2009
DOI: 10.1016/j.nuclphysb.2008.08.022
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Towards all-order Laurent expansion of generalised hypergeometric functions about rational values of parameters

Abstract: Hypergeometric functions provide a useful representation of Feynman diagrams occuring in precision phenomenology. In dimensional regularization, the ε-expansion of these functions about d = 4 is required. We discuss the current status of differential reduction algorithms. As an illustration, we consider the construction of the all-order ε-expansion of the Appell hypergeometric function F 1 around integer values of the parameters and present an explicit evaluation of the first few terms.

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Cited by 42 publications
(26 citation statements)
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“…In our case, the 5 Another example of such a cancellation was presented in ref. [37]. 6 We adopt the following definition of holonomic function [29]: a function is called holonomic if it satisfies a system of linear differential equations with polynomial coefficients whose solutions form a finite-dimensional vector space.…”
Section: Jhep07(2017)031mentioning
confidence: 99%
“…In our case, the 5 Another example of such a cancellation was presented in ref. [37]. 6 We adopt the following definition of holonomic function [29]: a function is called holonomic if it satisfies a system of linear differential equations with polynomial coefficients whose solutions form a finite-dimensional vector space.…”
Section: Jhep07(2017)031mentioning
confidence: 99%
“…An asymptotic expansion of the sunset integral has been given in [15]. Various forms for the integral have been considered either in geometrical terms [16], displaying some relations to one-loop amplitude [17], or a representation in terms of hypergeometric function as given in [18,19,20,21] or as an integral of Bessel functions as in [22,23]. Or a differential equation approach (in close relation to the method used in section 5 of the present work) was considered in [24,25,26,27,28].…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, the expansion of the last function is expressible in terms of MPLs of q-th roots of unity times powers of logarithms ln(1 − z) [7]. Again, according to [7] any of the three functions (4.2) can be expressed in terms of the first one (4.1). Therefore, it is sufficient to study the ǫ-expansion of (4.1).…”
Section: Representation In Terms Of a Hypergeometric Functionmentioning
confidence: 99%
“…After introducing the new variable [1,7] with the q-th roots of unity (4.3). Then the system (4.7) can be brought into Fuchsian class…”
Section: Representation In Terms Of a Hypergeometric Functionmentioning
confidence: 99%
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