Rule 201 in the deterministic Floquet-PXP model admits exact finite-dimensional MPO influence matrices for subsystem dynamics that solve algebraic conditions.
Influence-solvability: a systematic theory of $(1+1)D$ solvability and its application to brickwork circuits
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abstract
`Solvable' circuits, such as dual unitaries and its generalisations, have arisen as paradigmatic examples of tractable chaotic non-equilibrium dynamics, both in classical and quantum systems. However, while increasingly more complicated sufficient conditions have been proposed, a systematic theory classifying and understanding general features of solvable circuits is missing. We develop such a theory by introducing influence-solvable circuits, a class of $(1+1)D$ circuits whose influence matrix, which represents the `bath' generated by its own evolution, is given by a uniform MPS with finite bond-dimension $\chi$. This property allows for efficient computation of subsystem dynamics and essentially contains all known examples of solvable circuits. We derive a set of necessary and sufficient local conditions by using a version of the fundamental theorem of MPS for open boundary conditions. Next we apply our theory to brickwork circuits with $\chi=1$ influence-solvability and perform a systematic classification of classical brickwork circuits with local dimension up to $d=3$ and quantum brickwork circuits with $d=2$. Our search reveals new solvable circuits that are not captured by known solvability conditions.
fields
cond-mat.stat-mech 1years
2026 1verdicts
UNVERDICTED 1representative citing papers
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Exact subsystem dynamics in the deterministic Floquet-PXP model
Rule 201 in the deterministic Floquet-PXP model admits exact finite-dimensional MPO influence matrices for subsystem dynamics that solve algebraic conditions.