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(3.35),(3.36) <br />
P ′ 0 = R σI ∥ − R π<br />
1−P<br />
1+P I ∥<br />
R σ I ∥ + R π<br />
1−P<br />
1+P I ∥<br />
= sin2 2θ + (1 + cos 2 2θ)P<br />
(1 + cos 2 2θ) + sin 2 2θP<br />
(3.38)<br />
(3.39)<br />
β=90 ◦ β = 0 ◦ <br />
P ′ 90 <br />
P ′ 90 = − sin2 2θ + (1 + cos 2 2θ)P<br />
(1 + cos 2 2θ) − sin 2 2θP<br />
(3.40)<br />
P < sin 2 2θ/(1 + cos 2 2θ) ∼ 2θ 2 P P ′ 90 <br />
|P ′ 90 | P′ 90 < 0 θ = 2◦ <br />
P