Dynamics and equilibration in integrable and solvable interacting models
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This thesis studies the dynamics and equilibration of interacting quantum systems in which integrability, or the structure of conserved charges, shapes the long-time behavior. The In- troduction (Chapter 1) sets up machinery that the later chapters draw on: linear response and the fluctuation-dissipation theorem, large deviations and cumulant-generating functions, quantum state ensembles, and spectral diagnostics of chaos. With these in place, the four research chapters trace a single arc. They move from closed-system transport, to full counting statistics in boundary-driven steady states, to projected ensembles in systems with extensively many conserved charges, and finally to chaos diagnostics suited to near-term quantum hardware. The common technical thread is matrix product state methods (introduced in Chapter 2), combined with analytic input from (quasi-)local conserved quantities, to access regimes where integrability or solvability produces behavior outside the reach of generic thermalization arguments. Chapter 3 applies time-dependent DMRG to thermal transport in a chiral Z3 clock chain tuned along an integrable, time-reversal symmetric line. The thermal current’s finite overlap with a local conserved charge Q(2) obtained from the transfer matrix yields a Mazur bound that saturates the Drude weight at finite temperature, validated against a sum rule. Chapter 4 studies the boundary-driven XXZ chain, whose non-equilibrium steady state under maximally polarising Lindblad operators admits an exact matrix product solution. In the XX limit we obtain closed-form spin correlators, entropy per site, and SCGFs of local observables. For ∆ > 0 a cosine of a rational multiple of π, the MPS yields numerically exact SCGFs and rate functions for the local z-magnetisation, with finite-size corrections decaying exponentially at a rate discontinuous in ∆. A double-peak structure in the x-magnetisation density for ∆ ≲ 1 is suggestive of short-range ferromagnetic ordering. Chapter 5 uses the projected ensemble—subsystem states conditioned on measurements of the complement, to probe deep thermalisation in systems with extensively many (quasi-)local conserved charges. In a Floquet spin chain deep in its MBL regime and the ℓ-bit model as a 1-local archetype, the late-time projected ensemble converges to a Scrooge ensemble except when the measurement operator aligns with the conserved charges, a behaviour we link to the emergence of Porter–Thomas bitstring statistics and justify with semi-analytical arguments. Chapter 6 carries these diagnostics onto probes scalable on current quantum hardware, studying the mixed-field quantum Ising model on Erdős–Rényi graphs whose connectivity interpolates the dynamics between localized, chaotic, and permutation-symmetric integrable regimes–a crossover with implications for the trainability of variational algorithms such as QAOA. The regimes are characterized through convergence of the projected ensemble to Haar, a partial spectral form factor as a resource-efficient SFF proxy, and operator Krylov complexity, which is maximized in the chaotic regime. Taken together, the four chapters trace a path in which the role of conservation laws on quantum dynamics is investigated with progressively sharper probes.
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