Flattening a trapped atomic gas using a programmable optical potential in a feedback loop

We present a method for producing a flat, large-area Fermi gas of $^{6}\mathrm{Li}$ with a uniform area density. The method uses a programmable optical potential within a feedback loop to flatten the in-plane trapping potential for atoms. The optical potential is generated using a laser beam, whose intensity profile is adjusted by a spatial light modulator and optimized through measurements of the density distribution of the sample. The resulting planar sample exhibits a uniform area density within a region of about 480 $\textmu{}\mathrm{m}$ in diameter, and the standard deviation of the trap bottom potential is estimated to be $\ensuremath{\approx}{k}_{B}\ifmmode\times\else\texttimes\fi{}6.1$ nK, which is less than 20% of the transverse confinement energy. We discuss a dimensional crossover toward the two-dimensional regime by reducing the number of atoms in the planar trap, including the effect of the spatial variation of the transverse trapping frequency in the large-area sample.

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Publication Details

Journal
Physical review. A/Physical review, A
Published
2024-09-23
DOI
https://doi.org/10.1103/physreva.110.033326
Primary Topic
Cold Atom Physics and Bose-Einstein Condensates
Type
article
Field-Weighted Citation Impact
0.00

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article

Flattening a trapped atomic gas using a programmable optical potential in a feedback loop

Kyu‐Hwan Lee, J. C. Kim, S. H. Kim, Yong-il Shin
Physical review. A/Physical review, A
Cold Atom Physics and Bose-Einstein Condensates
article

Flattening a trapped atomic gas using a programmable optical potential in a feedback loop

Kyu‐Hwan Lee, J. C. Kim, S. H. Kim, Yong-il Shin
article en

Abstract

We present a method for producing a flat, large-area Fermi gas of $^{6}\mathrm{Li}$ with a uniform area density. The method uses a programmable optical potential within a feedback loop to flatten the in-plane trapping potential for atoms. The optical potential is generated using a laser beam, whose intensity profile is adjusted by a spatial light modulator and optimized through measurements of the density distribution of the sample. The resulting planar sample exhibits a uniform area density within a region of about 480 $\textmu{}\mathrm{m}$ in diameter, and the standard deviation of the trap bottom potential is estimated to be $\ensuremath{\approx}{k}_{B}\ifmmode\times\else\texttimes\fi{}6.1$ nK, which is less than 20% of the transverse confinement energy. We discuss a dimensional crossover toward the two-dimensional regime by reducing the number of atoms in the planar trap, including the effect of the spatial variation of the transverse trapping frequency in the large-area sample.

Physical review. A/Physical review, AVol. 110(3)
Seoul National University (KR)
National Research Foundation of Korea
Openalex Percentile: Top 86%
Cold Atom Physics and Bose-Einstein Condensates
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Flattening a trapped atomic gas using a programmable optical potential in a feedback loop — Kyu‐Hwan Lee, J. C. Kim, et al. · Physical review. A/Physical review, A (2024) | TGRS Research Map | TGRS