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d H φ H d L φ L m <br />
θ m <br />
|F (θ m )| = d<br />
mπ sin(mπγ)(φ H − φ L ) (3.27)<br />
φ |F (θ)| <br />
m m <br />
R m R I m R m = tanh 2 A (3.28)<br />
A <br />
R I m = A tan θ m<br />
mN<br />
tanh A (3.29)<br />
A = 2KNd<br />
m |F (θ m)| (3.30)<br />
K σ K σ =1π K π =| cos 2θ m | d <br />
A ≪ 1tanh A ≅ A (3.29) (3.28) <br />
R m = tanh 2 A ≅ A 2 (3.31)<br />
R I m = A tan θ m<br />
mN<br />
tanh A ≅ A2 tan θ m<br />
mN<br />
(3.32)<br />
<br />
(3.30) A K <br />
R m R I m K2 σ <br />
R mσ π R mπ R I mσ <br />
R I mπ <br />
R mπ<br />
R mσ<br />
= RI mπ<br />
R I mσ<br />
=<br />
( Kπ<br />
K σ<br />
) 2<br />
= cos 2 2θ m (3.33)<br />
(10keV ) θ m ≪ 1 (3.33) <br />
R mπ<br />
R mσ<br />
= RI mπ<br />
R I mσ<br />
= cos 2 2θ m ≅ 1 − 4θ 2 m (3.34)<br />
(3.18) θ 2 θ 1<br />
X 10 keV θ m