id	author	title	date	pages	extension	mime	words	sentences	flesch	summary	cache	txt
work_77r7tcvd5jeknnxkzfu4vox3qq	Swati Singh	Progress towards ultra-cold ensembles of rubidium and lithium	2007.0	96	.pdf	application/pdf	31434	3693	74	all laser cooling experiments is an atomic source, the details of the requirements and 4.2 The calculated loading rate for trapped atoms in a lithium MOT as a The other very important reason why the idea of temperature adopted in laser cooling in scientifically inappropriate is due to the fact that the system (atoms + photons), although in its steady state, cannot be called in thermal equilibrium [59]. Figure 3.2: Schematic of rubidium energy level diagram with the laser cooling and repump light shown for both 87Rb and 85Rb. Refer to [28] for more accurate frequencies. Figure 4.2: The calculated loading rate for trapped atoms in a lithium MOT as a Figure 4.4: The calculated steady state number for trapped atoms in a lithium MOT Figure 4.4: The calculated steady state number for trapped atoms in a lithium MOT Figure 4.4: The calculated steady state number for trapped atoms in a lithium MOT	./cache/work_77r7tcvd5jeknnxkzfu4vox3qq.pdf	./txt/work_77r7tcvd5jeknnxkzfu4vox3qq.txt