\begin{document}$\tau $\end{document}, three-dimensional magnetic field \begin{document}$ \left( {{B_x}, {B_y}, {B_z}} \right) $\end{document}, single-photon detuning \begin{document}$\varDelta $\end{document}, two-photon detuning \begin{document}$\delta $\end{document}, ratio of cooling beam power to repumping beam power \begin{document}${I_{{\text{cool}}}}/{I_{{\text{rep}}}}$\end{document}, and cooling beam power \begin{document}${I_{{\text{cooling}}}}$\end{document}. The optimal parameters in this system are follows: \begin{document}$ \tau = 7{\text{ ms}},\; \delta = 0.2{\text{ MHz}},\; \varDelta = 5\varGamma, \;{I_{{\text{cool}}}}/{I_{{\text{rep}}}} = 3, {\text{ and }} {I_{{\text{cool}}}} = 1.2{I_{{\text{sat}}}}. $\end{document} Comparing with traditional PGC-assisted loading, the number of atoms is increased about 4 times, and the atomic temperature decreases from \begin{document}$ 25{\text{ μK}} $\end{document} to \begin{document}$ 8{\text{ μK}} $\end{document}. This experiment provides important insights for preparing ultracold atomic samples and capturing single atom arrays."> - 必威体育下载

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Liu Yan-Xin, Wang Zhi-Hui, Guan Shi-Jun, Wang Qin-Xia, Zhang Peng-Fei, Li Gang, Zhang Tian-Cai
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  • Abstract views:1044
  • PDF Downloads:67
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  • Received Date:28 January 2024
  • Accepted Date:13 March 2024
  • Available Online:07 April 2024
  • Published Online:05 June 2024

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