2015
DOI: 10.1007/jhep02(2015)120
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A quasi-finite basis for multi-loop Feynman integrals

Abstract: We present a new method for the decomposition of multi-loop Euclidean Feynman integrals into quasi-finite Feynman integrals. These are defined in shifted dimensions with higher powers of the propagators, make explicit both infrared and ultraviolet divergences, and allow for an immediate and trivial expansion in the parameter of dimensional regularization. Our approach avoids the introduction of spurious structures and thereby leaves integrals particularly accessible to direct analytical integration techniques.… Show more

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Cited by 117 publications
(144 citation statements)
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“…Therefore we have calculated all the integrals numerically using the program SecDec-3.0 [20]. We partially used a finite basis [29] for the planar master integrals, as far as it turned out to be beneficial for the numerical integration.…”
Section: Nlo Cross Sectionmentioning
confidence: 99%
“…Therefore we have calculated all the integrals numerically using the program SecDec-3.0 [20]. We partially used a finite basis [29] for the planar master integrals, as far as it turned out to be beneficial for the numerical integration.…”
Section: Nlo Cross Sectionmentioning
confidence: 99%
“…These problems can in principle be avoided with the help of IBP relations, because it is always possible to write a Feynman integral in terms of master integrals without subdivergences [68]. Unfortunately, such IBP reductions are too complicated in our case.…”
Section: Pos(ll2016)038mentioning
confidence: 99%
“…The advantage of this approach is that there is no power divergence in the integrand in 6 − 2ǫ dimension, and the integral can be straightforwardly carried out order by order in ǫ. Similar strategy has been employed in the direct calculation of soft phase space integral [12], in the calculation of multi-box diagrams [31], and in searching for quasi finite master integral basis [32]. In d = 6 − 2ǫ dimension, eq.…”
Section: Jhep02(2015)155mentioning
confidence: 99%