It is very common in the literature to write down a Markovian quantum master equation in Lindblad form to describe a system with multiple degrees of freedom and weakly connected to multiple thermal baths which can, in general, be at different temperatures and chemical potentials. However, the microscopically derived quantum master equation up to leading order in system-bath coupling is of the so-called Redfield form which is known to not preserve complete positivity in most cases. We analytically show that, in such cases, enforcing complete positivity by imposing any Lindblad form, via any further approximation, necessarily leads to either violation of thermalization, or inaccurate coherences in the energy eigenbasis which then cause a violation of local conservation laws in the non-equilibrium steady state (NESS). In other words, a weak system-bath coupling quantum master equation that is completely positive, shows thermalization and preserves local conservation laws in NESS is fundamentally impossible in generic situations. On the other hand, the Redfield equation, although generically not completely positive, shows thermalization, always preserves local conservation laws and gives correct coherences to leading order. We exemplify our analytical results numerically in an interacting open quantum spin system.
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