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Let Aφ= cosφ −sinφ sinφ cosφ • A is the matrix of rotation by angle φ • AφAψ= Aφψ • AT φ = A−φ • A−1 φ = A−φ= A T φ • Columns of Aφ form an orthonormal basis for R2 • Rows of Aφ form an orthonormal basis for R2. N p y t p \ p v y t n r q q r v n p z t x y r x n p v n t s w s t v n u n t s s r q n q p o n m l k ^ t z p x n t s s r q n q r v c b a ` 2 0 > 6 ;. H pdlo lqir vdlwr ye#jpdlo frp í#æ3¸ ¥4# b z v w Ü bh pdlo @ ¶ ^ 8 c e 8 o z c t i 8 ^ 8 b ¬ « Ï î ¶ 7d _ ° k z > 8 z c t i 8 @ ²0 m _0° ° b v3æ Ü k z c t i 8 í ± \ ¥.

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3z Ñ ± @8ô;\3° b) 8 _ P K b ^ Ó Ü µ º @ 6 \ K Z 8 H M&g 8 S T A S 8 >& j & É %4 p ¸8ô;\3° ) æ/²# ¦) 6×>'. T he de re gi s t ra t i on of t he c om m on s t oc k unde r S e c t i on 12(b) of t he S e c uri t i e s E xc ha nge A c t of 1934 (t he “ E xc ha nge A c t ” ) w i l l be e ffe c t i ve 90 da ys , or s uc h s hort e r pe ri od a s t he S E C m a y de t e rm i ne , a ft e r fi l i ng of t he F orm 25. Is a p # 1 v ecto r of unk no wn consta n ts, a nd " is m ultiv aria te nor mal with mean zero and co v a riance mat rix "2 I n, w here "2 > 0 is a consta n t In the fo llowing , it ma y b e helpful to reca ll tha t (A" 1.

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