Circular
polarization is said to be right-handed if the direction of rotation is clockwise when viewed
against the direction of
propagation and left-handed if the sense of the rotation is opposite. When the position of the
endpoint of the electric vector is viewed at a given time
t as a function of distance along x, it forms a left-handed
helix if the light
polarization is left-handed and a right-handed
helix is it is right-handed.