Fano resonance through Higgs bound states in tunneling of Nambu-Goldstone modes
arXiv:1503.01516 · doi:10.1103/PhysRevA.92.043610
Abstract
We study collective modes of superfluid Bose gases in optical lattices combined with potential barriers. We assume that the system is in the vicinity of the quantum phase transition to a Mott insulator at a commensurate filling, where emergent particle-hole symmetry gives rise to two types of collective mode, namely a gapless Nambu-Goldstone (NG) phase mode and a gapful Higgs amplitude mode. We consider two kinds of potential barrier: One does not break the particle-hole symmetry while the other does. In the presence of the former barrier, we find Higgs bound states that have binding energies lower than the bulk Higgs gap and are localized around the barrier. We analyze tunneling properties of the NG mode incident to both barriers to show that the latter barrier couples the Higgs bound states with the NG mode, leading to Fano resonance mediated by the bound states. Thanks to the universality of the underlying field theory, it is expected that Higgs bound states may be present also in other condensed matter systems with a particle-hole symmetry and spontaneous breaking of a continuous symmetry, such as quantum dimer antiferromagnets, superconductors, and charge-density-wave materials.
21 pages, 15 figures
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- Response of the Higgs amplitude mode of superfluid Bose gases in a three dimensional optical lattice
- Two-dimensional Schrödinger symmetry and three-dimensional breathers and Kelvin-ripple complexes as quasi-massive-Nambu-Goldstone modes
- Stability of supercurrents in a superfluid phase of spin-1 bosons in an optical lattice
- Perfect transmission of Higgs modes via antibound states
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- Hybridization of the amplitude mode in a confined fermionic superfluid
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