Page 596 - Introduction to Information Optics
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Mueller matrices 0~ sin 20 sin 20 cos 20 0 0 sin 2 20 0_ 0 0 0 —sin 20 cos S ( 1 — cos S) sin 20 cos 20 cos 20 sin 6 sin 2 20 + eos 2 20cos<5 cos (5 —cos 20 sin d
cos 20 cos 2 20 2 sin 20 sin 20 cos 20 0 0 cos 2 20 + sin 2 20cos(5 0 (1 — cos d) sin 20 cos 20 sin 20 sin <5 Q~ 0 sin 20 0 0 -sin 20 cos 20 0 1_ 0
f 1 i cos 20 0 1 " 0 0 0 1 cos 20 0 0 J)
Table 10.2 Jones and Mueller Matrices for Linear Polarizer, Linear Retarder, and Rotation Matrices
(e u - 1) sin 0 cos 01
Jones matrices sin 0 cos 01 sin 2 0 j |_(e — I)sin0cos0 e sin 0 + cos 0 J COS0J
f cos 2 0 [sin 0 cos 0 IV 15 cos 2 0 + sin 2 0 cos 0 sin 0 1 [ — sin0
Type of component Linear polarizer: Transmission axis at angle 0 to the axis in the x-y plane Linear retarder: Fast-axis angle 0 to the x axis in the x-y plane, retardation (5 ~ (5 — <5 y x Rotation transform with rotation
