A rigid body really rotates about one default axis (through the centre of mass, or the door hinges) with angular speed ω.
You can also observe parallel axes a distance d away. By the parallel-axis theorem, inertia about that axis is I′ = I₀ + md². For the same angular momentum, the related speed is ω′ = I₀ω / (I₀ + md²).
So farther axes mean larger I′ and a smaller ω′ compared with ω.