  We establish a duality between open many-body systems governed by the
Gorini-Kossakowski-Sudarshan-Lindblad (GKSL) equation and satisfying the
detailed balance condition on the one side, and closed bilayer systems with a
self-adjoint Hamiltonian on the other side. Under this duality, the identity
operator on the open system side maps to the thermofield double state which
turns out to be a quantum many-body scar of the dual Hamiltonian $\mathcal H$.
A remarkable feature of this thermofield scar is a tunable entanglement entropy
controlled by the reservoir temperature on the open system side. Further, we
identify broad classes of many-body open systems with nontrivial explicit eigen
operators $Q$ of the Lindbladian superoperator. The expectation values of the
corresponding observables exhibit a simple exponential decay, $\langle
Q\rangle_t=e^{-\Gamma t} \langle Q \rangle_0$, irrespectively of the initial
state. Under the above duality, these eigen operators give rise to additional
(towers of) scars. Finally, we point out that more general superoperators (not
necessarily of the GKSL form) can be mapped to self-adjoint Hamiltonians of
bilayer systems harbouring scars, and provide an example thereof.
