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Normal Phase of Polarised Strongly Interacting Fermi Gases

  • Alessio RecatiEmail author
  • Sandro Stringari
Chapter
Part of the Lecture Notes in Physics book series (LNP, volume 836)

Abstract

The theory of the normal phase of strongly interacting polarized atomic Fermi gases at zero temperature is reviewed. We use the formalism of quasi-particles to build up the equation of state of the normal phase with the relevant parameters calculated via Monte-Carlo. The theory is used to discuss the phase diagram of polarized Fermi gases at unitarity. The Fermi liquid nature of these configurations is pointed out. The theory provides accurate predictions for many different quantities experimentally measured, like the Chandrasekhar–Clogston limit of critical polarization, the density profiles and the Radio-Frequency spectrum.

Keywords

Normal Phase Single Impurity Momentum Relaxation Time Minority Component Collisionless Regime 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

Notes

Acknowledgments

We are indebted to F. Chevy, S. Giorgini, C. Pethick, L. P. Pitaevskii, C. Salomon, W. Zwerger and M. Zwierlein for very useful discussions. We acknowledge support by EuroQUAM Fermix program and by MIUR PRIN 2007.

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Copyright information

© Springer-Verlag Berlin Heidelberg 2012

Authors and Affiliations

  1. 1.Dipartimento di FisicaUniversità di Trento and CNR-INO BEC CenterTrentoItaly

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