Weak Gaussian noise in control fields makes dissipation grow linearly with steps in quantum equilibration, yielding a finite optimal step count and minimal dissipated work derived from quantum thermodynamic length.
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Classical-quantum gravity with completely positive dynamics admits an embedding into a fully quantum theory on an enlarged Hilbert space, illustrated by a hybrid qubit-classical particle system that violates angular momentum conservation despite rotational symmetry.
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Finite steps optimise dissipation in stochastically controlled quantum systems
Weak Gaussian noise in control fields makes dissipation grow linearly with steps in quantum equilibration, yielding a finite optimal step count and minimal dissipated work derived from quantum thermodynamic length.
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Classical-quantum gravity as quantum gravity in disguise
Classical-quantum gravity with completely positive dynamics admits an embedding into a fully quantum theory on an enlarged Hilbert space, illustrated by a hybrid qubit-classical particle system that violates angular momentum conservation despite rotational symmetry.