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

ISBN-10: 9814667730

ISBN-13: 9789814667739

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 desire is this sequence will advertise examine via either highlighting contemporary breakthroughs and by way of outlining probably the most promising learn instructions within the field.

Readership: study scientists together with graduate scholars and top point undergraduate scholars.

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**Additional info for Annual Review of Cold Atoms and Molecules: Volume 3**

**Example text**

5ωz , and εb > ωz in the Bose limit. Here, n 2 = n ↑ = n ↓ is the planar density per spin. Therefore, the scattering length (denoted a2 ) is not always simply related to εb , and must be defined via the quasi-2D T matrix. The solid curve is obtained from a fit to the 2D QMC data 55 while the dashed line approximately corresponds to the weak-coupling result in the Fermi regime. (Reprinted figure with permission from: V. Makhalov, K. Martiyanov, and A. Turlapov, Phys. Rev. Lett. 112, 045301 (2014).

The occupied part of the spectral function at ln(k F a2D ) = 0. (left) Measured momentum-resolved photoemission signal, taken from Ref. 10. , k − εb . ) high-density region at the center of the trapped gas to the low-density region at the edge. Thus, we can in principle observe the entire FermiBose crossover in a single experiment. This argument relies on the local density approximation (LDA), where the in-plane trapping potential can be incorporated into the chemical potential, µ(r) = µ − V (r), and thus each point in the trap corresponds to a different ln (k F (r)a2D ).

The point µ = 0 may be regarded as the “crossover point” that approximately separates Fermi and Bose regimes, as we discuss in Sec. 5. 17 As shown in Fig 12, the comparison with the QMC prediction is reasonable, aside from the BCS side of the crossover (or Fermi regime), where the pressure is significantly higher. Indeed, this is in the limit where the weak-coupling result becomes March 4, 2015 6:20 Annual Review of Cold Atoms and Molecules Volume 3 36 9in x 6in b2033-ch01 page 36 J. Levinsen & M.

### Annual Review of Cold Atoms and Molecules: Volume 3 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

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