We develop linear, fully decoupled first- and second-order time-discretization schemes for the Cahn–Hilliard–Navier–Stokes system, by integrating the multiple scalar auxiliary variables (MSAV) approach with the Gauge–Uzawa (GU) method. The schemes are proved to ensure both mass conservation and unconditional energy stability. Moreover, by reformulating the system into matrix form, we present two linearly decoupled numerical solution algorithms through Gaussian elimination: a commonly adopted decoupled method with constant-coefficient matrices and an alternative approach involving solution-dependent coefficient matrices. Both schemes involve only solving a series of Poisson-type equations alongside a straightforward linear algebraic system at each time step. Notably, the proposed methods eliminate the need for artificial pressure boundary conditions. Besides, a rigorous error analysis of the first-order scheme is conducted, in which the idea of high-order consistency analysis is employed for the intermediate velocity by introducing an auxiliary momentum equation. It is shown that the scheme achieves optimal temporal convergence rates for the phase function and velocity across various norms. Finally, numerical experiments are performed to validate the theoretical findings and demonstrate the performance of the proposed schemes.
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