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math105-s22:s:jianzhi:start [2022/04/28 04:45]
jianzhi [FFT, Wavelet Transformation, Uncertainty Principle (The Last Presentation)]
math105-s22:s:jianzhi:start [2026/02/21 14:41] (current)
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 Remark: This problem is also equivalent to evaluating a polynomial at the roots of unity, the so-called changing from coefficient representation to value representation. Remark: This problem is also equivalent to evaluating a polynomial at the roots of unity, the so-called changing from coefficient representation to value representation.
  
-**Fast Fourer Transform**+**Fast Fourier Transform**
  
 A naive implementation of the Discrete Fourier Transform takes $O(N^2)$. However, Fast Fourier Transform performs it in $O(N log N)$ by exploiting the symmetry of the roots of unity. A naive implementation of the Discrete Fourier Transform takes $O(N^2)$. However, Fast Fourier Transform performs it in $O(N log N)$ by exploiting the symmetry of the roots of unity.
  
-An illustration of idea is: break down the polynomial into even and odd terms. We can recycle many computations. Use 1 and -1 as an example.+An illustration of idea is: break down the polynomial into even and odd terms. We can recycle many computations. Use $1and $-1as an example.
  
 **Inverse Fourier Transform** **Inverse Fourier Transform**
  
-$y_j = \frac{1}{N} \Sigma_{k=0}^{N-1} c_k e^{\frac{2 \pi ijk}{N}$+$y_j = \frac{1}{N} \Sigma_{k=0}^{N-1} c_k e^{\frac{2 \pi ijk}{N}}$
  
 The trick here is to notice that the inverse matrix is just another Vandermonde matrix with $\bar{\omega}$ instead of $\omega$.  The trick here is to notice that the inverse matrix is just another Vandermonde matrix with $\bar{\omega}$ instead of $\omega$. 
math105-s22/s/jianzhi/start.1651121146.txt.gz · Last modified: 2026/02/21 14:43 (external edit)