In this article, wikipedia describes a constantly accelerated rocket, assuming special relativity : $$ x(\tau) \;=\; \frac{c^2}{a} \left(\cosh \frac{a \ \tau}{c} -1 \right) $$ The proper time $\tau$ is less than $\frac{d_0}{c}$, where $d_0$ is the distance to the foreign star. For example, Alpha centauri is 4.37 light-years away from Earth, and the constantly accelerated rocket arrives there in 3.6 years (including the deceleration on the second half of the trip).
Doesn't this mean that, from the rocket's perspective, Alpha centauri moves faster than light ?
Let $d(\tau)$ be the distance from the rocket to Alpha centauri, as perceived by the rocket. That's the length of the spacelike geodesic orthogonal to the rocket's 4-speed, joining the rocket and the star. $d(0)$ is 4.37 light-years, when the rocket leaves Earth and $d(3.6)$ is zero, when the rocket reaches the star. By the mean value theorem, at some proper time $\tau$, $|\frac{dd}{d\tau}|>c$.