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The displacement 2²S1/2-2²P1/2 in singly ionized helium has been determined to be 14,020±{}100 mc/sec. The method is analogous to that employed for hydrogen by Lamb and Retherford, except that no beam of metastable ions is formed. Instead, helium atoms are bombarded by electrons of a few hundred volts energy. In about one percent of the ionizing collisions, the remaining atomic electron is excited to the metastable 2²S1/2 state of the ion. When the bombardment region is illuminated with microwave radiation of the proper frequency, transitions to the 2²P1/2 state are induced, and the ultraviolet photons emitted in the subsequent decay to the ground state 1²S1/2 are detected by a suitable photoelectric detector. Background effects due to metastable atoms and radiation from HeI are reduced by the use of a collodion film filter. Our experimental value for the 2²S1/2-2²P1/2 level shift is about 1.4 percent higher than the present theoretical value.
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Lamb et al. (1950) studied this question.
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