Padé approximant is the "best" approximation of a function by a rational function of given order - under this technique, the approximant's power series agrees with the power series of the function it is approximating. The technique was developed by Henri Padé, but goes back to Georg Frobenius who introduced the idea and investigated the features of rational approximations of power series.
The Padé approximant often gives better approximation of the function than truncating its Taylor series, and it may still work where the Taylor series does not converge. For these reasons Padé approximants are used extensively in computer calculations. They have also been used as auxiliary functions in Diophantine approximation and transcendental number theory, though for sharp results ad hoc methods in some sense inspired by the Padé theory typically replace them.
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Given a function f and two integers m ≥ 0 and n ≥ 0, the Padé approximant of order [m/n] is the rational function

which agrees with
to the highest possible order, which amounts to
.Equivalently, if
is expanded in a Maclaurin series (Taylor series at 0), its first m + n terms would cancel the first m + n terms of
, and as such:

The Padé approximant is unique for given m and n, that is, the coefficients
can be uniquely determined. It is for reasons of uniqueness that the zero-th order term at the denominator of
was chosen to be 1, otherwise the numerator and denominator of
would have been unique only up to multiplication by a constant.
The Padé approximant defined above is also denoted as
![[m/n]_f(x). \,](http://wpcontent.answcdn.com/wikipedia/en/math/7/a/0/7a0dc8a9d1149451ca54a7e3001eb4a2.png)
For given
, Padé approximants can be computed by Wynn's epsilon algorithm[1] and also other sequence transformations[citation needed] from the partial sums

of the Taylor series of
, i.e., we have

can also be a formal power series, and, hence, Padé approximants can also be applied to the summation of divergent series.
One way to compute a Pade approximant is via the extended euclidean algorithm for the polynomial gcd.[2] The relation

is equivalent to the existence of some factor K(x) such that
,which can be interpreted as the Bezout identity of one step in the computation of the extended gcd of the polynomials
and
.
To recapitulate: to compute the gcd of two polynomials p and q, one computes via long division the remainder sequence
,
with
, until
. For the Bezout identities of the extended gcd one computes simultaneously the two polynomial sequences

to obtain in each step the Bezout identity
.For the [m/n] approximant, one thus carries out the extended euclidean algorithm for

and stops it at the last instant that
has degree n or smaller.
Then the polynomials
give the [m/n] Pade approximant. If one were to computes all steps of the extended gcd computation, one would obtain an anti-diagonal of the Pade table.
To study the resummation of a divergent series, say

it can be useful to introduce the Padé or simply rational zeta function as

where
![R(x) = [m/n]_{f}(x),\,](http://wpcontent.answcdn.com/wikipedia/en/math/a/8/7/a870057f34b5b45fbb54c0a9775a28f9.png)
is just the Padé approximation of order (m, n) of the function f(x). The zeta regularization value at s = 0 is taken to be the sum of the divergent series.
The functional equation for this Padé zeta function is

where
and
are the coefficients in the Padé approximation. The subscript '0' means that the Padé is of order [0/0] and hence, we have the Riemann zeta function.
Padé approximants can be used to extract critical points and exponents of functions. In thermodynamics, if a function f(x) behaves in a non-analytic way near a point x = r like
, one calls x = r a critical point and p the associated critical exponent of f. If sufficient terms of the series expansion of f are known, one can approximately extract the critical points and the critical exponents from respectively the poles and residues of the Padé approximants
where
.
A Padé approximant approximates a function in one variable. An approximant in two variables is called a Chisholm approximant, in multiple variables a Canterbury approximant (after Graves-Morris at the University of Kent).
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