1985
DOI: 10.1007/bf01411951
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Transitions between Zeeman substates of excited He I levels induced by electric radiofrequency fields

Abstract: Making use of the large tensor polarizabilities of excited He I levels, transitions between Zeeman substates of 1 snd 1D 2 levels have been induced by electric radiofrequency fields after ion-impact excitation of He atoms. Resonance signals have been observed near the Larmor frequency co=coL as well as near co = 2co L. These signals are interpreted as 2-quantum electric-dipole (2El) transitions and 1El transitions, respectively, between the Zeeman sublevels with M=0 and M= _+2. The interaction of this 3-state … Show more

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Cited by 7 publications
(2 citation statements)
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“…4b) from the level crossing signals (Fig. 3), the recording was fitted using a superposition of three Lorentz functions with a fixed FWHM AB¢=h/(z.gj.#B) where = 38.7 ns is the radiative lifetime of the 41D level [21]. Due to the deflection of the ion beam in the magnetic field B=, a slight linear slope of the background intensity had to be taken into account.…”
Section: A) H~ + (D2 )-He Collisionsmentioning
confidence: 99%
“…4b) from the level crossing signals (Fig. 3), the recording was fitted using a superposition of three Lorentz functions with a fixed FWHM AB¢=h/(z.gj.#B) where = 38.7 ns is the radiative lifetime of the 41D level [21]. Due to the deflection of the ion beam in the magnetic field B=, a slight linear slope of the background intensity had to be taken into account.…”
Section: A) H~ + (D2 )-He Collisionsmentioning
confidence: 99%
“…For the measurements being considered in this paper, it is more favourable to apply this rf electric resonance technique than the rf magnetic resonance technique [6] usually used for high-resolution measurements of energy spacings between equal parity states. This can be seen by estimating the rf power [7] needed for each case.…”
Section: Introductionmentioning
confidence: 99%