2018
DOI: 10.1364/ol.43.001375
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Cavity-enhanced deep ultraviolet laser for two-photon cooling of atomic hydrogen

Abstract: We demonstrate a 650 mW 243 nm continuous-wave laser coupled to a linear optical enhancement cavity. The enhancement cavity can maintain >30  W of intracavity power for 1 h of continuous operation without degradation. This system has sufficient power for a demonstration of two-photon laser cooling of hydrogen and may be useful for experiments on other simple two-body atomic systems.

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Cited by 21 publications
(23 citation statements)
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References 34 publications
(48 reference statements)
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“…4), at least 10% of the molecules are photodissociated, for laser fluxes of ∼10 20 photons cm −2 s −1 . A buildup cavity with finesse of up to 1000 [27] must be implemented for the 100 W photodissociation laser at 266 nm [28]. Use of HI/DI can shift the photodissociation to 355 nm where there are more powerful lasers.…”
Section: Description Of the Methodsmentioning
confidence: 99%
“…4), at least 10% of the molecules are photodissociated, for laser fluxes of ∼10 20 photons cm −2 s −1 . A buildup cavity with finesse of up to 1000 [27] must be implemented for the 100 W photodissociation laser at 266 nm [28]. Use of HI/DI can shift the photodissociation to 355 nm where there are more powerful lasers.…”
Section: Description Of the Methodsmentioning
confidence: 99%
“…The increased atom-laser interaction time will compensate for the lower available power compared to a pulsed laser. These new converters combined with the recent demonstration of high-power CW lasers at 243/244 nm [35,36] that can be cavity enhanced to more than 33 W of intracavity power [37] will enable an improved measurement of the 1S-2S transition frequency by three orders of magnitude which is the aim of the ongoing Mu-MASS experiment.…”
Section: S-2s Transitionmentioning
confidence: 99%
“…While many areas in research and industry have and continue to benefit from these sources [1][2][3], the lack of wavelength selectivity and frequency resolution limits research in atomic, molecular, and optical physics. For example, access to single photon Rydberg excitation [4], Rydberg dressing [5], tight optical lattices [6] and precise determination of physical constants [7] all require tunable, wattlevel, DUV laser light with application-specific wavelengths. The development of these laser sources is also crucial to the burgeoning field of direct molecular laser cooling [8,9] as several promising candidates possess strong optical transitions with high saturation intensities in the DUV, e.g., AlF, AlCl [10][11][12], leading to large recoil velocities and the potential for significant light-mediated forces.…”
Section: Introductionmentioning
confidence: 99%