2011
DOI: 10.1103/physrevlett.106.213001
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Pulsed Sisyphus Scheme for Laser Cooling of Atomic (Anti)Hydrogen

Abstract: We propose a laser cooling technique in which atoms are selectively excited to a dressed metastable state whose light shift and decay rate are spatially correlated for Sisyphus cooling. The case of cooling magnetically trapped (anti)hydrogen with the 1S-2S-3P transitions by using pulsed ultraviolet and continuous-wave visible lasers is numerically simulated. We find a number of appealing features including rapid three-dimensional cooling from ∼1 K to recoil-limited, millikelvin temperatures, as well as suppres… Show more

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Cited by 21 publications
(28 citation statements)
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“…Thus, while laser cooling for a confined Ps gas can be envisioned [676], the effects of confinement would have to be explicitly addressed, either by using sufficiently large cavities or other confining structures [123], or possibly by using alternative cooling schemes employing short-pulsed lasers (e.g. [677,678]). …”
Section: Bose-einstein Condensationmentioning
confidence: 99%
“…Thus, while laser cooling for a confined Ps gas can be envisioned [676], the effects of confinement would have to be explicitly addressed, either by using sufficiently large cavities or other confining structures [123], or possibly by using alternative cooling schemes employing short-pulsed lasers (e.g. [677,678]). …”
Section: Bose-einstein Condensationmentioning
confidence: 99%
“…With the recent trapping of anti-hydrogen in its ground state, a larger beam would also prove beneficial in mitigating the difficulties created by the low number of trapped anti-hydrogen atoms available [12,13]. However, we are mainly motivated to develop a power scalable 243 nm laser in order to explore proposals to laser cool atomic hydrogen using the 1S-2S transition [14][15][16].…”
Section: Introductionmentioning
confidence: 99%
“…Two photon laser cooling could be more rapid and flexible than the more traditional approach using Lyman-alpha radiation at 121.6 nm -mostly due to the greater ease at producing radiation at 243 nm. To obtain reasonable scattering rates with such schemes requires that the 2S state is coupled to a state with short lifetime, for instance either the 2P [15] or 3P [16] states, and the average power of the cavity enhanced 243 nm radiation source should be at the ∼100 W level. For a beam diameter of ∼ 500 µm, this would lead to a scattering rate of ∼500 Hz when maximally coupling the 2S and 2P states [15].…”
Section: Introductionmentioning
confidence: 99%
“…Then isolating the z component of F = m d 2 r dt 2 , an oscillatory equation of motion is found: 14) where ω z = qV 0 md 2 . In thex andŷ directions, however, the equations of motion have only exponential, and therefore unconfined, solutions.…”
Section: Single Particle Confinementmentioning
confidence: 99%
“…Moreover, to assist spectroscopic efforts, there are a number of schemes to further cool and de-excite the antihydrogen atoms to the ground state [12][13][14].…”
Section: Precision Comparison Of the Properties Of Hydrogen And Antihmentioning
confidence: 99%