By Kirk W Madison, Kai Bongs, Visit Amazon's Lincoln D Carr Page, search results, Learn about Author Central, Lincoln D Carr, , Ana Maria Rey, Hui Zhai
The purpose of this e-book is to include evaluate articles describing the newest theoretical and experimental advancements within the box of chilly atoms and molecules. Our wish is this sequence will advertise examine via either highlighting contemporary breakthroughs and by way of outlining probably the most promising study instructions within the field.
Readership: examine scientists together with graduate scholars and higher point undergraduate scholars.
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However, the mean-field result is not quantitatively accurate in the Fermi regime since it does not capture the leading order dependence on the interaction, as discussed in Sec. 3. The 2D contact may be experimentally determined from the highfrequency tail of the RF spectrum,80 as well as from the momentum profile. In contrast to the pressure, the contact appears to be surprisingly insensitive to temperature in the degenerate regime T < TF . 5. The 2D crossover “point” Finally, we turn to the crossover from Fermi to Bose behavior in the 1.
4. Equation of state in a trapped gas The fact that the interaction parameter ln(k F a2D ) can be tuned by varying the density has important consequences for the trapped 2D gas. Specifically, it implies that ln(k F a2D ) decreases as we move from the March 4, 2015 6:20 Annual Review of Cold Atoms and Molecules Volume 3 b2033-ch01 page 46 J. Levinsen & M. M. 5 Fig. 18. The occupied part of the spectral function at ln(k F a2D ) = 0. (left) Measured momentum-resolved photoemission signal, taken from Ref.
119. 1. Variational approach An intuitive way to describe the Fermi polaron theoretically is through variational wavefunctions.