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Complexity enriched dynamical phases for fermions on graphs
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abstract
Dynamical quantum phase transitions, encompassing phenomena like many-body localization transitions and measurement-induced phase transitions, are often characterized and identified through the analysis of quantum entanglement. Here, we highlight that the dynamical phases defined by entanglement are further enriched by complexity. We investigate both the entanglement and Krylov complexity for fermions on regular graphs, which can be implemented by systems like $^6$Li atoms confined by optical tweezers. Our investigations unveil that while entanglement follows volume laws on both types of regular graphs with degree $d = 2$ and $d = 3$, the Krylov complexity exhibits distinctive behaviors. We analyze both free fermions and interacting fermions models. In the absence of interaction, both numerical results and theoretical analysis confirm that the dimension of the Krylov space scales as $D\sim N$ for regular graphs of degree $d = 2$ with $N$ sites, and we have $D\sim N^2$ for $d = 3$. The qualitative distinction also persists in interacting fermions on regular graphs. For interacting fermions, our theoretical analyses find the dimension scales as $D\sim 4^{N^\alpha}$ for regular graphs of $d = 2$ with $0.38\leq\alpha\leq0.59$, whereas it scales as $D\sim 4^N$ for $d = 3$. The distinction in the complexity of quantum dynamics for fermions on graphs with different connectivity can be probed in experiments by measuring the out-of-time-order correlators.
Forward citations
Cited by 2 Pith papers
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Correlations and Krylov spread for a non-Hermitian Hamiltonian: Ising chain with a complex-valued transverse magnetic field
For a non-Hermitian Ising chain, the Krylov spread detects three dynamical phases in the gapped-spectrum region and is analytically related to the spin-spin correlation function.
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Quantum complexity phase transition in fermionic quantum circuits
A measure of operator spreading, Krylov complexity, undergoes a phase transition in quantum percolation: at the percolation threshold for free fermions, but at a lower threshold p=1/4 for 1D interacting fermions.
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