Starting from the Mellin-Barnes integral representation of a Feynman integral depending on set of kinematic variables $z_i$, we derive a system of partial differential equations w.r.t.\ new variables $x_j$, which parameterize the differentiable constraints $z_i=y_i(x_j)$. In our algorithm, the powers of propagators can be considered as arbitrary parameters. Our algorithm can also be used for the reduction of multiple hypergeometric sums to sums of lower dimension, finding special values and reduction equations of hypergeometric functions in a singular locus of continuous variables, or finding systems of partial differential equations for master integrals with arbitrary powers of propagators. As an illustration, we produce a differential equ...
We show that all Feynman integrals in two Euclidean dimensions with massless propagators and arbitra...
It is shown how the geometrical splitting of N-point Feynman diagrams can be used to simplify the pa...
We investigate the structure of a particular class of massive vacuum Feynman integrals at two loops....
Starting from the Mellin-Barnes integral representation of a Feynman integraldepending on set of kin...
AbstractWe argue that the Mellin–Barnes representations of Feynman diagrams can be used for obtainin...
Applying the system of linear partial differential equations derived from Mellin-Barnes representati...
In this manuscript, we elaborate on a procedure to derive $\epsilon$-factorised differential equatio...
We proposed a recipe to systematically calculate Feynman integrals containing linear propagators usi...
A method of functional reduction for the dimensionally regularized one-loop Feynman integrals with m...
In the Lee-Pomeransky representation, Feynman integrals can be identified as a subset of Euler-Melli...
In recent years, differential equations have become the method of choice to compute multi-loop Feynm...
We elaborate on the method of differential equations for evaluating Feynman integrals. We focus on s...
We elaborate on the connection between Gel'fand-Kapranov-Zelevinsky systems, de Rham theory for twis...
The long-standing problem of representing the general massive one-loop Feynman integral as a meromor...
Bejdakic E. Feynman integrals, hypergeometric functions and nested sums. Bielefeld (Germany): Bielef...
We show that all Feynman integrals in two Euclidean dimensions with massless propagators and arbitra...
It is shown how the geometrical splitting of N-point Feynman diagrams can be used to simplify the pa...
We investigate the structure of a particular class of massive vacuum Feynman integrals at two loops....
Starting from the Mellin-Barnes integral representation of a Feynman integraldepending on set of kin...
AbstractWe argue that the Mellin–Barnes representations of Feynman diagrams can be used for obtainin...
Applying the system of linear partial differential equations derived from Mellin-Barnes representati...
In this manuscript, we elaborate on a procedure to derive $\epsilon$-factorised differential equatio...
We proposed a recipe to systematically calculate Feynman integrals containing linear propagators usi...
A method of functional reduction for the dimensionally regularized one-loop Feynman integrals with m...
In the Lee-Pomeransky representation, Feynman integrals can be identified as a subset of Euler-Melli...
In recent years, differential equations have become the method of choice to compute multi-loop Feynm...
We elaborate on the method of differential equations for evaluating Feynman integrals. We focus on s...
We elaborate on the connection between Gel'fand-Kapranov-Zelevinsky systems, de Rham theory for twis...
The long-standing problem of representing the general massive one-loop Feynman integral as a meromor...
Bejdakic E. Feynman integrals, hypergeometric functions and nested sums. Bielefeld (Germany): Bielef...
We show that all Feynman integrals in two Euclidean dimensions with massless propagators and arbitra...
It is shown how the geometrical splitting of N-point Feynman diagrams can be used to simplify the pa...
We investigate the structure of a particular class of massive vacuum Feynman integrals at two loops....