| This is a file in the archives of the Stanford Encyclopedia of Philosophy. |
Figure 6. Peak density at the center of the sample as a function of
the final depth of the evaporative cut on the RF frequency. As
evaporation progresses to smaller values of the frequency, the cloud
shrinks and cools, causing a modest increase in peak density until the
frequency reaches 4.23 MHz. The sudden discontinuity at 4.23 MHz
indicates the first appearance of the high-density condensate as the
cloud undergoes a phase transition. From Anderson et al. (1995).
| Allan Franklin allan.franklin@colorado.edu |