We extend the exponential stability theorem for the three-dimensional incompressible Navier-Stokes equations from hyperbolic 3-space (established in a companion paper) to complete simply connected Riemannian 3-manifolds with pinched negative sectional curvature and bounded geometry (including a strictly positive injectivity radius). The deformation Laplacian remains the viscous operator, selected by Lagrangian kinematics. We prove that the {exact} system admits a unique global mild solution for small data, with exponential decay at a rate determined by the spectral gap of the Stokes operator. The extension overcomes three obstacles absent on : (i) the semigroup factorisation fails because is not a scalar multiple of the metric; (ii) the Leray projector no longer commutes with ; (iii) the exact spectral gap is unknown. We resolve (i) unconditionally, without any curvature restriction, by observing that the Ricci perturbation is negative semi-definite and applying a Trotter product bound with the diamagnetic inequality. We resolve (ii) by an algebraic reduction of the commutator to the complementary projector applied to the shifted Ricci endomorphism, giving a clean zeroth-order bound proportional to the curvature variation . This is the sole source of a curvature pinching constraint. We resolve (iii) via McKean’s theorem, the diamagnetic inequality, and the Weitzenböck identity. The Fujita-Kato temporal singularity exponent is unchanged from the case, confirming that the ultraviolet scaling obstruction is local and geometry-independent, driven fundamentally by an unresolvable temporal scaling mismatch.

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