In mathematics, a Cauchy matrix, named after Augustin-Louis Cauchy, is an m×n matrix with elements aij in the form
where [math]\displaystyle{ x_i }[/math] and [math]\displaystyle{ y_j }[/math] are elements of a field [math]\displaystyle{ \mathcal{F} }[/math], and [math]\displaystyle{ (x_i) }[/math] and [math]\displaystyle{ (y_j) }[/math] are injective sequences (they contain distinct elements).
The Hilbert matrix is a special case of the Cauchy matrix, where
Every submatrix of a Cauchy matrix is itself a Cauchy matrix.
The determinant of a Cauchy matrix is clearly a rational fraction in the parameters [math]\displaystyle{ (x_i) }[/math] and [math]\displaystyle{ (y_j) }[/math]. If the sequences were not injective, the determinant would vanish, and tends to infinity if some [math]\displaystyle{ x_i }[/math] tends to [math]\displaystyle{ y_j }[/math]. A subset of its zeros and poles are thus known. The fact is that there are no more zeros and poles:
The determinant of a square Cauchy matrix A is known as a Cauchy determinant and can be given explicitly as
It is always nonzero, and thus all square Cauchy matrices are invertible. The inverse A−1 = B = [bij] is given by
where Ai(x) and Bi(x) are the Lagrange polynomials for [math]\displaystyle{ (x_i) }[/math] and [math]\displaystyle{ (y_j) }[/math], respectively. That is,
with
A matrix C is called Cauchy-like if it is of the form
Defining X=diag(xi), Y=diag(yi), one sees that both Cauchy and Cauchy-like matrices satisfy the displacement equation
(with [math]\displaystyle{ r=s=(1,1,\ldots,1) }[/math] for the Cauchy one). Hence Cauchy-like matrices have a common displacement structure, which can be exploited while working with the matrix. For example, there are known algorithms in literature for
Here [math]\displaystyle{ n }[/math] denotes the size of the matrix (one usually deals with square matrices, though all algorithms can be easily generalized to rectangular matrices).
Original source: https://en.wikipedia.org/wiki/Cauchy matrix.
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