Abstract
We study the growth and saturation of Krylov spread (K-) complexity under random quantum circuits. In Haar-random unitary evolution, we show that, for large system sizes, K-complexity grows linearly before saturating at a late-time value of $D/2$, where $D$ is the Hilbert space dimension, at timescales $\sim D$. Our numerical analysis encompasses two classes of random circuits: brick-wall random unitary circuits and Floquet random circuits. In brick-wall case, K-complexity exhibits dynamics consistent with Haar-random unitary evolution, while the inclusion of measurements significantly slows its growth down. For Floquet random circuits, we show that localized phases lead to reduced late-time saturation values of K-complexity, forbye we utilize these saturation values to probe the transition between thermal and many-body localized phases.
| Original language | English |
|---|---|
| DOIs | |
| Publication status | Published - 5 Sept 2024 |
Bibliographical note
major changes in fig 1. 7 pages, 3 figuresKeywords
- quant-ph
- cond-mat.dis-nn
- cond-mat.stat-mech
- cond-mat.str-el
- hep-th
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