[en] $\mathcal{P}\mathcal{T}$-symmetric quantum mechanics, the extension of conventional quantum mechanics to the non-Hermitian Hamiltonian invariant under the combined parity ($\mathcal{P}$) and time reversal ($\mathcal{T}$) symmetry, has been successfully applied to a variety of fields—such as solid state physics, mathematical physics, optics, quantum field theory. Recently, the extension of $\mathcal{P}\mathcal{T}$-symmetrical theory to entangled quantum systems has been challenged, in that $\mathcal{P}\mathcal{T}$ formulation within the conventional Hilbert space violates the no-signaling principle. Here, we revisit the derivation of non-signaling principle in the framework of $\mathcal{C}\mathcal{P}\mathcal{T}$ inner product prescription. Our results preserve the no-signaling principle for a two-qubit system, reaffirm the invariance of the entanglement, and reproduce the Clauser–Horne–Shimony–Holt (CHSH) inequality. We conclude that $\mathcal{P}\mathcal{T}$-symmetric quantum mechanics satisfies the requirements for a fundamental theory and provides a consistent description of quantum systems. (paper)