Phonon-mediated Casimir interaction between finite mass impurities
arXiv:1809.11071 · doi:10.1103/PhysRevB.98.161410
Abstract
The Casimir effect, a two-body interaction via vacuum fluctuations, is a fundamental property of quantum systems. In solid state physics it emerges as a long-range interaction between two impurity atoms via virtual phonons. In the classical limit for the impurity atoms in dimensions the interaction is known to follow the universal power-law . However, for finite masses of the impurity atoms on a lattice, it was predicted to be at large distances. We examine how one power-law can change into another with increase of the impurity mass and in presence of an external potential. We provide the exact solution for the system in one-dimension. At large distances indeed for finite impurity masses, while for the infinite impurity masses or in an external potential it crosses over to . At short distances the Casimir interaction is not universal and depends on the impurity mass and the external potential.
arXiv comment5+7 pages, 5+6 figures
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- Induced pairing of fermionic impurities in a one-dimensional strongly correlated Bose gas
- Field-theoretical approach to the Casimir-like interaction in a one-dimensional Bose gas
- Impurities in a one-dimensional Bose gas: the flow equation approach
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- Many-impurity phonon Casimir effect in atomic chains
- Phonon Casimir effect in polyatomic systems
- Effective approaches to the dynamical properties of two distinguishable Bose polarons