TY - JOUR
T1 - Stable Measurement-Induced Floquet Enriched Topological Order
AU - Vu, Dinhduy
AU - Lavasani, Ali
AU - Lee, Jong Yeon
AU - Fisher, Matthew P.A.
N1 - This research was supported in part by the National Science Foundation under Grant No. NSF PHY-1748958, the Heising-Simons Foundation and the Simons Foundation (216179, LB). The authors acknowledge the University of Maryland supercomputing resources made available for conducting the research reported in this Letter. D. V. is supported by the Laboratory for Physical Science. J. Y. L. is supported by the Gordon and Betty Moore Foundation under the Grant No. GBMF8690 and by the National Science Foundation under the Grant No. PHY-1748958. M. P. A. F. is supported by the Heising-Simons Foundation and the Simons Collaboration on Ultra-Quantum Matter, which is a grant from the Simons Foundation (651457).
PY - 2024/2/16
Y1 - 2024/2/16
N2 - The Floquet code utilizes a periodic sequence of two-qubit measurements to realize the topological order. After each measurement round, the instantaneous stabilizer group can be mapped to a honeycomb toric code, explaining the topological feature. The code also possesses a time-crystal order - the e-m transmutation after every cycle, breaking the Floquet symmetry of the measurement schedule. This behavior is distinct from the stationary topological order realized in either random circuits or time-independent Hamiltonian. Therefore, the resultant phase belongs to the overlap between the classes of Floquet enriched topological orders and measurement-induced phases. In this Letter, we construct a continuous path interpolating between the Floquet and toric codes, focusing on the transition between the time-crystal and stationary topological phases. We show that this transition is characterized by a divergent length scale. We also add single-qubit perturbations to the model and obtain a richer two-dimensional parametric phase diagram of the Floquet code, showing the stability of the Floquet enriched topological order.
AB - The Floquet code utilizes a periodic sequence of two-qubit measurements to realize the topological order. After each measurement round, the instantaneous stabilizer group can be mapped to a honeycomb toric code, explaining the topological feature. The code also possesses a time-crystal order - the e-m transmutation after every cycle, breaking the Floquet symmetry of the measurement schedule. This behavior is distinct from the stationary topological order realized in either random circuits or time-independent Hamiltonian. Therefore, the resultant phase belongs to the overlap between the classes of Floquet enriched topological orders and measurement-induced phases. In this Letter, we construct a continuous path interpolating between the Floquet and toric codes, focusing on the transition between the time-crystal and stationary topological phases. We show that this transition is characterized by a divergent length scale. We also add single-qubit perturbations to the model and obtain a richer two-dimensional parametric phase diagram of the Floquet code, showing the stability of the Floquet enriched topological order.
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U2 - 10.1103/PhysRevLett.132.070401
DO - 10.1103/PhysRevLett.132.070401
M3 - Article
C2 - 38427862
AN - SCOPUS:85185410407
SN - 0031-9007
VL - 132
JO - Physical review letters
JF - Physical review letters
IS - 7
M1 - 070401
ER -