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Cover:The figure on the cover depicts a time sequence of images showing one cycle of the ringing of a Bose-Einstein condensate (BEC) in the JILA TOP (time-averaged orbiting potential) trap after being driven by strong oscillations of trap potential. The top left image shows the earliest time, with time increasing from left to right. To create each image, a BEC was formed and then strongly driven and finally allowed to expand ballistically, after which a picture was taken. BEC excitations have recently been observed in both the JILA [D. S. Jin et al., Phys. Rev. Lett. 77, 420 (1996)] and MIT [M.-O. Mewes et al., Phys. Rev. Lett. 77, 988 (1996)] traps. The ringing frequencies of a BEC for weak driving agree well with zero-temperature mean-field theory. Cover photographs courtesy Eric Cornell, JILA, Boulder, CO 80309.
Bose-Einstein Condensation
PrefaceAmong the most remarkable effects that quantum mechanics adds to the catalog of the thermal properties of matter is the "condensation" of an ideal gas of identical particles into a single quantum state, the principle of which was discovered in the theory of statistical mechanics by Bose and Einstein in the 1920s.Bose-Einstein condensation (BEC) is thus a mechanism for producing a macroscopic quantum system, and is exemplary of the macroscopic quantum phenomena of superconductivity and superfluidity. However, it has proven most difficult to attain BEC in the laboratory vs in the theory of the ideal gas. As discussed in the first article of this Special Issue, the basic criterion for BEC is that the typical distance between particles be comparable to or less than their deBroglie wavelengths; and in virtually every real material system, the effects of...