Let xi=L/fi, with positive f focusing in the first transverse plane. The doublet matrix is M=Q2D(L)Q1, with Qi=(1−1/fi01). Its lower-left entry is Cx=−(x1+x2−x1x2)/L. In the other plane both quadrupolesigns reverse, giving Cy=−(−x1−x2−x1x2)/L. Thus positive effective focusing power in both planes requires
For a parallel incident ray bundle, actual downstream focal distances are ℓx=L(1−x1)/(x1+x2−x1x2) and ℓy=L(1+x1)/(−x1−x2−x1x2). Requiring both foci downstream adds ∣x1∣<1. Positive effective power alone need not imply a real image after the final element. The original schematic below distinguishes these conditions.