Collective modes of a soliton train in a Fermi superfluid
arXiv:1612.04845 · doi:10.1103/PhysRevLett.118.260402
Abstract
We characterize the collective modes of a soliton train in a quasi-one-dimensional Fermi superfluid, using a mean-field formalism. In addition to the expected Goldstone and Higgs modes, we find novel long-lived gapped modes associated with oscillations of the soliton cores. The soliton train has an instability that depends strongly on the interaction strength and the spacing of solitons. It can be stabilized by filling each soliton with an unpaired fermion, thus forming a commensurate Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) phase. We find that such a state is always dynamically stable, which paves the way for realizing long-lived FFLO states in experiments via phase imprinting.
Published version: 4-page article + references + supplement. Supplement contains two new sections on (i) protocol to engineer soliton train states and (ii) convention for Bogoliubov operators. Results and conclusions unchanged
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Cited by in corpus (7)
- Suppressed solitonic cascade in spin-imbalanced superfluid Fermi gas
- Ring solitons and soliton sacks in imbalanced fermionic systems
- Snake instability of dark solitons across the BEC-BCS crossover: an effective field theory perspective
- Density-Matrix Renormalization Group for Continuous Quantum Systems
- Protocol to engineer Fulde-Ferrell-Larkin-Ovchinnikov states in a cold Fermi gas
- Collective modes in Fulde-Ferrell-Larkin-Ovchinnikov superconductors: The role of long-range Coulomb interaction and signatures in density response
- Detecting Topological Phase Transition in Superconductor-Semiconductor Hybrids by Electronic Raman Spectroscopy