2017
DOI: 10.1103/physrevd.96.125013
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Vacuum seagull: Evaluating a three-loop Feynman diagram with three mass scales

Abstract: We study a 3-loop 5-propagator Feynman Integral, which we call the vacuum seagull, with arbitrary masses and spacetime dimension using the Symmetries of Feynman Integrals method. It is our first example with potential numerators. We determine the associated group G ⊂ GL(3) which happens to be 5 dimensional and the associated set of 5 differential equations. G is determined by a geometric approach which we term "current freedom". We find the generic G-orbit to be co-dimension 0 and hence the method is maximally… Show more

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Cited by 10 publications
(24 citation statements)
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“…By now, SFI was further developed and numerous diagrams have been analyzed within it [8][9][10][11][12][13][14][15]. Even though these diagrams are relatively basic, the analysis achieved new results including the value of the seagull diagram (to be discussed below) in a 3 mass scale sector and the value of the kite diagram (2-loop 2-leg) throughout its singular locus.…”
Section: Jhep01(2021)165mentioning
confidence: 99%
“…By now, SFI was further developed and numerous diagrams have been analyzed within it [8][9][10][11][12][13][14][15]. Even though these diagrams are relatively basic, the analysis achieved new results including the value of the seagull diagram (to be discussed below) in a 3 mass scale sector and the value of the kite diagram (2-loop 2-leg) throughout its singular locus.…”
Section: Jhep01(2021)165mentioning
confidence: 99%
“…[54]- [73] found a variety of important special analytical cases that have been incorporated into 3VIL.…”
Section: Conventions and Setupmentioning
confidence: 99%
“…Analytic calculation of Feynman diagrams with several mass scales is a challenge, but it is important for higher loop corrections to Standard Model/Core Theory 1 observables involving several different particles, and it is of intrinsic interest to Quantum Field Theory. The Symmetries of Feynman Integrals method (SFI) [2], see also developments in [3][4][5][6][7][8], reduces the diagram to its value at some allowed and more convenient base point in parameter space, namely the space X of masses and kinematical invariants, plus a line integral in X over simpler diagrams (with one edge contracted).…”
mentioning
confidence: 99%