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RESEARCH PRODUCT

Symmetry-protected intermediate trivial phases in quantum spin chains

Augustine KshetrimayumRoman OrusHong-hao Tu

subject

Quantum phase transitionPhysicsQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)Time-evolving block decimationFOS: Physical sciences02 engineering and technologyQuantum entanglementQuantum phasesAstrophysics::Cosmology and Extragalactic Astrophysics021001 nanoscience & nanotechnology01 natural sciencesCondensed Matter - Strongly Correlated ElectronsQuantum mechanics0103 physical sciencesThermodynamic limitTopological order010306 general physics0210 nano-technologyCentral chargeQuantum Physics (quant-ph)Phase diagram

description

Symmetry-protected trivial (SPt) phases of matter are the product-state analogue of symmetry-protected topological (SPT) phases. This means, SPt phases can be adiabatically connected to a product state by some path that preserves the protecting symmetry. Moreover, SPt and SPT phases can be adiabatically connected to each other when interaction terms that break the symmetries protecting the SPT order are added in the Hamiltonian. It is also known that spin-1 SPT phases in quantum spin chains can emerge as effective intermediate phases of spin-2 Hamiltonians. In this paper we show that a similar scenario is also valid for SPt phases. More precisely, we show that for a given spin-2 quantum chain, effective intermediate spin-1 SPt phases emerge in some regions of the phase diagram, these also being adiabatically connected to non-trivial intermediate SPT phases. We characterize the phase diagram of our model by studying quantities such as the entanglement entropy, symmetry-related order parameters, and 1-site fidelities. Our numerical analysis uses Matrix Product States (MPS) and the infinite Time-Evolving Block Decimation (iTEBD) method to approximate ground states of the system in the thermodynamic limit. Moreover, we provide a field theory description of the possible quantum phase transitions between the SPt phases. Together with the numerical results, such a description shows that the transitions may be described by Conformal Field Theories (CFT) with central charge c=1. Our results are in agreement, and further generalize, those in [Y. Fuji, F. Pollmann, M. Oshikawa, Phys. Rev. Lett. 114, 177204 (2015)].

https://dx.doi.org/10.48550/arxiv.1511.06338