AbstractWe prove the existence of small amplitude, time-quasi-periodic solutions (invariant tori) for the incompressible Navier–Stokes equation on the d-dimensional torus $$\mathbb T^d$$
T
d
, with a small, quasi-periodic in time external force. We also show that they are orbitally and asymptotically stable in $$H^s$$
H
s
(for s large enough). More precisely, for any initial datum which is close to the invariant torus, there exists a unique global in time solution which stays close to the invariant torus for all times. Moreover, the solution converges asymptotically to the invariant torus for $$t \rightarrow + \infty $$
t
→
+
∞
, with an exponential rate of convergence $$O( e^{- \alpha t })$$
O
(
e
-
α
t
)
for any arbitrary $$\alpha \in (0, 1)$$
α
∈
(
0
,
1
)
.