Erratum: Landau Phonon-Roton Theory Revisited for Superfluid ^{4}He and Fermi Gases [Phys. Rev. Lett. 119, 260402 (2017)].

This corrects the article DOI: 10.1103/PhysRevLett.119.

Pair-Breaking Collective Branch in BCS Superconductors and Superfluid Fermi Gases.

We demonstrate the existence of a collective excitation branch in the pair-breaking continuum of superfluid Fermi gases and BCS superconductors. At zero temperature, we analytically continue the equation on the collective mode energy in Anderson's Random Phase Approximation or Gaussian fluctuations through its branch cut associated with the continuum, and obtain the full complex dispersion relation, including in the strong coupling regime. The branch exists as long as the chemical potential μ is positive and the wave number below sqrt[2mμ]/ℏ (with m the fermion mass).

Landau Phonon-Roton Theory Revisited for Superfluid ^{4}He and Fermi Gases.

Liquid helium and spin-1/2 cold-atom Fermi gases both exhibit in their superfluid phase two distinct types of excitations, gapless phonons and gapped rotons or fermionic pair-breaking excitations. In the long wavelength limit, revising and extending the theory of Landau and Khalatnikov initially developed for helium [Zh. Exp.

Limit of spin squeezing in finite-temperature Bose-Einstein condensates.

We show that, at finite temperature, the maximum spin squeezing achievable using interactions in Bose-Einstein condensates has a finite limit when the atom number N→∞ at fixed density and interaction strength. We calculate the limit of the squeezing parameter for a spatially homogeneous system and show that it is bounded from above by the initial noncondensed fraction.