2007/01/23 by Tim Schmiedl, Udo Seifert · 395 citations
Mathematics · Physics and Astronomy · #Advanced Thermodynamics and Statistical Mechanics #Applied mathematics #Mathematical optimization #Mathematics #Optimal control #Particle (ecology) #Physics #Protocol (science) #Quantum Electrodynamics and Casimir Effect #Quantum Mechanics and Applications #Statistical physics #Stochastic differential equation #Thermodynamics #Trap (plumbing) #Work (physics) #cond-mat.soft #cond-mat.stat-mech
paper · pdf · doi:10.1103/physrevlett.98.108301
published in Physical Review Letters 98(10), 108301 (American Physical Society) · 4 pages, 1 figure, accepted for publication in Phys. Rev. Lett
arxiv created 2007/01/23 · openalex publication_date 2007/03/07 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/08
For a small system like a colloidal particle or a single biomolecule embedded in a heat bath, the optimal protocol of an external control parameter minimizes the mean work required to drive the system from one given equilibrium state to another in a finite time. In general, this optimal protocol obeys an integro-differential equation. Explicit solutions both for a moving laser trap and a time-dependent strength of such a trap show finite jumps of the optimal protocol to be typical both at the beginning and at the end of the process.