2004
DOI: 10.1140/epjc/s2004-01974-2
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Laurent series expansion of sunrise-type diagrams using configuration space techniques

Abstract: We show that configuration space techniques can be used to efficiently calculate the complete Laurent series ε-expansion of sunrise-type diagrams to any loop order in D-dimensional spacetime for any external momentum and for arbitrary mass configurations. For negative powers of ε the results are obtained in analytical form. For positive powers of ε including the finite ε 0 contribution the result is obtained numerically in terms of low-dimensional integrals. We present general features of the calculation and p… Show more

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Cited by 13 publications
(14 citation statements)
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“…For n = 3, however, the numerator factorintegral is no longer reducible [137]. The problem of irreducible numerator factors has a straightforward solution in configuration space by the integration-by-parts technique [141]. The starting expression involving the non-trivial numerator factor (k 1 · k 2 ) (or any other scalar product of linear independent inner moments) corresponds toΠ *…”
Section: Irreducible Numerator: Three-loop Vacuum Bubble Casementioning
confidence: 99%
“…For n = 3, however, the numerator factorintegral is no longer reducible [137]. The problem of irreducible numerator factors has a straightforward solution in configuration space by the integration-by-parts technique [141]. The starting expression involving the non-trivial numerator factor (k 1 · k 2 ) (or any other scalar product of linear independent inner moments) corresponds toΠ *…”
Section: Irreducible Numerator: Three-loop Vacuum Bubble Casementioning
confidence: 99%
“…The goal of this paper is to study the first SFI examples of Feynman integrals with numerators and correspondingly to extend the SFI equation system and to study some of its solutions. For some of the other works on the topic of Feynman diagrams with numerators, see [16][17][18][19][20][21][22][23][24].…”
Section: Jhep01(2021)165mentioning
confidence: 99%
“…For a complete discussion of basketball integrals in dimensional regularization, see ref. [37]. -0.00031675 -0.00036476 -0.00032547 -0.00014179 1.063 * φ 21 0.0075590 0.0023970 -0.0033645 0.00069377 - * φ 22 -0.0025197 -0.00079883 0.0011212 -0.00023111 - * φ 31 0.0036091 0.0031005 -0.00069559 -0.00088573 - * φ 32 -0.0012030 -0.0026312 0.0043532 -0.0011224 - * φ 33 0.0 0.00053248 -0.0013736 0.00047246 - Table 3: The fit coefficients allowing to estimate the functions φ ij ,φ ij in the range 0.0 ≤ am 3 ≤ 1.0, according to Eq.…”
Section: Appendix C the 3-loop Basketball In Lattice Regularizationmentioning
confidence: 99%