Optimal preparation of Bose and Fermi atomic gas mixtures of ^(87)Rb and ^(40)K in a crossed optical dipole trap
作者机构:State Key Laboratory of Quantum Optics and Quantum Optics DevicesInstitute of Opto-electronicsCollaborative Innovation Center of Extreme OpticsShanxi UniversityTaiyuan 030006China Hefei National LaboratoryHefei 230000China
出 版 物:《Chinese Physics B》 (中国物理B(英文版))
年 卷 期:2024年第33卷第6期
页 面:356-361页
核心收录:
学科分类:07[理学] 070205[理学-凝聚态物理] 0702[理学-物理学]
基 金:supported by the Innovation Program for Quantum Science and Technology (Grant No. 2021ZD0302003) the National Natural Science Foundation of China (Grant Nos. 12034011, U23A6004, 12374245,12322409, 92065108, 11974224, and 12022406) the National Key Research and Development Program of China (Grant Nos. 2022YFA1404101 and 2021YFA1401700) the Fund for Shanxi 1331 Project Key Subjects Construction
主 题:optical dipole trap Bose and Fermi gas mixtures atomic lifetime
摘 要:We report on the optimal production of the Bose and Fermi mixtures with ^(87) Rb and ^(40)K in a crossed optical dipole trap(ODT).We measure the atomic number and lifetime of the mixtures in combination of the spin state |F=9/2,m_(F)=9/2 of^(40)K and |1,1of ^(87) Rb in the ODT,which is larger and longer compared with the combination of the spin state |9/2,9/2 of^(40)K and 12,2) of ^(87)Rb in the *** observe the atomic numbers of ^(87)Rb and ^(40)K shown in each stage of the sympathetic cooling process while gradually reducing the depth of the optical *** optimizing the relative loading time of atomic mixtures in the MOT,we obtain the large atomic number of ^(40)K(~6 ×10^(6)) or the mixtures of atoms with an equal number(~1.6 × 10^(6)) at the end of evaporative cooling in the *** experimentally investigate the evaporative cooling in an enlarged volume of the ODT via adding a third laser beam to the crossed ODT and found that more atoms(8 × 10^(6)) and higher degeneracy(T/T_(F)=0.25) of Fermi gases are *** ultracold atomic gas mixtures pave the way to explore phenomena such as few-body collisions and the Bose-Fermi Hubbard model,as well as for creating ground-state molecules of ^(87)Rb^(40)K.