We study coupled mass transport in a tumor–microenvironment setting with two motile densities and non-motile state switching . The populations diffuse and undergo chemotactic drift; follow pointwise ODE switching. A decoupled inhibitory field satisfies a damped Neumann heat equation, giving maximum-principle bounds and exponential decay. Together with the pointwise invariant , these identities yield global existence, positivity, and long-time reduction to limiting kinetics with a unique globally attracting coexistence state. Neumann eigenmode reduction gives closed dispersion relations. The base reaction–diffusion block remains stable for all nonconstant modes for any , excluding classical Turing destabilization. Chemotaxis is posed via a diffusive cue , since is undefined for non-diffusive . In one-way damped coupling, the linearized mode matrix is block triangular and leaves the spectrum unchanged. Two-way coupling adds a feedback rank-one mobility correction, induces effective cross-diffusion, and admits mode growth. We give explicit trace/determinant criteria for unstable Laplacian modes and the resulting instability thresholds.

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