Chapter 1 The Fourier Transform
tions f as di erentiable everywhere, vanishing at t= ˇLand identically zero outside [ ˇL;ˇL]. We rewrite this as f(t) = X1 n=1 eint L 1 2ˇL f^(n L) which looks like a Riemann sum approximation to the integral f(t) = 1 2ˇ Z 1 1 f^( )ei td (1.2.1) 3
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