For several multiloop Feynman integral systems, the monodromy group has a basis where its generators are matrices over Z[z,1/z] with z = exp(iπd), obtained by a numerical recognition method.
Symmetric $\epsilon$- and $(\epsilon+1/2)$-forms and quadratic constraints in "elliptic" sectors
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abstract
Within the differential equation method for multiloop calculations, we examine the systems irreducible to $\epsilon$-form. We argue that for many cases of such systems it is possible to obtain nontrivial quadratic constraints on the coefficients of $\epsilon$-expansion of their homogeneous solutions. These constraints are the direct consequence of the existence of symmetric $(\epsilon+1/2)$-form of the homogeneous differential system, i.e., the form where the matrix in the right-hand side is symmetric and its $\epsilon$-dependence is localized in the overall factor $(\epsilon+1/2)$. The existence of such a form can be constructively checked by available methods and seems to be common to many irreducible systems, which we demonstrate on several examples. The obtained constraints provide a nontrivial insight on the structure of general solution in the case of the systems irreducible to $\epsilon$-form. For the systems reducible to $\epsilon$-form we also observe the existence of symmetric form and derive the corresponding quadratic constraints.
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Monodromy of multiloop integrals in $d$ dimensions
For several multiloop Feynman integral systems, the monodromy group has a basis where its generators are matrices over Z[z,1/z] with z = exp(iπd), obtained by a numerical recognition method.