Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physical Review A

Laser cooling of cesium atoms in gray optical molasses down to 1.1 μK

Denis Boiron, A. Michaud, P. Lemonde, Yvan Castin, Ch Salomon, S. Weyers, K. Szymaniec, Laurent Cognet, Andr  Clairon

Published Jun 1, 1996• 91 citations
Publisher

Abstract

We have studied the behavior of cesium atoms cooled in six-beam "gray" optical molasses. Cooling occurs for a laser detuned to the blue side of the $6{S}_{\frac{1}{2}}$, $F=3\ensuremath{\rightarrow}6{P}_{\frac{3}{2}}$, ${F}^{\ensuremath{'}}=2$ transition, and a Sisyphus-type effect accumulates the atoms in states not coupled to the light. We measure a minimum temperature of 1.1\ifmmode\pm\else\textpm\fi{}0.1 \ensuremath{\mu}K at low atomic density. The typical cooling time is on the order of 1 ms. A linear dependence of the temperature versus atomic density is found with a slope of \ensuremath{\sim}0.6 \ensuremath{\mu}K/(${10}^{10}$ atoms/${\mathrm{cm}}^{3}$).

DOI
10.1103/physreva.53.r3734

Related papers

Three-dimensional cooling of cesium atoms in four-beam gray optical molasses

Denis Boiron, C. Triché, D. R. Meacher +2 more

We report the observation of three-dimensional cooling of cesium atoms using a four-beam optical molasses tuned to the blue side of the ${\mathit{F}}_{\mathit{g}}$=3\ensuremath{\rightarrow}${\mathit{F}}_{\mathit{e}}$=2 hyperfine component of the 6${\mathit{S}}_{1/2}$\ensuremath{\rightarrow}6${\mathit{P}}_{3/2}$ transition. The cooling mechanism is a Sisyphus effect involving atomic states that are nearly uncoupled from the light field. Starting from a magneto-optical trap at 70 \ensuremath{\mu}K, the cooling time was on the order of 1 ms with almost 100% capture efficiency and temperature smaller than 5 \ensuremath{\mu}K measured. We also present a probe transmission spectrum showing that almost all the atoms are found in the nearly dark states.

Physical Review A•Nov 1, 1995•68 citations

Laser Cooling of Cesium Atoms Below 3 μK

Ch Salomon, Jean Dalibard, William D. Phillips +2 more

We have measured the temperature of cesium atoms released from optical molasses. For a wide range of laser intensity and detuning from resonance, the temperature depends only on the intensity-to-detuning ratio. The lowest temperature achieved is (2.5 ± 0.6) μK, which corresponds to an r.m.s. velocity of 12.5 mm/s or 3.6 times the single-photon recoil velocity. This is, to our knowledge, the coldest kinetic temperature ever measured for three-dimensional (3D) cooling.

Europhysics Letters (EPL)•Aug 15, 1990•239 citations

Experimental study on laser cooling of cesium atoms by optical molasses

Jidong Hou, LI Yi-min, Donghai Yang +1 more

We have studied the relationship between the temperature of Cs cold atoms and the parameters of the cooling laser. The atoms are first cooled and captured by a magneto-optical trap and then further cooled by optical molasses. The temperature of atoms is measured by a time-of-flight method. For relatively large laser intensity and small detuning, the temperature depends linearly on the intensity-to-detuning ratio, and nonlinear relationship has also been found in other case.

Acta Physica Sinica (Overseas Edition)•Dec 1, 1998•2 citations

Laser cooling: Beyond optical molasses and beyond closed transitions

Vladan Vuletić

We present a simple and general optical cooling method based on 3D degenerate Raman sideband cooling with adiabatic release that goes significantly beyond the density and temperature limitations of optical molasses. In 10 ms we cool a sample of 3×108 cesium atoms to a temperature of 330 nK at a density of 1.1×1011 cm−3, which corresponds to a phase-space density nλdB3=1/500.We further propose to cool atoms or molecules inside an optical cavity that enhances the scattering of blue-detuned photons and show that the dissipative mechanism can be viewed as a cavity-induced generalized Doppler cooling. Since the cooling depends on the atom’s internal level structure only through the photon scattering rate, cavity Doppler cooling is applicable to particles that do not possess a closed optical transition, which may allow one to extend laser cooling to a greater class of atoms or molecules. Large samples are cooled at the same rate as single atoms if the effect of one atom on the cavity resonance frequency is small. We also show how to achieve 3D cooling with a single optical cavity.

AIP conference proceedings•Jan 1, 2001•0 citations

Gray-molasses cooling of 39 K to a high phase-space density

Guillaume Salomon, Lauriane Fouché, Pengjun Wang +3 more

We present new techniques in cooling 39 K atoms using laser light close to the D1 transition.First, a new compressed-MOT configuration is taking advantage of gray-molasses-type cooling induced by blue-detuned D1 light.It yields an optimized density of atoms.Then, we use pure D1 gray molasses to further cool the atoms to an ultra-low temperature of 6 μK.The resulting phase-space density is 2 × 10 -4 and will ease future experiments with ultracold potassium.As an example, we use it to directly load up to 3 × 10 7 atoms in a far detuned optical trap, a result that opens the way to the all-optical production of potassium degenerate gases.

arXiv:1310.4014•Europhysics Letters (EPL)•Dec 1, 2013•112 citations

Sub-Doppler cooling of sodium atoms in gray molasses

Giacomo Colzi, Gianmaria Durastante, Eleonora Fava +3 more

We report on the realization of sub-Doppler laser cooling of sodium atoms in gray molasses using the ${D}_{1}$ optical transition $(3s\phantom{\rule{0.16em}{0ex}}^{2}S_{1/2}\ensuremath{\rightarrow}3p\phantom{\rule{0.16em}{0ex}}^{2}P_{1/2})$ at 589.8 nm. The technique is applied to samples containing $3\ifmmode\times\else\texttimes\fi{}{10}^{9}$ atoms, previously cooled to $350\phantom{\rule{0.28em}{0ex}}\ensuremath{\mu}\mathrm{K}$ in a magneto-optical trap, and it leads to temperatures as low as $9\phantom{\rule{0.28em}{0ex}}\ensuremath{\mu}\mathrm{K}$ and phase-space densities in the range of ${10}^{\ensuremath{-}4}$. The capture efficiency of the gray molasses is larger than 2/3, and we observe no density-dependent heating for densities up to ${10}^{11}\phantom{\rule{0.28em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}3}$.

arXiv:1512.07053•Physical Review A•Feb 18, 2016•45 citations
We have studied the behavior of cesium atoms cooled in six-beam "gray" optical molasses. Cooling occurs for a laser detuned to the blue side of the 6S126{S}_{\frac{1}{2}}6S21​​, F=3\ensuremath→6P32F=3\ensuremath{\rightarrow}6{P}_{\frac{3}{2}}F=3\ensuremath→6P23​​, F\ensuremath′=2{F}^{\ensuremath{'}}=2F\ensuremath′=2 transition, and a Sisyphus-type effect accumulates the atoms in states not coupled to the light. We measure a minimum temperature of 1.1\ifmmode\pm\else\textpm\fi{}0.1 \ensuremath{\mu}K at low atomic density. The typical cooling time is on the order of 1 ms. A linear dependence of the temperature versus atomic density is found with a slope of \ensuremath{\sim}0.6 \ensuremath{\mu}K/(1010{10}^{10}1010 atoms/cm3{\mathrm{cm}}^{3}cm3).
We report the observation of three-dimensional cooling of cesium atoms using a four-beam optical molasses tuned to the blue side of the Fg{\mathit{F}}_{\mathit{g}}Fg​=3\ensuremath{\rightarrow}Fe{\mathit{F}}_{\mathit{e}}Fe​=2 hyperfine component of the 6S1/2{\mathit{S}}_{1/2}S1/2​\ensuremath{\rightarrow}6P3/2{\mathit{P}}_{3/2}P3/2​ transition. The cooling mechanism is a Sisyphus effect involving atomic states that are nearly uncoupled from the light field. Starting from a magneto-optical trap at 70 \ensuremath{\mu}K, the cooling time was on the order of 1 ms with almost 100% capture efficiency and temperature smaller than 5 \ensuremath{\mu}K measured. We also present a probe transmission spectrum showing that almost all the atoms are found in the nearly dark states.
We present a simple and general optical cooling method based on 3D degenerate Raman sideband cooling with adiabatic release that goes significantly beyond the density and temperature limitations of optical molasses. In 10 ms we cool a sample of 3×108 cesium atoms to a temperature of 330 nK at a density of 1.1×1011 cm−3, which corresponds to a phase-space density nλdB3=1/500.We further propose to cool atoms or molecules inside an optical cavity that enhances the scattering of blue-detuned photons and show that the dissipative mechanism can be viewed as a cavity-induced generalized Doppler cooling. Since the cooling depends on the atom’s internal level structure only through the photon scattering rate, cavity Doppler cooling is applicable to particles that do not possess a closed optical transition, which may allow one to extend laser cooling to a greater class of atoms or molecules. Large samples are cooled at the same rate as single atoms if the effect of one atom on the cavity resonance frequency is small. We also show how to achieve 3D cooling with a single optical cavity.
We present new techniques in cooling 39 K atoms using laser light close to the D1 transition.First, a new compressed-MOT configuration is taking advantage of gray-molasses-type cooling induced by blue-detuned D1 light.It yields an optimized density of atoms.Then, we use pure D1 gray molasses to further cool the atoms to an ultra-low temperature of 6 μK.The resulting phase-space density is 2 × 10 -4 and will ease future experiments with ultracold potassium.As an example, we use it to directly load up to 3 × 10 7 atoms in a far detuned optical trap, a result that opens the way to the all-optical production of potassium degenerate gases.
We report on the realization of sub-Doppler laser cooling of sodium atoms in gray molasses using the D1{D}_{1}D1​ optical transition $(3s\phantom{\rule{0.16em}{0ex}}^{2}S_{1/2}\ensuremath{\rightarrow}3p\phantom{\rule{0.16em}{0ex}}^{2}P_{1/2})$ at 589.8 nm. The technique is applied to samples containing $3\ifmmode\times\else\texttimes\fi{}{10}^{9}$ atoms, previously cooled to $350\phantom{\rule{0.28em}{0ex}}\ensuremath{\mu}\mathrm{K}$ in a magneto-optical trap, and it leads to temperatures as low as $9\phantom{\rule{0.28em}{0ex}}\ensuremath{\mu}\mathrm{K}$ and phase-space densities in the range of ${10}^{\ensuremath{-}4}$. The capture efficiency of the gray molasses is larger than 2/3, and we observe no density-dependent heating for densities up to ${10}^{11}\phantom{\rule{0.28em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}3}$.