Hidden Single-Qubit Topological Phase Transition without Gap Closing in Anisotropic Light-Matter Interactions

Conventionally the occurrence of topological phase transitions (TPTs) requires gap closing, whereas there are also unconventional cases without need of gap closing. Although traditionally TPTs lie in many-body systems in condensed matter, both cases of TPTs may find analogs in few-body systems. Inde...

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Bibliographic Details
Main Author: Ying, Z.-J (Author)
Format: Article
Language:English
Published: John Wiley and Sons Inc 2022
Subjects:
Online Access:View Fulltext in Publisher
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020 |a 25119044 (ISSN) 
245 1 0 |a Hidden Single-Qubit Topological Phase Transition without Gap Closing in Anisotropic Light-Matter Interactions 
260 0 |b John Wiley and Sons Inc  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1002/qute.202100165 
520 3 |a Conventionally the occurrence of topological phase transitions (TPTs) requires gap closing, whereas there are also unconventional cases without need of gap closing. Although traditionally TPTs lie in many-body systems in condensed matter, both cases of TPTs may find analogs in few-body systems. Indeed, the ground-state node number provides a topological classification for single-qubit systems. While the no-node theorem of spinless systems is shown to restrict the fundamental quantum Rabi model in light-matter interactions, it is demonstrated that the limitation of the no-node theorem can be broken not only in small counter-rotating terms (CRTs) but also in the large-CRT regime, which striates a rich phase diagram with different TPTs. While these transitions are mostly accompanied with gap closing and parity reversal, a hidden node-phase transition is revealed that has neither gap closing nor parity change, which turns out to be an analog of the unconventional TPT in condensed matter. A hysteresis sign for the unconventional TPT is unveiled via the transition from phase squeezing to amplitude squeezing in the gapped phase. The imprints in the Wigner function are also addressed. The clarified mechanisms provide some special insights for the subtle role of the CRTs. © 2022 Wiley-VCH GmbH. 
650 0 4 |a anisotropic quantum Rabi model 
650 0 4 |a Anisotropic quantum rabi model 
650 0 4 |a Anisotropy 
650 0 4 |a Counter rotating 
650 0 4 |a few-body quantum phase transition 
650 0 4 |a Few-body quantum phase transition 
650 0 4 |a Gap closing 
650 0 4 |a Ground state 
650 0 4 |a light-matter interaction 
650 0 4 |a Light-matter interactions 
650 0 4 |a Phase diagrams 
650 0 4 |a Phase transitions 
650 0 4 |a Quantum optics 
650 0 4 |a Quantum-phase transition 
650 0 4 |a Qubits 
650 0 4 |a Strong-coupling 
650 0 4 |a Topological phase 
650 0 4 |a topological phase transition without gap closing 
650 0 4 |a Topological phase transition without gap closing 
650 0 4 |a Topology 
650 0 4 |a ultra-strong coupling 
650 0 4 |a Ultra-strong coupling 
700 1 0 |a Ying, Z.-J.  |e author 
773 |t Advanced Quantum Technologies