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Topological Phase Transition and Z_{2} Index for S=1 Quantum Spin Chains
1Department of Physics, Gakushuin University, Mejiro, Toshima-ku, Tokyo 171-8588, Japan.
Physical Review Letters
|October 20, 2018
Summary
Researchers rigorously proved the existence of a topological phase transition in S=1 quantum spin systems. This transition, between the Affleck-Kennedy-Lieb-Tasaki (AKLT) model and trivial models, is a symmetry-protected topological phase.
Area of Science:
- Condensed Matter Physics
- Quantum Mechanics
- Statistical Mechanics
Background:
- S=1 quantum spin systems are crucial for understanding exotic phases of matter.
- Short-ranged Hamiltonians with specific symmetries are key to exploring novel quantum phenomena.
- The Affleck-Kennedy-Lieb-Tasaki (AKLT) model serves as a foundational example in topological quantum matter.
Purpose of the Study:
- To rigorously prove the existence of a topological phase transition in S=1 quantum spin systems.
- To establish that the AKLT model resides in a nontrivial symmetry-protected topological phase.
- To introduce a Z2 index for characterizing gapped unique ground states.
Main Methods:
- Definition of a Z2 index for gapped unique ground states.
- Proof of the Z2 index's invariance under smooth deformation.
- Utilizing the Z2 index to demonstrate a topological phase transition.
Main Results:
- A rigorous proof for a topological phase transition between the AKLT model and trivial models.
- Demonstration that this transition is undetectable by conventional order parameters.
- Establishment of the AKLT model as a nontrivial symmetry-protected topological phase.
Conclusions:
- The Z2 index provides a robust tool for identifying and characterizing topological phases.
- Symmetry-protected topological phases represent a distinct and important class of quantum matter.
- This work rigorously confirms the topological nature of the AKLT model, advancing the field of quantum information and condensed matter theory.
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