Boosting thermalization of classical and quantum many-body systems
Designing the coupling to an environment offers a way to prepare many-body thermal states faster while preserving the target equilibrium state.
RESEARCH ARCHIVE
Quantum correlations, nonequilibrium dynamics, and the geometry of control.
Complete publication list on Google ScholarDesigning the coupling to an environment offers a way to prepare many-body thermal states faster while preserving the target equilibrium state.
Systematic optimization helps identify multipartite Bell tests with stronger quantum violations, supporting the search for experimentally useful nonlocality witnesses.
Optimizing spectral gaps along a preparation path helps reduce the bottlenecks that make adiabatic quantum-state preparation slow.
Extends standard nonequilibrium relations so they still work in relativistic settings.
Clarifies how to model open quantum dynamics without losing thermodynamic consistency.
Explains which notion of quantum work remains useful when initial coherence is present.
Organizes several fluctuation relations into one unified picture for driven systems.
Connects quantum heat fluctuations with their classical Brownian-motion limit.
Provides an explicit optimal-control recipe for pushing Brownian engines to maximum power.
A geometric bound quantifies the extra energy needed for fast membrane separation and identifies paths that reduce that cost.
Uses geometric control ideas to improve finite-time Brownian engine performance.
Introduces a geometric control principle for faster adiabatic quantum evolution.
Moves beyond average efficiency and characterizes the full performance fluctuations of the engine.
Finite-duration measurements can estimate thermodynamic length, making a quantity that bounds dissipation accessible without infinitely slow experiments.
Shows that a finite-time quantum Otto engine can outperform standard maximum-power benchmarks.
Shows how carefully timed control can improve both power and efficiency in Otto engines.
Shows how particle interactions reshape the efficiency of a quantum Otto engine.
Shows what continuous monitoring changes, and what it preserves, in mesoscopic transport.
Identifies observable finite-time signatures of first-order phase transitions.
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