
We study the conditions under which one can conserve local translationally invariant operators by local translationally invariant Lindblad equations in one-dimensional rings of spin-1/2 particles. We prove that for any 1-local operator (e.g., particle density) there exist Lindblad dissipators that conserve that operator, while on the other hand we prove that among 2-local operators (e.g., energy density) only trivial ones of the Ising type can be conserved, while all the other cannot be conserved, neither locally nor globally, by any 2- or 3-local translationally invariant Lindblad equation. Our statements hold for rings of any finite length larger than some minimal length determined by the locality of Lindblad equation. These results show in particular that conservation of energy density in interacting systems is fundamentally more difficult than conservation of 1-local quantities.
Quantum Physics, Lindblad equations, Statistical Mechanics (cond-mat.stat-mech), Unified quantum theories, conservation of energy, FOS: Physical sciences, Quantum Physics (quant-ph), Lattice systems (Ising, dimer, Potts, etc.) and systems on graphs arising in equilibrium statistical mechanics, Condensed Matter - Statistical Mechanics
Quantum Physics, Lindblad equations, Statistical Mechanics (cond-mat.stat-mech), Unified quantum theories, conservation of energy, FOS: Physical sciences, Quantum Physics (quant-ph), Lattice systems (Ising, dimer, Potts, etc.) and systems on graphs arising in equilibrium statistical mechanics, Condensed Matter - Statistical Mechanics
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