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

arXiv:1811.02185 · SciPost Physics

Sub-Doppler laser cooling of $^{39}$K via the 4S$\to$5P transition

Govind Unnikrishnan, Michael Gröbner, Hanns‐Christoph Nägerl

Published Apr 18, 2019• 6 citations
arXivHTMLPDF

Abstract

We demonstrate sub-Doppler laser cooling of ^{39} 39 K using degenerate Raman sideband cooling via the 4S _{1/2} \rightarrow 1 / 2 → 5P _{1/2} 1 / 2 transition at 404.8 nm. By using an optical lattice in combination with a magnetic field and optical pumping beams, we obtain a spin-polarized sample of up to 5.6 \times 10^{7} 5.6 × 10 7 atoms cooled down to a sub-Doppler temperature of 4 \upmu μ K, reaching a peak density of 3.9 \times 10^{9} 3.9 × 10 9 atoms/cm ^{3} 3 , a phase-space density greater than 10^{-5} 10 − 5 , and an average vibrational level of \langle \nu \rangle=0.6 ⟨ ν ⟩ = 0.6 in the lattice. This work opens up the possibility of implementing a single-site imaging scheme in a far-detuned optical lattice utilizing shorter wavelength transitions in alkali atoms, thus allowing improved spatial resolution.

DOI
10.21468/scipostphys.6.4.047

Related papers

Degenerate Raman sideband cooling of K39

Michael Gröbner, Philipp Weinmann, Emil Kirilov +1 more

We report on a realization of sub-Doppler laser cooling of $^{39}\mathrm{K}$ atoms using degenerate three-dimensional Raman sideband cooling. We take advantage of the well-resolved excited hyperfine states on the ${D}_{1}$ optical transition to produce spin-polarized samples with $1.4\ifmmode\times\else\texttimes\fi{}{10}^{8}$ atoms at temperatures of 1.8 $\ensuremath{\mu}\mathrm{K}$. The phase-space densities are $\ensuremath{\ge}{10}^{\ensuremath{-}4}$, which significantly improves the initial conditions for a subsequent evaporative cooling step. The presented cooling technique using the ${D}_{1}$ line can be adapted to other atomic species and is applicable to high-resolution imaging schemes in far off-resonant optical lattices.

arXiv:1612.02309•Physical Review A•Mar 15, 2017•24 citations

Degenerate Raman sideband cooling of K40 atoms

Elad Zohar, Yanay Florshaim, Oded Zilberman +2 more

We report on the implementation of degenerate Raman sideband cooling of $^{40}\mathrm{K}$ atoms. The scheme incorporates a three-dimensional (3D) optical lattice, which confines the atoms and drives the Raman transitions. The optical cooling cycle is closed by two optical pumping beams. The wavelength of the laser beams forming the lattice is close to the ${\mathrm{D}}_{2}$ atomic transition, while the optical pumping is operated near the ${\mathrm{D}}_{1}$ transition. With this cooling method, we achieve a temperature of $\ensuremath{\sim}1\phantom{\rule{0.16em}{0ex}}\ensuremath{\mu}\mathrm{K}$ of a cloud with $\ensuremath{\sim}{10}^{7}$ atoms. This corresponds to a phase space density of $\ensuremath{\ge}{10}^{\ensuremath{-}3}$. Moreover, the fermionic ensemble is spin polarized to conditions which are favorable for subsequent evaporative cooling. We study the dependence of the cooling scheme on several parameters, including the applied magnetic field and the detuning, duration, and intensity profile of the optical pumping beams. Adding this optical cooling stage to current Fermi gas experiments can improve the final conditions and increase the data rate.

arXiv:2208.05160•Physical Review A•Dec 23, 2022•8 citations

Two-dimensional sideband Raman cooling and m=0 Zeeman state preparation in an optical lattice

А. В. Тайченачев, Anatolii M Tumaikin, Valeriy I. Yudin +1 more

Summary form only given. Laser cooled atoms play a critical role in modern designs of frequency standards such as atomic fountains. Recently, an elegant and efficient method of two-dimensional cooling to the vibrational ground state of a far-off resonance optical lattice has been demonstrated. This method is a variant of Raman sideband cooling based on the Raman transitions between the vibrational manifolds of adjacent Zeeman substates. A static magnetic field is used to tune the Zeeman levels so that Raman resonance occurs on the red sideband and results in cooling. Two circularly polarized fields are used to recycle the atoms for repetitive Raman cooling. Unfortunately, a direct application of this scheme to frequency standards meets with several difficulties. Stimulated by these concepts and results, we propose a new variant of transverse sideband cooling, where these problems are avoided, while still maintaining most of the attractive features. The field configuration used for the optical lattice consists of three linearly polarized beams having equal amplitudes and propagating in the xy plane with angles of 2/spl pi//3 between each other. The polarization vectors of these beams are tilted through a small angle with respect to the z-axis. All the beams have the same frequency far-detuned to the red of the D/sub 2/ resonance line. Raman transitions between vibrational levels of adjacent magnetic substates are induced by the small in-plane component of the field. Two other important requirements for Raman sideband cooling are a uniform energy shift of the magnetic sublevels and optical pumping.

Quantum Electronics and Laser Science Conference•May 12, 2000•0 citations

Raman sideband cooling of rubidium atoms in optical lattice

Chunhua Wei, Shuhua Yan

We develop a simple and practical scheme to apply sideband cooling to a cloud of rubidium atoms. A sample containing 4 × 10 70 87 Rb is trapped in a far red detuned optical lattice. Through optimizing the relevant parameters, i.e., laser detuning, magnetic field, polarization, and duration time, a temperature around 1.5 μK and phase space density close to 1/500 are achieved. Compared with polarization gradient cooling, the temperature decreases by around one order of magnitude. This technique could be used in high precision measurement such as atomic clocks and atom interferometer. It could also serve as a precooling means before evaporation cooling in a dipole trap, and may be a promising method of achieving quantum degeneracy with purely optical means.

Chinese Physics B•Aug 1, 2017•2 citations

3D Raman Sideband Cooling of Cesium Atoms at High Density

Dian-Jiun Han, Steffen Wolf, Steven J. Oliver +3 more

We laser cool $5\ifmmode\times\else\texttimes\fi{}{10}^{7}$ Cs atoms to a spin-polarized phase space density of 1/30, the highest ever obtained by laser cooling. It is achieved by compression and polarization gradient cooling in a 3D far-off-resonant optical lattice, followed by 3D Raman sideband cooling optimized at a density of $1.5\ifmmode\times\else\texttimes\fi{}{10}^{12}\mathrm{atoms}/{\mathrm{cm}}^{3}$, and adiabatic release. In the lattice, $23%$ of the sites are occupied, $95%$ of the atoms are in the lowest energy magnetic sublevel, and $37%$ are in the lowest 3D vibrational state.

Physical Review Letters•Jul 24, 2000•108 citations

Sub-Doppler laser cooling of potassium atoms

Manuele Landini, Sanjukta Roy, L. Carcagní +4 more

We investigate the sub-Doppler laser cooling of bosonic potassium isotopes, whose small hyperfine splitting has so far prevented cooling below the Doppler temperature. We find instead that the combination of a dark optical molasses scheme that naturally arises in this kind of system and an adiabatic ramping of the laser parameters allows us to reach sub-Doppler temperatures for small laser detunings. We demonstrate temperatures as low as $25\ifmmode\pm\else\textpm\fi{}3$ $\ensuremath{\mu}$K and $47\ifmmode\pm\else\textpm\fi{}5$ $\ensuremath{\mu}$K in high-density samples of the two isotopes ${}^{39}$K and ${}^{41}$K, respectively. Our findings should find application to other atomic systems.

arXiv:1107.2337•Physical Review A•Oct 28, 2011•77 citations
Sub-Doppler laser cooling of 39^{39}39K via the 4S$\to$5P transition
We demonstrate sub-Doppler laser cooling of ^{39} 39 K using degenerate Raman sideband cooling via the 4S _{1/2} \rightarrow 1 / 2 → 5P _{1/2} 1 / 2 transition at 404.8 nm. By using an optical lattice in combination with a magnetic field and optical pumping beams, we obtain a spin-polarized sample of up to 5.6 \times 10^{7} 5.6 × 10 7 atoms cooled down to a sub-Doppler temperature of 4 \upmu μ K, reaching a peak density of 3.9 \times 10^{9} 3.9 × 10 9 atoms/cm ^{3} 3 , a phase-space density greater than 10^{-5} 10 − 5 , and an average vibrational level of \langle \nu \rangle=0.6 ⟨ ν ⟩ = 0.6 in the lattice. This work opens up the possibility of implementing a single-site imaging scheme in a far-detuned optical lattice utilizing shorter wavelength transitions in alkali atoms, thus allowing improved spatial resolution.
We report on a realization of sub-Doppler laser cooling of 39K^{39}\mathrm{K}39K atoms using degenerate three-dimensional Raman sideband cooling. We take advantage of the well-resolved excited hyperfine states on the D1{D}_{1}D1​ optical transition to produce spin-polarized samples with $1.4\ifmmode\times\else\texttimes\fi{}{10}^{8}$ atoms at temperatures of 1.8 $\ensuremath{\mu}\mathrm{K}$. The phase-space densities are $\ensuremath{\ge}{10}^{\ensuremath{-}4}$, which significantly improves the initial conditions for a subsequent evaporative cooling step. The presented cooling technique using the D1{D}_{1}D1​ line can be adapted to other atomic species and is applicable to high-resolution imaging schemes in far off-resonant optical lattices.
We report on the implementation of degenerate Raman sideband cooling of 40K^{40}\mathrm{K}40K atoms. The scheme incorporates a three-dimensional (3D) optical lattice, which confines the atoms and drives the Raman transitions. The optical cooling cycle is closed by two optical pumping beams. The wavelength of the laser beams forming the lattice is close to the D2{\mathrm{D}}_{2}D2​ atomic transition, while the optical pumping is operated near the D1{\mathrm{D}}_{1}D1​ transition. With this cooling method, we achieve a temperature of $\ensuremath{\sim}1\phantom{\rule{0.16em}{0ex}}\ensuremath{\mu}\mathrm{K}$ of a cloud with $\ensuremath{\sim}{10}^{7}$ atoms. This corresponds to a phase space density of $\ensuremath{\ge}{10}^{\ensuremath{-}3}$. Moreover, the fermionic ensemble is spin polarized to conditions which are favorable for subsequent evaporative cooling. We study the dependence of the cooling scheme on several parameters, including the applied magnetic field and the detuning, duration, and intensity profile of the optical pumping beams. Adding this optical cooling stage to current Fermi gas experiments can improve the final conditions and increase the data rate.
Summary form only given. Laser cooled atoms play a critical role in modern designs of frequency standards such as atomic fountains. Recently, an elegant and efficient method of two-dimensional cooling to the vibrational ground state of a far-off resonance optical lattice has been demonstrated. This method is a variant of Raman sideband cooling based on the Raman transitions between the vibrational manifolds of adjacent Zeeman substates. A static magnetic field is used to tune the Zeeman levels so that Raman resonance occurs on the red sideband and results in cooling. Two circularly polarized fields are used to recycle the atoms for repetitive Raman cooling. Unfortunately, a direct application of this scheme to frequency standards meets with several difficulties. Stimulated by these concepts and results, we propose a new variant of transverse sideband cooling, where these problems are avoided, while still maintaining most of the attractive features. The field configuration used for the optical lattice consists of three linearly polarized beams having equal amplitudes and propagating in the xy plane with angles of 2/spl pi//3 between each other. The polarization vectors of these beams are tilted through a small angle with respect to the z-axis. All the beams have the same frequency far-detuned to the red of the D/sub 2/ resonance line. Raman transitions between vibrational levels of adjacent magnetic substates are induced by the small in-plane component of the field. Two other important requirements for Raman sideband cooling are a uniform energy shift of the magnetic sublevels and optical pumping.
We develop a simple and practical scheme to apply sideband cooling to a cloud of rubidium atoms. A sample containing 4 × 10 70 87 Rb is trapped in a far red detuned optical lattice. Through optimizing the relevant parameters, i.e., laser detuning, magnetic field, polarization, and duration time, a temperature around 1.5 μK and phase space density close to 1/500 are achieved. Compared with polarization gradient cooling, the temperature decreases by around one order of magnitude. This technique could be used in high precision measurement such as atomic clocks and atom interferometer. It could also serve as a precooling means before evaporation cooling in a dipole trap, and may be a promising method of achieving quantum degeneracy with purely optical means.
We laser cool $5\ifmmode\times\else\texttimes\fi{}{10}^{7}$ Cs atoms to a spin-polarized phase space density of 1/30, the highest ever obtained by laser cooling. It is achieved by compression and polarization gradient cooling in a 3D far-off-resonant optical lattice, followed by 3D Raman sideband cooling optimized at a density of $1.5\ifmmode\times\else\texttimes\fi{}{10}^{12}\mathrm{atoms}/{\mathrm{cm}}^{3}$, and adiabatic release. In the lattice, 2323%23 of the sites are occupied, 9595%95 of the atoms are in the lowest energy magnetic sublevel, and 3737%37 are in the lowest 3D vibrational state.
We investigate the sub-Doppler laser cooling of bosonic potassium isotopes, whose small hyperfine splitting has so far prevented cooling below the Doppler temperature. We find instead that the combination of a dark optical molasses scheme that naturally arises in this kind of system and an adiabatic ramping of the laser parameters allows us to reach sub-Doppler temperatures for small laser detunings. We demonstrate temperatures as low as $25\ifmmode\pm\else\textpm\fi{}3$ $\ensuremath{\mu}$K and $47\ifmmode\pm\else\textpm\fi{}5$ $\ensuremath{\mu}$K in high-density samples of the two isotopes 39{}^{39}39K and 41{}^{41}41K, respectively. Our findings should find application to other atomic systems.