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Showing posts from March, 2023

More on matrix determinants

The determinant of a general n×n matrix is quite complicated. We give a mechanical, recursive definition first and then think about its meaning later. Definition (Determinant) Let A=(aij)Mn. The determinant |A| of A is defined recursively in the following manner. If n=1, then |A|=a11. If n>1, then let Aij denote the (n1)×(n1) matrix obtained by removing the i-th row and the j-th column from A, and |A|=j=1n(1)i+jaij|Aij| where i is any arbitrary index from 1 to n. (Instead of a row, you may use an arbitrary column to obtain the same result.) According to this definition, if we want to compute |A| of an n×n matrix, we need to compute the determinants |Aij| of (many) (n1)×(n1) matrices, which requires computing determinants of (n2)×(n2) matrices, and so on, until we reach the determinants of 1×1 matrices which are tri...

Fourier transform

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So far we have been studying the Fourier series of functions with period 2π. What about the functions with periods other than 2π? Furthermore, what about non-periodic functions? In this section, we consider these problems informally and briefly.  Suppose f is a smooth function with a period of 2lπ where l>0 is a constant. We have (eq:f2lpi)f(x)=k=ckeikx/l and the right-hand side converges uniformly. The Fourier coefficients are given by ck=12πllπlπf(x)eikx/ldx   (kZ). Thus, the Fourier series can be readily extended to any periodic function with period other than 2π. Next, we consider functions that are not necessarily periodic. Suppose that f is a function of class C1 with a bounded support.  Remark . The support supp(f) of a function f is the subset of the domain, defined by \[\mathrm{supp}(f) = \{x \in \mathbb{R} \mid f(...