The parallel index of refraction is defined as
| (41) |
Here Bj are the contravariant coordinates of B, given by
| (42) |
where
| (43) |
such that the contravariant coordinates of B are
| (44) |
where α is the angle between to such that
| (45) |
Because is orientated outward we have -π∕2 < α < π∕2. Then (??) yields
| (46) |
where P = and T = .