Electrons were accelerated from a filament heated by a constant current, to an iron plate, and the photo-electric effect of the radiation excited on a plate carefully shielded from stray electrons, was measured. All surfaces exposed to the radiation were of metal and were maintained at definite potentials, and the tube after thorough baking was maintained at a pressure of mm or less during measurements. (1) series, 40 to 175 volts. Nine critical potentials were observed, the corresponding values being 3.46, 6.03, 7.05, 8.21, 9.63, 10.40, 10.88, 11.33 and 11.83, where is the Rydberg frequency. The first and third are interpreted as resonance potentials of the , series, the others as belonging to the series. The difference in for the two levels comes out 2.58. (2) series, 600 to 700 volts. The three points observed correspond to Sommerfeld's , and , the values being 45.5, 47.0, and 51.5. These agree well with x-ray data.
Ionizing potentials for iron. The convergence limit of series is which should correspond to an ionizing potential for that level. For the L series, the value for comes out .
Extreme ultra-violet spectrum of iron, 1188 to 18 A.—The critical potentials are interpreted as corresponding to emission lines of wave-length 264, 151, 129.6, 111.0, 94.6, 87.8, 83.9, 80.5 and 77.0 A. Differences between various pairs of the values correspond closely with eleven wave-lengths, from 294 to 1188 A, measured by Millikan, indicating that these belong to combination series. The L potentials correspond to 20.0, 19.4 and 17.7 A.
- Received 20 May 1923
DOI:https://doi.org/10.1103/PhysRev.23.35
©1924 American Physical Society