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Published on: November 11, 2013
Quantum reservoir probing of quantum phase transitions
Kaito Kobayashi1, Yukitoshi Motome2
1Department of Applied Physics, University of Tokyo, Tokyo, Japan. kaito-kobayashi92@g.ecc.u-tokyo.ac.jp.
Local quantum quenches can now detect quantum phase transitions. Quantum reservoir probing (QRP) extracts localized excitations, revealing phase boundaries even in complex quantum spin systems.
Area of Science:
- Quantum Many-Body Physics
- Condensed Matter Physics
Background:
- Quantum phase transitions (QPTs) are critical phenomena in quantum many-body systems.
- Identifying QPTs in equilibrium systems presents significant theoretical and experimental challenges.
- Existing dynamical detection protocols rely on global quantum quenches and global excitations.
Purpose of the Study:
- To introduce a novel method for detecting quantum phase transitions using local quantum quenches.
- To demonstrate the efficacy of quantum reservoir probing (QRP) in analyzing localized excitations.
- To show that this framework can precisely delineate phase boundaries near quantum critical points.
Main Methods:
- Implementing local quantum quenches to induce localized out-of-equilibrium excitations.
- Utilizing the quantum reservoir probing (QRP) framework to isolate the effects of local quenches.
- Analyzing single-site observables to detect changes in quantum phases.
Main Results:
- Local quantum quenches and QRP can effectively detect quantum phase transitions.
- The impact of local quenches varies across different quantum phases.
- Quantum fluctuations near critical points suppress local quench effects, aiding phase boundary delineation.
- This method successfully identified QPTs in integrable and non-integrable quantum spin systems, including topological QPTs.
Conclusions:
- Local quantum quenches combined with QRP offer a powerful and versatile tool for detecting quantum phase transitions.
- This approach overcomes limitations of global quench methods by focusing on localized dynamics.
- The framework is applicable to various quantum systems and transition types, including topological transitions.
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