2020
DOI: 10.1016/j.nuclphysb.2020.114952
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GKZ-hypergeometric systems for Feynman integrals

Abstract: Basing on the systems of linear partial differential equations derived from Mellin-Barnes representations and Miller's transformation, we obtain GKZ-hypergeometric systems of one-loop self energy, one-loop triangle, two-loop vacuum, and two-loop sunset diagrams, respectively. The codimension of derived GKZ-hypergeometric system equals the number of independent dimensionless ratios among the external momentum squared and virtual mass squared. Taking GKZ-hypergeometric systems of one-loop self energy, massless o… Show more

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Cited by 33 publications
(20 citation statements)
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“…We warn the reader that, apart from restricting to the kinematic space or even smaller subspaces E of P |A|−1 , an important difference with A-discriminant analysis is that we discard singularities of {F G = 0} inside the locus {U G = 0}. Related recent applications of A-discriminants to holonomic systems for Feynman integrals include [53][54][55][56].…”
Section: Motivationmentioning
confidence: 99%
“…We warn the reader that, apart from restricting to the kinematic space or even smaller subspaces E of P |A|−1 , an important difference with A-discriminant analysis is that we discard singularities of {F G = 0} inside the locus {U G = 0}. Related recent applications of A-discriminants to holonomic systems for Feynman integrals include [53][54][55][56].…”
Section: Motivationmentioning
confidence: 99%
“…It is well known to all that, there are a lot of two loop diagrams [25,26] contributing to muon MDM in SUSY models. So, to identify the important two loop diagrams is a meaning- Fig.…”
Section: Introductionmentioning
confidence: 99%
“…(4.7) 30 The terminology of -vectors employed here is of course not be confused with vectors that have l components or the like, which is why have chosen a different symbol .…”
Section: Relating the Frobenius Basis Of M L−1 To The Basis Of Kähler Classes On W L−1mentioning
confidence: 99%