2020
DOI: 10.1007/jhep02(2020)079
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Integration-by-parts reductions of Feynman integrals using Singular and GPI-Space

Abstract: We introduce an algebro-geometrically motived integration-by-parts (IBP) reduction method for multi-loop and multi-scale Feynman integrals, using a framework for massively parallel computations in computer algebra. This framework combines the computer algebra system Singular with the workflow management system GPI-Space, which are being developed at the TU Kaiserslautern and the Fraunhofer Institute for Industrial Mathematics (ITWM), respectively. In our approach, the IBP relations are first trimmed by modern … Show more

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Cited by 56 publications
(58 citation statements)
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“…Relying on the module intersection IBP reduction method and its implementation in the Singular-GPI-Space framework for massively parallel computations, the analytic IBP reduction coefficients were calculated for the integrals with ISP up to the degree 4 in the sector (1, 1, 1, 1, 1, 1, 1, 1, 0, 0, 0) in ref. [33]. 2 The size of the IBP reduction coefficients with respect to a Laporta basis is 2.4GB (with all parameters analytic).…”
Section: Jhep12(2020)054mentioning
confidence: 99%
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“…Relying on the module intersection IBP reduction method and its implementation in the Singular-GPI-Space framework for massively parallel computations, the analytic IBP reduction coefficients were calculated for the integrals with ISP up to the degree 4 in the sector (1, 1, 1, 1, 1, 1, 1, 1, 0, 0, 0) in ref. [33]. 2 The size of the IBP reduction coefficients with respect to a Laporta basis is 2.4GB (with all parameters analytic).…”
Section: Jhep12(2020)054mentioning
confidence: 99%
“…They are listed in the following: As we have observed in ref. [33], if we reduce the target integrals to the UT basis, the size of coefficients is reduced to 712MB. More importantly, the IBP reduction coefficients with respect to UT basis have no "mixed" poles and all kinematic denominators are symbol letters.…”
Section: Jhep12(2020)054mentioning
confidence: 99%
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