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Note first that
A = ∫ 0 1 sin 2 x − tan ( tan x ) ln ( cos 2 x ) cos 2 x − tan x cot ( tan x ) d x = ∫ 0 1 sin 2 x cot ( tan x ) − 2 ln ( cos x ) cos 2 x cot ( tan x ) − tan x cot 2 ( tan x ) d x and putting u = sin 2 x cot ( tan x ) − 2 ln ( cos x ) for 0 < u < tan − 1 π gives lim x → 0 u = 2 and d x d u = 2 cos 2 x cot ( tan x ) − sin 2 x c o s e c 2 ( tan x ) sec 2 x + 2 tan x = 2 cos 2 x cot ( tan x ) − 2 tan x ( c o s e c 2 ( tan x ) − 1 ) = 2 [ cos 2 x cot ( tan x ) − tan x cot 2 ( tan x ) ] and hence, putting α = sin 2 cot ( tan 1 ) − 2 ln ( cos 1 ) we see that A = ∫ 2 α 2 u d u = 2 1 ln ( 2 α ) = 2 1 ln ( 2 1 sin 2 cot ( tan 1 ) − ln ( cos 1 ) ) which makes ⌊ 1 0 0 0 0 A ⌋ = − 2 3 7 7 .