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In mathematics, the '''Stieltjes transformation''' ''S''<sub>&rho;</sub>(''z'') of a measure of density &rho; on a real interval ''I'' is the function of the complex variable ''z'' defined outside ''I'' by the formula
 
:<math>S_{\rho}(z)=\int_I\frac{\rho(t)\,dt}{z-t}.</math>
 
Under certain conditions we can reconstitute the density function &rho; starting from its Stieltjes transformation thanks to the inverse formula of Stieltjes-Perron. For example, if the density &rho; is continuous throughout ''I'', one will have inside this interval
 
:<math>\rho(x)=\underset{\varepsilon\rightarrow 0^+}{\text{lim}}\frac{S_{\rho}(x-i\varepsilon)-S_{\rho}(x+i\varepsilon)}{2i\pi}.</math>
 
==Connections with moments of measures==
{{Main|moment problem}}
 
If the measure of density &rho; has [[moment (mathematics)|moments]] of any order defined for each integer by the equality
 
:<math>m_{n}=\int_I t^n\,\rho(t)\,dt,</math>
 
then the [[Stieltjes]] transformation of &rho; admits for each integer ''n'' the [[Asymptotic analysis|asymptotic]] expansion in the neighbourhood of infinity given by
 
:<math>S_{\rho}(z)=\sum_{k=0}^{k=n}\frac{m_k}{z^{k+1}}+o\left(\frac{1}{z^{n+1}}\right).</math>
 
Under certain conditions the complete expansion as a [[Laurent series]] can be obtained:
:<math>S_{\rho}(z)=\sum_{n=0}^{n=\infty}\frac{m_n}{z^{n+1}}.</math>
 
==Relationships to orthogonal polynomials==
 
The correspondence <math>(f,g)\mapsto \int_I f(t)g(t)\rho(t)\,dt</math>  defines an [[inner product]] on the space of [[continuous function]]s on the interval ''I''.
 
If  {''P<sub>n</sub>''} is a sequence of [[orthogonal polynomials]] for this product, we can create the sequence of associated [[secondary polynomials]] by the formula
 
: <math>Q_n(x)=\int_I \frac{P_n (t)-P_n (x)}{t-x}\rho (t)\,dt.</math>
 
It appears that <math>F_n(z)=\frac{Q_n(z)}{P_n(z)}</math> is a [[Padé approximation]] of ''S''<sub>&rho;</sub>(''z'') in a neighbourhood of infinity, in the sense that
 
: <math>S_\rho(z)-\frac{Q_n(z)}{P_n(z)}=O\left(\frac{1}{z^{2n}}\right).</math>
 
Since these two sequences of polynomials satisfy the same recurrence relation in three terms, we can develop a [[generalized continued fraction|continued fraction]] for the Stieltjes transformation whose successive [[Convergent (continued fraction)|convergents]] are the fractions ''F<sub>n</sub>''(''z'').
 
The Stieltjes transformation can also be used to construct from the density &rho; an effective measure for transforming the secondary polynomials into an orthogonal system. (For more details see the article [[secondary measure]].)
 
==See also==
 
* [[Orthogonal polynomials]]
* [[Secondary polynomials]]
* [[Secondary measure]]
 
==References==
*{{cite book|author = H. S. Wall|title = Analytic Theory of Continued Fractions|publisher = D. Van Nostrand Company Inc.|year = 1948}}
 
[[Category:Integral transforms]]
[[Category:Continued fractions]]

Revision as of 19:56, 10 June 2013

In mathematics, the Stieltjes transformation Sρ(z) of a measure of density ρ on a real interval I is the function of the complex variable z defined outside I by the formula

Sρ(z)=Iρ(t)dtzt.

Under certain conditions we can reconstitute the density function ρ starting from its Stieltjes transformation thanks to the inverse formula of Stieltjes-Perron. For example, if the density ρ is continuous throughout I, one will have inside this interval

ρ(x)=limε0+Sρ(xiε)Sρ(x+iε)2iπ.

Connections with moments of measures

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If the measure of density ρ has moments of any order defined for each integer by the equality

mn=Itnρ(t)dt,

then the Stieltjes transformation of ρ admits for each integer n the asymptotic expansion in the neighbourhood of infinity given by

Sρ(z)=k=0k=nmkzk+1+o(1zn+1).

Under certain conditions the complete expansion as a Laurent series can be obtained:

Sρ(z)=n=0n=mnzn+1.

Relationships to orthogonal polynomials

The correspondence (f,g)If(t)g(t)ρ(t)dt defines an inner product on the space of continuous functions on the interval I.

If {Pn} is a sequence of orthogonal polynomials for this product, we can create the sequence of associated secondary polynomials by the formula

Qn(x)=IPn(t)Pn(x)txρ(t)dt.

It appears that Fn(z)=Qn(z)Pn(z) is a Padé approximation of Sρ(z) in a neighbourhood of infinity, in the sense that

Sρ(z)Qn(z)Pn(z)=O(1z2n).

Since these two sequences of polynomials satisfy the same recurrence relation in three terms, we can develop a continued fraction for the Stieltjes transformation whose successive convergents are the fractions Fn(z).

The Stieltjes transformation can also be used to construct from the density ρ an effective measure for transforming the secondary polynomials into an orthogonal system. (For more details see the article secondary measure.)

See also

References

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