Casimir–Polder interaction between an atom and a Chern insulator: topological signature and long-range repulsion

We consider the Casimir–Polder interaction between a two-level atomic system and a Chern insulator for both the resonant and nonresonant channels. For a right circularly polarized excited atomic state near a Chern insulator with a negative Chern number C, the resonant Casimir–Polder force can be monotonically repulsive over a large range of separations. In the presence of the same Chern insulator, a right circularly polarized metastable atomic state is expected to experience a repulsive nonresonant Casimir–Polder force over a certain range of atom-surface separations in the far-field region. At still greater separations, the nonresonant Casimir–Polder force is expected to become attractive and exhibit a topological signature, being proportional to [Formula: see text], where [Formula: see text] is the fine-structure constant.

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Publication Details

Journal
International Journal of Modern Physics A
Published
2024-12-31
DOI
https://doi.org/10.1142/s0217751x25430110
Citations
2
Primary Topic
Quantum Electrodynamics and Casimir Effect
Type
article
Field-Weighted Citation Impact
0.68
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article

Casimir–Polder interaction between an atom and a Chern insulator: topological signature and long-range repulsion

Bing-Sui Lu
2 citations
International Journal of Modern Physics A
Quantum Electrodynamics and Casimir Effect
0.68
article

Casimir–Polder interaction between an atom and a Chern insulator: topological signature and long-range repulsion

Bing-Sui Lu
article en
2 citations

Abstract

We consider the Casimir–Polder interaction between a two-level atomic system and a Chern insulator for both the resonant and nonresonant channels. For a right circularly polarized excited atomic state near a Chern insulator with a negative Chern number C, the resonant Casimir–Polder force can be monotonically repulsive over a large range of separations. In the presence of the same Chern insulator, a right circularly polarized metastable atomic state is expected to experience a repulsive nonresonant Casimir–Polder force over a certain range of atom-surface separations in the far-field region. At still greater separations, the nonresonant Casimir–Polder force is expected to become attractive and exhibit a topological signature, being proportional to [Formula: see text], where [Formula: see text] is the fine-structure constant.

International Journal of Modern Physics AVol. 40(10n11)
Thammasat University (TH)
Openalex Percentile: Top 29%
Quantum Electrodynamics and Casimir Effect
0.68
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