本實驗致力於實現高效雙腔體架構之銣原子玻色愛因斯坦凝聚。本實驗以腔體間的差動幫浦維持兩真空腔體間大於1000倍之壓力差,其中科學真空腔的真空度為1.3 × 10^−11 mbar,銣原子源側的真空腔真空度為5×10^8 mbar。經分析與優化,超高真空腔之磁光阱(Magneto-optical trap)的原子捕捉率約1 × 10^8 1/s,經灰色糖蜜冷卻(Gray molasses cooling),我們在三維磁光阱內捕捉到約1×10^9 顆原子,並降溫至18 μK。目前已將2.9×10^6 顆原子載入光偶極阱(Optical dipoletrap),進行強迫蒸發冷卻後,相空間密度(Phase space density) 達到1.1×10^−4,阱內剩餘原子為4.6×10^4 顆原子。
The goal of this experiment is to realize efficient production of rubidium Bose-Einstein condensates. We built a dual-chamber ultra-high vacuum system with a pressure difference of more than three orders of magnitude, where 1.3 × 10^−11 mbar is achieved in the science chamber, while 5 × 10^−8 mbar is detected in the vapor chamber. We transferred laser-cooled atoms from the 2D+ magneto-optical trap (MOT) in the vapor chamber to the 3D MOT in the science chamber with a loading rate of 1×10^8 1/s. We further implemented the gray molasses cooling (GMC) and compared the performance of GMC with temporal dark MOT. The optimized atom number after GMC is 1×10^9 with a temperature of 18 μK. We loaded 2.9×10^6 atoms into an optical dipole trap (ODT), and performed the evaporative cooling. We achieved a final phase space density of 1.1×10^−4, with 4.6×10^4 atoms remained in the trap.