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Exactly Solvable Model for a Deconfined Quantum Critical Point in 1D
Carolyn Zhang1, Michael Levin1
1Department of Physics, Kadanoff Center for Theoretical Physics, University of Chicago, Chicago, Illinois 60637, USA.
We developed an exactly solvable model for a deconfined quantum critical point (DQCP) in 1+1 dimensions. This model reveals DQCPs are linked to Z4 symmetry breaking critical points at the edge of a 2+1 dimensional topological phase.
Area of Science:
- Condensed Matter Physics
- Quantum Field Theory
- Topological Phases of Matter
Background:
- Deconfined quantum critical points (DQCPs) represent exotic transitions between distinct quantum phases.
- Symmetry Protected Topological (SPT) phases offer unique boundary phenomena.
- Understanding DQCPs in lower dimensions is crucial for theoretical advancements.
Purpose of the Study:
- To construct an exactly solvable lattice model for a DQCP in (1+1) dimensions.
- To investigate the unusual setting of a DQCP at the edge of a (2+1) dimensional bosonic SPT phase.
- To establish a connection between DQCPs and Z4 symmetry breaking critical points.
Main Methods:
- Construction of an exactly solvable lattice model.
- Utilizing an exact mapping between the SPT edge theory and a Z4 spin chain.
- Analysis of phase transitions in (1+1) and (2+1) dimensional systems.
Main Results:
- An exactly solvable lattice model for a DQCP in (1+1) dimensions is successfully constructed.
- The DQCP is found to occur at the edge of a (2+1) dimensional bosonic SPT phase with Z2×Z2 symmetry.
- The study reveals a direct relationship between these DQCPs and ordinary Z4 symmetry breaking critical points.
Conclusions:
- The developed model provides a tractable framework for studying DQCPs in novel contexts.
- The findings highlight the intricate relationship between topological phases and quantum criticality.
- This work bridges the understanding of DQCPs and conventional symmetry breaking phenomena.
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