Yb+ ions confined in a rf trap disappear due to some background gases when the Yb+ ions are in excited states. We examined O2, H2O, and H2 as the test background gas. We found that O2 gas enhanced the disappearance to a large degree, as did H2O gas to some degree, but H2 gas had little effect.
It is known that fluorescence of trapped Yb+ ions fades with continuous driving of the 2S1/2${\mathrm{\ensuremath{-}}}^{2}$P1/2 transition in the presence of buffer gases. This phenomenon has been interpreted as being caused by population trapping in the 2F7/2 state of Yb+ . As another cause of the fluorescence disappearance, we found the production of YbH+ by chemical reaction of Yb+ in excited states with H2 gas. We found that the wavelengths of 369.482, 369.202, and 368.947 nm, formerly assigned as wavelengths for deexcitation of Yb+ in the 2F7/2 state to the 2S1/2 ground state, are actually photodissociation lines of YbH+ . The change of the resonance point of rf resonance absorption signals indicates the production and dissociation of YbH+ ions. The production of YbH+ may be a problem in establishing frequency standards using buffer-gas-cooled Yb+ , owing to difficulty in removing H2 gas from vacuum systems.
The storage time of Yb+ ions trapped in an r.f. trap was determined by the rf resonance absorption method in the presence of buffer gas, without and with laser radiation of a frequency equal to the transition from the S1/2 ground state to the excited P1/2 state. The storage time of the ions with the buffer gas (presure between 1 × 10−4 and 4·2 × 10−4 Pa) was several hours without the laser radiation; this period was shortened to several hundred seconds by irradiation with a 500 nW laser source. This phenomenon shows that the trapped Yb+ ions disappeared from the trap as a result of irradiation with the resonance laser light.
We report on a study to determine the efficiency of various buffer gases in quenching the population trapping states of laser-excited ytterbium ions. The ions were confined in an rf-dc hybrid trap, and their 2S1/2${\mathrm{\ensuremath{\leftrightarrows}}}^{2}$P3/2 transition was excited with 329-nm laser light. Buffer gases used include H2, N2, CO2, Ar, and He at several different pressure regimes. We have identified N2 to be highly efficient in quenching the population of the trapping states and thus be the most suitable buffer gas to use with ytterbium for the development of a trapped-ion microwave frequency standard.
Characteristics of the Yb+ ion cloud trapped in a rf trap in the presence of He buffer gas were determined by fluorescence detection as well as the rf resonance method. Combining the results obtained by the two methods, we determined the spatial ion density distribution and found that the trapped ions were thermalized by collisions with the He buffer gas. It was confirmed by both methods that the harmonic motion of the trapped ions was excited by the trapping field leaked to the rf resonance detection circuit (subharmonic oscillation), and moreover, by the fluorescence detection method, that the probing rf field used for the rf resonance method was indispensable as “the initial push” for exciting the amplitude.
We report on a study to determine the efficiency of various buffer gases in quenching the population trapping states of laser excited ytterbium ions. The ions were confined in an rf/dc hybrid trap, and their /sup 2/S/sub 1/2//spl hArr//sup 2/P/sub 3/2/ transition was excited with 329 nm laser light. Buffer gases used include H/sub 2/, N/sub 2/, CO/sub 2/, Ar, and He at several different pressure regimes. We have identified N/sub 2/ to be highly efficient in quenching the population of the trapping states, and thus be the most suitable buffer gas to use with ytterbium for the development of a trapped ion microwave frequency standard.
Resonant laser excitation of Yb ions confined in an rf ion trap is found to result in perfect population trapping in the highly metastable 2F7/2 state. The lifetime of this level is measured to be greater than 8 days. Population and depopulation of this level under narrow- and broad-band laser excitation conditions is investigated and its potentiality for ultimate-resolution laser spectroscopy indicated.