2006
DOI: 10.1007/3-540-30611-0
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Feynman Integral Calculus

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Cited by 38 publications
(23 citation statements)
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“…And because loop integration remains considerably harder than integrand construction, it is extremely convenient to reuse integrals for many different computations or reduce them to a smaller set of master integrals, see e.g. [120][121][122][123] and references therein. While we are not using integral reduction in this work, we are simplifying the work required to find integrand-level representations, after which integration-by-parts identities could be exploited.…”
Section: From Generalized To Prescriptive Unitaritymentioning
confidence: 99%
“…And because loop integration remains considerably harder than integrand construction, it is extremely convenient to reuse integrals for many different computations or reduce them to a smaller set of master integrals, see e.g. [120][121][122][123] and references therein. While we are not using integral reduction in this work, we are simplifying the work required to find integrand-level representations, after which integration-by-parts identities could be exploited.…”
Section: From Generalized To Prescriptive Unitaritymentioning
confidence: 99%
“…, α L }. Note that the β integration is not projective here (but could be projectivized using the Cheng-Wu theorem [28,29]). Rescaling these parameters,…”
Section: Feynman Parameterizationmentioning
confidence: 99%
“…Before getting started, however, we should perhaps clarify our terminology. What we will call 'Feynman parameters' are sometimes more specifically referred to as 'Schwinger parameters' or even 'α parameters' [38,39]-distinguished by how these integrals are de-projectivized. For the most part, de-projectivization is a trivial distinction; but to be clear, when we have reason to de-projectivize any integral explicitly, we will always use δ(α i − 1) instead of Feynman's choice of δ(( i α i )−1).…”
Section: Feynman Parameter Integrals In Dual Coordinatesmentioning
confidence: 99%
“…which can for example be computed directly with HyperInt 8 or by using standard algorithms for the evaluation of Mellin-Barnes integrals [38,39,45]. In this case, the fundamental strip of M{I 2mh }(z) is (µ, ν) = (0, 1) with a third order pole at z = 0.…”
Section: Analytic Extraction Of Divergent and Finite Coefficientsmentioning
confidence: 99%