2023
DOI: 10.1007/jhep04(2023)117
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Bananas of equal mass: any loop, any order in the dimensional regularisation parameter

Abstract: We describe a systematic approach to cast the differential equation for the l-loop equal mass banana integral into an ε-factorised form. With the known boundary value at a specific point we obtain systematically the term of order j in the expansion in the dimensional regularisation parameter ε for any loop l. The approach is based on properties of Calabi-Yau operators, and in particular on self-duality.

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Cited by 21 publications
(8 citation statements)
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“…[26][27][28][29][30][31][32][33][34][35][36][37][38], one must in general consider integrals that are not themselves Feynman integrals. An example of such a choice that appeared after our initial preprint leverages the notion of Calabi-Yau operators to further decompose the equalmass sunrise and ice cream cone integrals [83][84][85]. It would be interesting to see if these notions can be generalized to the generic-mass case and to other multivariate problems more generally.…”
Section: Discussionmentioning
confidence: 99%
“…[26][27][28][29][30][31][32][33][34][35][36][37][38], one must in general consider integrals that are not themselves Feynman integrals. An example of such a choice that appeared after our initial preprint leverages the notion of Calabi-Yau operators to further decompose the equalmass sunrise and ice cream cone integrals [83][84][85]. It would be interesting to see if these notions can be generalized to the generic-mass case and to other multivariate problems more generally.…”
Section: Discussionmentioning
confidence: 99%
“…Although 𝐿 (0) 3 (𝑦) is not a Calabi-Yau operator, see [12,13] in the context of Feynman integrals, we can nevertheless construct special normal forms [30] from 𝜓 0 , 𝜓 1 and 𝜓 2 , from which we define a "𝑌 "-invariant:…”
Section: Pos(radcor2023)017mentioning
confidence: 99%
“…The relation between 𝑦 and 𝑞 in (12) only holds in a vicinity of 𝑦 = 0. In the context of elliptic curves, one can analytically continue the above to a bijection relation valid for the whole kinematic regime, i.e., given a kinematic value 𝑦 ∈ R + 𝑖0 (with Feynman 𝑖0 prescription), we can obtain the same value from the following sequence:…”
Section: Analytic Continuationmentioning
confidence: 99%
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