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This key to this problem is the identity x sin x = ∏ k = 1 ∞ cos ( 2 k x ) . Once this identity is applied, the integral becomes routine. This formula, I think, is credited to Euler and you may have come across it if you've studied Fourier transforms, but if you haven't seen it before, here's a quick proof:
By applying the double angle identity over and over we get: sin x = 2 sin 2 x cos 2 x = 4 sin 4 x cos 4 x cos 2 x ⋮ = 2 n sin 2 n x k = 1 ∏ n cos 2 k x
Taking the limit as n → ∞ we get sin x = k = 1 ∏ ∞ cos 2 k x ( n → ∞ lim 2 n sin 2 n x )
Now, as n → ∞ , 2 n x → 0 , so by the small angle approximation sin 2 n x → 2 n x . Hence, lim n → ∞ 2 n sin 2 n x = x .