Humbert Series
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In mathematics, Humbert series are a set of seven hypergeometric series Φ1, Φ2, Φ3, Ψ1, Ψ2, Ξ1, Ξ2 of two
variable Variable may refer to: * Variable (computer science), a symbolic name associated with a value and whose associated value may be changed * Variable (mathematics), a symbol that represents a quantity in a mathematical expression, as used in many ...
s that generalize Kummer's confluent hypergeometric series 1''F''1 of one variable and the
confluent hypergeometric limit function In mathematics, a generalized hypergeometric series is a power series in which the ratio of successive coefficients indexed by ''n'' is a rational function of ''n''. The series, if convergent, defines a generalized hypergeometric function, which ...
0''F''1 of one variable. The first of these double series was introduced by .


Definitions

The Humbert series Φ1 is defined for , ''x'', < 1 by the double series: : \Phi_1(a,b,c;x,y) = F_1(a,b,-,c;x,y) = \sum_^\infty \frac \,x^m y^n ~, where the Pochhammer symbol (''q'')''n'' represents the rising factorial: :(q)_n = q\,(q+1) \cdots (q+n-1) = \frac~, where the second equality is true for all complex q except q=0,-1,-2,\ldots. For other values of ''x'' the function Φ1 can be defined by analytic continuation. The Humbert series Φ1 can also be written as a one-dimensional
Euler Leonhard Euler ( , ; 15 April 170718 September 1783) was a Swiss mathematician, physicist, astronomer, geographer, logician and engineer who founded the studies of graph theory and topology and made pioneering and influential discoveries in ma ...
-type integral: : \Phi_1(a,b,c;x,y) = \frac \int_0^1 t^ (1-t)^ (1-xt)^ e^ \,\mathrmt, \quad \real \,c > \real \,a > 0 ~. This representation can be verified by means of Taylor expansion of the integrand, followed by termwise integration. Similarly, the function Φ2 is defined for all ''x'', ''y'' by the series: : \Phi_2(b_1,b_2,c;x,y) = F_1(-,b_1,b_2,c;x,y) = \sum_^\infty \frac \,x^m y^n ~, the function Φ3 for all ''x'', ''y'' by the series: : \Phi_3(b,c;x,y) = \Phi_2(b,-,c;x,y) = F_1(-,b,-,c;x,y) = \sum_^\infty \frac \,x^m y^n ~, the function Ψ1 for , ''x'', < 1 by the series: : \Psi_1(a,b,c_1,c_2;x,y) = F_2(a,b,-,c_1,c_2;x,y) = \sum_^\infty \frac \,x^m y^n ~, the function Ψ2 for all ''x'', ''y'' by the series: : \Psi_2(a,c_1,c_2;x,y) = \Psi_1(a,-,c_1,c_2;x,y) = F_2(a,-,-,c_1,c_2;x,y) = F_4(a,-,c_1,c_2;x,y) = \sum_^\infty \frac \,x^m y^n ~, the function Ξ1 for , ''x'', < 1 by the series: : \Xi_1(a_1,a_2,b,c;x,y) = F_3(a_1,a_2,b,-,c;x,y) = \sum_^\infty \frac \,x^m y^n ~, and the function Ξ2 for , ''x'', < 1 by the series: : \Xi_2(a,b,c;x,y) = \Xi_1(a,-,b,c;x,y) = F_3(a,-,b,-,c;x,y) = \sum_^\infty \frac \,x^m y^n ~.


Related series

* :There are four related series of two variables, ''F''1, ''F''2, ''F''3, and ''F''4, which generalize Gauss's hypergeometric series 2''F''1 of one variable in a similar manner and which were introduced by
Paul Émile Appell :''M. P. Appell is the same person: it stands for Monsieur Paul Appell''. Paul Émile Appell (27 September 1855, in Strasbourg – 24 October 1930, in Paris) was a French mathematician and Rector of the University of Paris. Appell polynomials and ...
in 1880.


References

* (see p. 126) * (see p. 225) * * {{DEFAULTSORT:Humbert Series Hypergeometric functions Mathematical series