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. Definition 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 f(x) to the highest possible order, which amounts to \[ \begin{array}{rcl} f(0)&=&R(0)\\ f'(0)&=&R'(0)\\ f''(0)&=&R''(0)\\ &\vdots& \\ f^{(m+n)}(0)&=&R^{(m+n)}(0)\end{array} . \] Equivalently, if R(x) is expanded in a Maclaurin series (Taylor series at 0), its first m + n terms would cancel the first m + n terms of f(x), and as such: \[ f(x)R(x) = c_{m+n+1}x^{m+n+1}+c_{m+n+2}x^{m+n+2}+\cdots \] The Padé approximant is unique for given m and n, that is, the coefficients a_0, a_1, \dots, a_m, b_1, \dots, b_n can be uniquely determined. It is for reasons of uniqueness that the zeroth order term at the denominator of R(x) was chosen to be 1, otherwise the numerator and denominator of R(x) would have been unique only up to multiplication by a constant. The Padé approximant defined above is also denoted as \[ [m/n]_f(x). \, \] For given x, Padé approximants can be computed by Wynn's epsilon algorithm and also other sequence transformations from the partial sums \[ s_n(x)=c_0 + c_1 x + c_2 x^2 + \cdots + c_n x^n \] of the Taylor series of f, i.e., we have \[ c_k = \frac{f^{(k)}(0)}{k!}. \] f can also be a formal power series, and, hence, Padé approximants can also be applied to the summation of divergent series. To study the resummation of a divergent series, say \[ \sum_{z=1}^{\infty}f(z), \] it can be useful to introduce the Padé or simply rational zeta function as \[ \zeta _{R}(s) = \sum_{z=1}^{\infty} \frac{R(z)}{z^{s}}, \] where \[ R(x) = [m/n]_{f}(x),\, \] 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 \[ \sum_{j=0}^{n}p_{j}\zeta _{R}(sj)= \sum_{j=0}^{m}q_{j}\zeta_{0}(sj), \] where p_j and q_j are the coefficients in the Padé approximation. The subscript '0' means that the Padé is of order [0/0] and hence, we got 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 nonanalytic way near a point \[ x = r like f(x)\sim \leftxr\right^{p} \], 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 \[ \left[n/n+1\right]_{g}\left(x\right) \] where \[ g=\frac{f'}{f}.\] 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 GravesMorris at the University of Kent). Padé table References Baker, G. A., Jr.; and GravesMorris, P. Padé Approximants. Cambridge U.P., 1996 External links Weisstein, Eric W., "Padé Approximant" from MathWorld. Retrieved from "http://en.wikipedia.org/"

