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The spin operator along an arbitrary direction = (sin 0 cos 0) is defined as sin 0 sin o cos (1.18) h where S 2 _ (a) Find th

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bs girea, (in cesti (Sins sin + SaK and whare () () & Y So th 3ind Cos Sino sinb 1 O Ccos isinp Sing (etin) ine CosO in8 madrshen get 3inS i 2 - Cos sin e. - i4 b e a which a (1- coss and the relationo - 2 sin and b atan 2 3 ta121 Condition normalisaGo terun Spinom Crite th twe Cen (.)-i etono K1- 91 () Sin 2 Con0 1 A.Y e Cos Aohution tre pherionn (tahich neduces to Coso a

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