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In this chapter we consider the first problem posed in the introduction
where the matrix and vector are given and we want to interpret and give structure to the calculation of the vector . Equation [link] has a variety of special cases. The matrix may be square or may be rectangular. It may have full column or row rank or it may not. It may be symmetric or orthogonalor non-singular or many other characteristics which would be interesting properties as an operator. If we view the vectors as signals and thematrix as an operator or processor, there are two interesting interpretations.
An example of the first would be the discrete Fourier transform (DFT) where one calculates frequency components of a signal which arecoordinates in a frequency space for a given signal. The definition of the DFT from [link] can be written as a matrix-vector operation by which, for and , is
An example of the second might be convolution where you are processing or filtering asignal and staying in the same space or coordinate system.
A particularly powerful sequence of operations is to first change the basis for a signal, then process the signal in this new basis, and finally returnto the original basis. For example, the discrete Fourier transform (DFT) of a signal is taken followed by setting some of the Fourier coefficients tozero followed by taking the inverse DFT.
Another application of [link] is made in linear regression where the input signals are rows of and the unknown weights of the hypothesisare in and the outputs are the elements of .
Consider the two views:
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