A double cover is a mathematical concept where one space "covers" another in such a way that each point in the base space corresponds to exactly two points in the covering space.
Example: The Circle and the Line
A simple example is the map f:R→S1f: \mathbb{R} \to S^1f:R→S1 given by:
f(θ)=eiθf(\theta) = e^{i\theta}f(θ)=eiθ
Here, every point on the unit circle S1S^1S1 corresponds to infinitely many points on R\mathbb{R}R, but if we restrict the domain to [0,2π)∪[π,3π)[0, 2\pi) \cup [\pi, 3\pi)[0,2π)∪[π,3π), each point on S1S^1S1 corresponds to exactly two points. This makes it a double cover when restricted appropriately.
Example: Spin(n)Spin(n)Spin(n) and SO(n)SO(n)SO(n)
For rotation groups, Spin(n)Spin(n)Spin(n) is a double cover of SO(n)SO(n)SO(n), meaning that every rotation in SO(n)SO(n)SO(n) corresponds to two elements in Spin(n)Spin(n)Spin(n). The map from Spin(n)→SO(n)Spin(n) \to SO(n)Spin(n)→SO(n) identifies these two elements as equivalent, but in the covering space Spin(n)Spin(n)Spin(n), they remain distinct.
This is crucial in physics and mathematics because in even dimensions, these two elements in Spin(2k)Spin(2k)Spin(2k) can correspond to "left-handed" and "right-handed" rotations, which is directly related to the chirality question you're investigating.