“…As in section II, in order to analyze cosmic parallax we need to find null geodesics in the spacetime that connect an observer and various sources at two different times. Letting latin indices run over 1, 2, 3 and (x 0 , x 1 , x 2 , x 3 ) = (t, x, y, z), the non-zero Christoffel symbol components for the Bianchi-I metric in (13) are…”