2010
DOI: 10.1134/s0021364010220133
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Sub-doppler laser cooling of thulium atoms in a magneto-optical trap

Abstract: We have experimentally studied sub-Doppler laser cooling in a magneto-optical trap for thulium atoms working at the wavelength of 410.6 nm. Without any dedicated molasses period of sub-Doppler cooling, the cloud of 3 × 10 6 atoms at the temperature of 25(5) µK was observed. The measured temperature is significantly lower than the Doppler limit of 240µK for the cooling transition at 410.6 nm. High efficiency of the sub-Doppler cooling process is due to a near-degeneracy of the Landé-g factors of the lower 4f 13… Show more

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Cited by 19 publications
(10 citation statements)
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“…As a consequence, the Doppler temperature is close to a mK. Such a high temperature makes direct loading from a MOT into a dipole trap difficult and inefficient, even when sub-Doppler mechanisms take place [14,15]. To further decrease the temperature of atoms prior to the dipole trap loading, an additional MOT stage based on an ultra-narrow kHzlinewidth transition was applied in Refs.…”
mentioning
confidence: 99%
“…As a consequence, the Doppler temperature is close to a mK. Such a high temperature makes direct loading from a MOT into a dipole trap difficult and inefficient, even when sub-Doppler mechanisms take place [14,15]. To further decrease the temperature of atoms prior to the dipole trap loading, an additional MOT stage based on an ultra-narrow kHzlinewidth transition was applied in Refs.…”
mentioning
confidence: 99%
“…An unusual, anisotropic sub-Doppler cooling effect was observed inside these Er, Dy, and Tm MOTs [167,227,[230][231][232]. The effect is a consequence of the fact that the Landé g factors of the ground and excited states are nearly the same, yielding nearly zero differential Zeeman shift on the cooling transition.…”
Section: Optical Cooling Trapping and Evaporative Cooling Of Open-she...mentioning
confidence: 87%
“…The corresponding boundaries will be S b1 = 5 × 10 −5 and S b2 = 7×10 −4 (comparable to the values for a 87 Rb MOT [29] of S b1 = 9 × 10 −5 and S b2 = 6 × 10 −4 ). For a typical first-stage Tm MOT [20], we use S 0 ≈ 0.1 and ∆ ≈ −Γ, which corresponds to the case S = 0.02 ≫ S b2 . In this case the width of the polarization gradient resonance is large enough to play a dominant role in the cooling process, resulting in a regular one-temperature Maxwellian distribution of atoms [ Fig.…”
Section: B the Symmetric Regimementioning
confidence: 99%
“…For nearly all transitions involved in laser cooling of hollow-shell lanthanides, the magnetic Landé g-factors of the upper and lower cooling levels are close to each other [18,19]. As a result, efficient sub-Doppler cooling was observed directly in the first-stage MOT of Tm [20], Dy [21], Er [22] and Ho [7] even in the presence of a strong magnetic field gradient. However, sub-Doppler cooling in the second-stage MOT has not been reported yet.…”
Section: Introductionmentioning
confidence: 99%