REVIEW 3 major objections 5 minor 2 cited by
Integration-by-parts reductions of Feynman integrals using Singular and GPI-Space
T0 review · 3 major / 5 minor · reviewed 2026-08-14 · deepseek-v4-flash
Pith's one-line read This paper presents an analytic integration-by-parts reduction of the two-loop five-point nonplanar double-pentagon integrals up to numerator degree 4, obtained by trimming the IBP system with module intersections and solving it with a…
desk verdict A credible analytic IBP reduction of the nonplanar double pentagon, with real downloadable artifacts, though the completeness bound is heuristic and the pipeline is not yet a proven black box. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is the module intersection $M_1 \cap M_2$ over $R = \mathbb{Q}(c_i)[z_1,\dots,z_m]$: $M_1$ is the module of polynomial multipliers $a_i(z), b(z)$ satisfying the syzygy relation $\sum_i a_i \partial P/\partial z_i + bP = 0$ (no dimension shifts), and $M_2$ imposes $a_i = b_i z_i$ for propagator variables (no double propagators). A Grobner-basis computation of this intersection, with a user-set degree bound, generates exactly the IBP relations the subsequent linear algebra needs. The second machinery is the parallel reduction workflow: a Petri-net description in the workflow manager GPI-Space schedules many semi-numeric row reductions, detects bad interpolation points, and reconstructs rational coefficients via a reference-point cancellation algorithm that reduces rational-function interpolation to polynomial interpolation. Together these two pieces turn a problem whose naive linear system is enormous into per-cut systems of roughly 1100 to 1250 relations.
What would settle it
Set a higher degree bound (for example 6 or 7) in the module-intersection step, rerun the reduction of the same 26 target integrals, and compare every coefficient with the published degree-5 result; any difference in the $26 \times 108$ matrices would disprove the claim that degree 5 yields sufficiently many IBP relations. A second check would evaluate the analytic coefficients at a rational kinematic point and compare with a high-precision independent IBP reduction at that point.
Extended reading notes
Core claim
The central claim is that a complete analytic IBP reduction of the two-loop five-point nonplanar double pentagon family is achievable. The method computes, for each of the 11 spanning cuts, the module intersection of the syzygy module avoiding dimension shifts with the module avoiding double propagators, using a heuristic degree bound of 5 to keep the Grobner-basis computation small; finite-field checks then indicate that enough IBP relations were obtained. The small, block-triangular linear systems are reduced by a semi-numeric algorithm in which $c_4$, $c_5$, and the dimension $D$ stay symbolic while $c_2$ and $c_3$ are integer-valued, with rational-function interpolation reconstructing the final coefficients. The output is a $26 \times 108$ matrix of IBP coefficients in a Laporta basis, consistent with an independent numerical check. Converting the master-integral basis to a dlog basis yields the same reduction with coefficients whose maximal degree in $c_2$ and $c_3$ drops and whose total on-disk size falls by 76%.
Load-bearing premise
The result depends on the heuristic choice of degree bound 5 in the module-intersection computation; if higher-degree generators are needed to capture all IBP relations, the trimmed system would omit relations and could produce wrong master-integral coefficients, and the numerical cross-check for this one example does not by itself prove the bound is sufficient in general.
Editorial extensions
If this is right
- IBP systems without double propagators can be generated for every subsector, not just the top sector, making the reduction block-triangular and easier to solve; the paper states this extension and applies it to all 11 cuts.
- The same module-intersection relations can simplify reductions for integrals that do have double or multiple propagators, since the generated relations do not raise propagator exponents.
- A dlog or uniformly transcendental master-integral basis is not only convenient for differential equations; converting to it reduces IBP coefficient size on disk by 76% in this example and lowers interpolation degrees, so basis choice can be used as a practical simplification tool.
- When only dlog-basis coefficients are wanted, interpolating the converted product directly rather than the Laporta coefficients reduces the number of semi-numeric runs.
- The Petri-net parallelization of symbolic row reduction carries over to other large symbolic linear algebra problems with parameters, such as the algebraic-geometry solution of Bethe-Ansatz equations mentioned in the paper.
Reading between the lines
- One can test the heuristic degree bound systematically: for a smaller integral family where the complete module intersection is computable, compare the degree-bounded IBP system against the full one and measure how often degree 5 would be insufficient; this would turn the heuristic into a quantitative reliability curve.
- The 76% coefficient-size drop suggests a cost metric for basis selection: on-disk size and maximal parameter degrees may predict evaluation time of IBP coefficients, so one could benchmark numerical evaluation per phase-space point for Laporta versus dlog bases.
- The same trimming-by-module-intersection strategy may extend beyond massless five-point integrals to families with massive propagators or elliptic sectors, where dlog or uniform-transcendentality reduction fails; the algebraic trimming and parallel reconstruction layers are independent of uniform transcendentality.
- Since the interpolation algorithm works by heuristically matching leading exponents across semi-numeric points, adversarial rational functions with near-cancellations could require many points; a stress test on artificial IBP systems with known high-degree denominators would reveal the algorithm's failure modes.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents an automated, parallel framework for integration-by-parts (IBP) reduction of multi-loop Feynman integrals, combining the computer algebra system Singular with the workflow manager GPI-Space. The method uses algebraic geometry—specifically module intersections with a heuristic degree bound—to trim the IBP system, followed by sparse linear algebra over finite fields and semi-numeric rational-function interpolation. The central demonstration is the analytic IBP reduction of the two-loop five-point nonplanar double-pentagon integral family up to numerator degree four, covering 26 target integrals, with coefficients in both a Laporta basis and a dlog basis. The authors report a 76% reduction in the on-disk size of the coefficients after conversion to the dlog basis, and state that the result has been cross-checked numerically against FIRE6.
Significance. If the result is correct, this is a significant computational advance: it is the first analytic IBP reduction of the two-loop five-point nonplanar double pentagon with numerator degree up to four, a problem with five kinematic variables plus the spacetime dimension. The paper also demonstrates a genuinely parallel, automatized architecture that scales to hundreds of cores, and the dlog-basis conversion is practically useful for amplitude computations. Strengths include the principled use of module intersections from prior work [59], the detailed Petri-net description of the parallel algorithm, and the independent FIRE6 consistency check. However, the advertised analytic result rests on two empirical heuristics—the degree-bound completeness in Section 6.1 and the majority-vote interpolation in Appendix A—neither of which is accompanied by a proof or a sufficiently detailed validation protocol. The absence of source code or scripts also limits external reproducibility of the completeness claims.
major comments (3)
- [Section 6.1] The completeness of the trimmed IBP system is asserted through an empirical degree bound. The text states: 'choosing the degree bound 5 ... Later on, by finite-field methods, we find that with this choice of degree bound, we obtain sufficiently many IBPs for our problem.' This verifies sufficiency only at the specific finite-field kinematics used in the trimming step. The module intersection M1∩M2 could contain independent generators of degree greater than 5 that are needed only at generic kinematic points; if so, the cut systems in Table 2 would be rank-deficient and the coefficients of the 26 target integrals in Section 6.2 would be incorrect. The FIRE6 consistency check in Section 6.2 ('By setting all Mandelstam variables to integers') is not described with enough detail to certify the analytic result: finitely many integer-kinematics checks cannot exclude rational functions that agree at the tested points but differ elsewhere. I therefore ask for either a proof of the degree-bound completeness, for example a Gröbner basis certificate, or a much more extensive and documented finite-field verification at many random generic points, with the number of points and prime fields stated.
- [Appendix A] The rational function interpolation relies on a majority-vote heuristic. Step 2 drops all semi-numeric results whose leading exponent in x_{k+1},...,x_k is not the most frequent value r, on the claim that this 'ensures that the gcd ... is just an integer.' This is not a proof: cancellations after substituting integer values for x_1,...,x_{k1} can occur for a subset of points, and the leading-exponent majority vote does not guarantee that every retained point has the same polynomial common-factor structure. The normalization formulas (A.12)–(A.14) then need not yield the true F/G. Since the final Laporta and dlog coefficients are produced by this interpolation, a failure here would invalidate the central result. Please provide a rigorous correctness statement with explicit genericity assumptions, or replace the heuristic by a provably correct reconstruction algorithm with verification steps.
- [Section 6.2 / Table 2] The interpolation degree bounds d2 and d3 are determined from univariate reductions in which one parameter is symbolic and all others are numeric. The text states that this 'easily' determines the maximal degree. For a multivariate rational function, the degree in c2 at a single generic point can be smaller than the maximal degree over the full kinematic domain, so the number of interpolation points (d2+1)(d3+1), as used after Eq. (2.11), is not guaranteed to be sufficient. The manuscript does not report how many univariate substitutions were used, whether they were varied, or whether the resulting multivariate interpolation was independently verified beyond the single integer-kinematics FIRE6 check. Please either prove the degree bounds from the algebraic structure of the reduction or document a validation strategy that checks the interpolated coefficients at additional random points.
minor comments (5)
- [Abstract] The abstract contains a typo: 'algebro-geometrically motived' should be 'algebro-geometrically motivated'.
- [Section 6, first paragraph] The list of independent Mandelstam variables repeats s45: 's12, s23, s34, s45, s45, s15' should be a list of five distinct variables, presumably omitting one duplicate.
- [Section 4.4 / Table 1] The row for one core reports a 'relative speedup' of 1.201 and an efficiency of 1.201, which is confusing because the text explains that the single-core timing is special and the 15-core run is used as the reference; please clarify this in the table caption or add a footnote.
- [Section 2.1] The notation 'κ' is introduced without an explicit definition in the sentence 'Suppose we wish to reduce an integral family with nj ≤ 0, j = κ+1,...,m'; defining κ as the number of propagators with positive index would improve readability.
- [Figure 8] The spelling 'non-planar' appears with a hyphen in the caption but as 'nonplanar' elsewhere in the paper; please unify the spelling.
Circularity Check
No significant circularity: the IBP reduction is computed from the syzygy/module-intersection system and checked against FIRE6; self-citations are tool citations, not load-bearing.
full rationale
The paper's derivation chain is self-contained: IBP relations are generated from the syzygy equations (2.6)-(2.7), the simultaneous solutions are computed as the module intersection M1∩M2, and the resulting linear system is reduced by row-reduction and rational-function interpolation. No fitted parameter is reused as a prediction: the degree bounds d2 and d3 are obtained from univariate reductions and used only to fix the number of interpolation points, and the sufficiency of the degree-bound-5 module intersection is tested over finite fields and cross-checked against FIRE6 at integer kinematics. The dlog basis is imported from prior work [77] by overlapping authors, and the module-intersection method from [59], but these are computational tools and input bases, not the claimed output; the claimed output (analytic reduction coefficients for the 26 double-pentagon integrals) is computed, not assumed. The degree-bound heuristic in Section 6.1 is a completeness risk rather than a circularity, and the FIRE6 check provides external mitigation. Score 1 reflects minor self-citations that are not load-bearing.
Assumptions & free parameters
free parameters (2)
- module intersection degree bound (degbound) =
5
- interpolation degree bounds d2 and d3 =
per cut, d2 up to 35 and d3 up to 30; dlog basis d2'=20, d3'=20
assumptions (4)
- standard math Gröbner basis computation of M1 intersect M2 gives the full module intersection.
- domain assumption Baikov representation and IBP identities as total derivatives with no surface terms.
- domain assumption IBPs without double propagators generated from (2.6) and (2.7) are sufficient to reduce the 26 target integrals.
- ad hoc to paper Rational function reconstruction from a reference point plus majority-vote degree selection.
Cite this review
Pith. "Pith review of Integration-by-parts reductions of Feynman integrals using Singular and GPI-Space." pith.science (2026). https://pith.science/paper/MVL2ZEI2
@misc{pith2026190804301,
author = {Pith},
title = {Pith review of: Integration-by-parts reductions of Feynman integrals using Singular and GPI-Space},
year = {2026},
howpublished = {\url{https://pith.science/paper/MVL2ZEI2}},
note = {Machine review of arXiv:1908.04301}
}
read the original 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 is being developed at the Fraunhofer Institute for Industrial Mathematics (ITWM). In our approach, the IBP relations are first trimmed by modern algebraic geometry tools and then solved by sparse linear algebra and our new interpolation methods. These steps are efficiently automatized and automatically parallelized by modeling the algorithm in GPI-Space using the language of Petri-nets. We demonstrate the potential of our method at the nontrivial example of reducing two-loop five-point nonplanar double-pentagon integrals. We also use GPI-Space to convert the basis of IBP reductions, and discuss the possible simplification of IBP coefficients in a uniformly transcendental basis.
Forward citations
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Reference graph
Works this paper leans on
- [59]
- [1]
-
[2]
T. Gehrmann, J. M. Henn, and N. A. Lo Presti, Analytic form of the two-loop planar five-gluon all-plus-helicity amplitude in QCD , Phys. Rev. Lett. 116 (2016), no. 6 062001, [arXiv:1511.05409]. [Erratum: Phys. Rev. Lett.116,no.18,189903(2016)]
arXiv 2016
- [3]
- [4]
- [5]
- [6]
-
[7]
R. H. Boels, Q. Jin, and H. Luo, Efficient integrand reduction for particles with spin , arXiv:1802.06761
Show all 82 references
-
[8]
Gehrmann, J
T. Gehrmann, J. M. Henn, and N. A. Lo Presti, Pentagon functions for massless planar scattering amplitudes, JHEP 10 (2018) 103, [ arXiv:1807.09812]
2018 arXiv
-
[9]
Badger, C
S. Badger, C. Brnnum-Hansen, H. B. Hartanto, and T. Peraro, Analytic helicity amplitudes for two-loop five-gluon scattering: the single-minus case , JHEP 01 (2019) 186, [arXiv:1811.11699]
2019 arXiv
-
[10]
Abreu, J
S. Abreu, J. Dormans, F. Febres Cordero, H. Ita, and B. Page, Analytic Form of Planar Two-Loop Five-Gluon Scattering Amplitudes in QCD , Phys. Rev. Lett. 122 (2019), no. 8 082002, [arXiv:1812.04586]
2019 arXiv
-
[11]
Chicherin, T
D. Chicherin, T. Gehrmann, J. M. Henn, P. Wasser, Y. Zhang, and S. Zoia, Analytic result for a two-loop five-particle amplitude , Phys. Rev. Lett. 122 (2019), no. 12 121602, [arXiv:1812.11057]
2019 arXiv
-
[12]
Chicherin, T
D. Chicherin, T. Gehrmann, J. M. Henn, P. Wasser, Y. Zhang, and S. Zoia, The two-loop five-particle amplitude in N = 8 supergravity, JHEP 03 (2019) 115, [ arXiv:1901.05932]
2019 arXiv
-
[13]
Abreu, L
S. Abreu, L. J. Dixon, E. Herrmann, B. Page, and M. Zeng, The two-loop five-point amplitude inN = 8 supergravity, JHEP 03 (2019) 123, [ arXiv:1901.08563]
2019 arXiv
-
[14]
Abreu, J
S. Abreu, J. Dormans, F. Febres Cordero, H. Ita, B. Page, and V. Sotnikov, Analytic Form of the Planar Two-Loop Five-Parton Scattering Amplitudes in QCD , JHEP 05 (2019) 084, [arXiv:1904.00945]
2019 arXiv
-
[15]
H. B. Hartanto, S. Badger, C. Brnnum-Hansen, and T. Peraro, A numerical evaluation of planar two-loop helicity amplitudes for a W-boson plus four partons , arXiv:1906.11862
1906 arXiv
-
[16]
Zhang, Integrand-Level Reduction of Loop Amplitudes by Computational Algebraic Geometry Methods, JHEP 09 (2012) 042, [ arXiv:1205.5707]
Y. Zhang, Integrand-Level Reduction of Loop Amplitudes by Computational Algebraic Geometry Methods, JHEP 09 (2012) 042, [ arXiv:1205.5707]. – 28 –
2012 arXiv
-
[17]
Mastrolia, E
P. Mastrolia, E. Mirabella, G. Ossola, and T. Peraro, Scattering Amplitudes from Multivariate Polynomial Division , Phys. Lett. B718 (2012) 173–177, [ arXiv:1205.7087]
2012 arXiv
-
[18]
J. M. Henn, Multiloop integrals in dimensional regularization made simple , Phys. Rev. Lett. 110 (2013) 251601, [ arXiv:1304.1806]
2013 arXiv
-
[19]
J. M. Henn, Lectures on differential equations for Feynman integrals , J. Phys. A48 (2015) 153001, [arXiv:1412.2296]
2015 arXiv
-
[20]
Ita, Two-loop Integrand Decomposition into Master Integrals and Surface Terms , Phys
H. Ita, Two-loop Integrand Decomposition into Master Integrals and Surface Terms , Phys. Rev. D94 (2016), no. 11 116015, [ arXiv:1510.05626]
2016 arXiv
-
[21]
Abreu, F
S. Abreu, F. Febres Cordero, H. Ita, M. Jaquier, B. Page, and M. Zeng, Two-Loop Four-Gluon Amplitudes from Numerical Unitarity , Phys. Rev. Lett. 119 (2017), no. 14 142001, [arXiv:1703.05273]
2017 arXiv
-
[22]
L. J. Dixon, J. M. Drummond, and J. M. Henn, Bootstrapping the three-loop hexagon, JHEP 11 (2011) 023, [ arXiv:1108.4461]
2011 arXiv
-
[23]
L. J. Dixon, J. M. Drummond, M. von Hippel, and J. Pennington, Hexagon functions and the three-loop remainder function, JHEP 12 (2013) 049, [ arXiv:1308.2276]
2013 arXiv
-
[24]
L. J. Dixon and M. von Hippel, Bootstrapping an NMHV amplitude through three loops , JHEP 10 (2014) 065, [ arXiv:1408.1505]
2014 arXiv
-
[25]
Caron-Huot, L
S. Caron-Huot, L. J. Dixon, A. McLeod, and M. von Hippel, Bootstrapping a Five-Loop Amplitude Using Steinmann Relations , Phys. Rev. Lett. 117 (2016), no. 24 241601, [arXiv:1609.00669]
2016 arXiv
-
[26]
L. J. Dixon, M. von Hippel, and A. J. McLeod, The four-loop six-gluon NMHV ratio function, JHEP 01 (2016) 053, [ arXiv:1509.08127]
2016 arXiv
-
[27]
L. J. Dixon, J. Drummond, T. Harrington, A. J. McLeod, G. Papathanasiou, and M. Spradlin, Heptagons from the Steinmann Cluster Bootstrap , JHEP 02 (2017) 137, [arXiv:1612.08976]
2017 arXiv
-
[28]
Chicherin, J
D. Chicherin, J. Henn, and V. Mitev, Bootstrapping pentagon functions, JHEP 05 (2018) 164, [arXiv:1712.09610]
2018 arXiv
-
[29]
Caron-Huot, L
S. Caron-Huot, L. J. Dixon, F. Dulat, M. von Hippel, A. J. McLeod, and G. Papathanasiou, Six-Gluon Amplitudes in Planar N = 4 Super-Yang-Mills Theory at Six and Seven Loops , arXiv:1903.10890
1903 arXiv
-
[30]
von Manteuffel and R
A. von Manteuffel and R. M. Schabinger, A novel approach to integration by parts reduction , Phys. Lett. B744 (2015) 101–104, [ arXiv:1406.4513]
2015 arXiv
-
[31]
Peraro, Scattering amplitudes over finite fields and multivariate functional reconstruction , JHEP 12 (2016) 030, [ arXiv:1608.01902]
T. Peraro, Scattering amplitudes over finite fields and multivariate functional reconstruction , JHEP 12 (2016) 030, [ arXiv:1608.01902]
2016 arXiv
-
[32]
Klappert and F
J. Klappert and F. Lange, Reconstructing Rational Functions with FireFly, arXiv:1904.00009
1904 arXiv
-
[33]
Peraro, FiniteFlow: multivariate functional reconstruction using finite fields and dataflow graphs, JHEP 07 (2019) 031, [ arXiv:1905.08019]
T. Peraro, FiniteFlow: multivariate functional reconstruction using finite fields and dataflow graphs, JHEP 07 (2019) 031, [ arXiv:1905.08019]
2019 arXiv
-
[34]
Chetyrkin and F
K. Chetyrkin and F. Tkachov, Integration by parts: The algorithm to calculate -functions in 4 loops, Nuclear Physics B 192 (1981), no. 1 159 – 204
1981
-
[35]
Laporta, High precision calculation of multiloop Feynman integrals by difference equations , – 29 – Int
S. Laporta, High precision calculation of multiloop Feynman integrals by difference equations , – 29 – Int. J. Mod. Phys. A15 (2000) 5087–5159, [ hep-ph/0102033]
2000 arXiv
-
[36]
A. V. Smirnov, Algorithm FIRE – Feynman Integral REduction , JHEP 10 (2008) 107, [arXiv:0807.3243]
2008 arXiv
-
[37]
A. V. Smirnov, FIRE5: a C++ implementation of Feynman Integral REduction , Comput. Phys. Commun. 189 (2015) 182–191, [ arXiv:1408.2372]
2015 arXiv
-
[38]
A. V. Smirnov and F. S. Chuharev, FIRE6: Feynman Integral REduction with Modular Arithmetic, arXiv:1901.07808
1901 arXiv
-
[39]
Maierhoefer, J
P. Maierhoefer, J. Usovitsch, and P. Uwer, Kira - A Feynman Integral Reduction Program , Comput. Phys. Commun. 230 (2018) 99–112, [ arXiv:1705.05610]
2018 arXiv
- [40]
-
[41]
von Manteuffel and C
A. von Manteuffel and C. Studerus, Reduze 2 - Distributed Feynman Integral Reduction , arXiv:1201.4330
-
[42]
Gluza, K
J. Gluza, K. Kajda, and D. A. Kosower, Towards a Basis for Planar Two-Loop Integrals , Phys.Rev. D83 (2011) 045012, [ arXiv:1009.0472]
2011 arXiv
-
[43]
R. M. Schabinger, A New Algorithm For The Generation Of Unitarity-Compatible Integration By Parts Relations , JHEP 01 (2012) 077, [ arXiv:1111.4220]
2012 arXiv
-
[44]
K. J. Larsen and Y. Zhang, Integration-by-parts reductions from unitarity cuts and algebraic geometry, Phys. Rev. D93 (2016), no. 4 041701, [ arXiv:1511.01071]
2016 arXiv
-
[45]
Z. Bern, M. Enciso, H. Ita, and M. Zeng, Dual Conformal Symmetry, Integration-by-Parts Reduction, Differential Equations and the Nonplanar Sector , Phys. Rev. D96 (2017), no. 9 096017, [arXiv:1709.06055]
2017 arXiv
-
[46]
R. N. Lee and A. A. Pomeransky, Critical points and number of master integrals , JHEP 11 (2013) 165, [ arXiv:1308.6676]
2013 arXiv
-
[47]
Georgoudis, K
A. Georgoudis, K. J. Larsen, and Y. Zhang, Azurite: An algebraic geometry based package for finding bases of loop integrals , Comput. Phys. Commun. 221 (2017) 203–215, [arXiv:1612.04252]
2017 arXiv
-
[48]
Bitoun, C
T. Bitoun, C. Bogner, R. P. Klausen, and E. Panzer, Feynman integral relations from parametric annihilators, arXiv:1712.09215
-
[49]
H. A. Chawdhry, M. A. Lim, and A. Mitov, Two-loop five-point massless QCD amplitudes within the IBP approach , arXiv:1805.09182
-
[50]
Badger, D
S. Badger, D. Chicherin, T. Gehrmann, G. Heinrich, J. M. Henn, T. Peraro, P. Wasser, Y. Zhang, and S. Zoia, Analytic form of the full two-loop five-gluon all-plus helicity amplitude, Phys. Rev. Lett. 123 (2019), no. 7 071601, [ arXiv:1905.03733]
2019 arXiv
-
[51]
D. A. Kosower, Direct Solution of Integration-by-Parts Systems , Phys. Rev. D98 (2018), no. 2 025008, [ arXiv:1804.00131]
2018 arXiv
-
[52]
Mastrolia and S
P. Mastrolia and S. Mizera, Feynman Integrals and Intersection Theory , JHEP 02 (2019) 139, [arXiv:1810.03818]
2019 arXiv
-
[53]
Frellesvig, F
H. Frellesvig, F. Gasparotto, S. Laporta, M. K. Mandal, P. Mastrolia, L. Mattiazzi, and S. Mizera, Decomposition of Feynman Integrals on the Maximal Cut by Intersection Numbers, JHEP 05 (2019) 153, [ arXiv:1901.11510]
2019 arXiv
-
[54]
Frellesvig, F
H. Frellesvig, F. Gasparotto, M. K. Mandal, P. Mastrolia, L. Mattiazzi, and S. Mizera, Vector – 30 – Space of Feynman Integrals and Multivariate Intersection Numbers , arXiv:1907.02000
1907 arXiv
-
[55]
Liu and Y.-Q
X. Liu and Y.-Q. Ma, Determining arbitrary Feynman integrals by vacuum integrals , Phys. Rev. D99 (2019), no. 7 071501, [ arXiv:1801.10523]
2019 arXiv
-
[56]
Liu, Y.-Q
X. Liu, Y.-Q. Ma, and C.-Y. Wang, A Systematic and Efficient Method to Compute Multi-loop Master Integrals, Phys. Lett. B779 (2018) 353–357, [ arXiv:1711.09572]
2018 arXiv
-
[57]
Y. Wang, Z. Li, and N. Ul Basat, Direct Reduction of Amplitude, arXiv:1901.09390
1901 arXiv
-
[58]
Kardos, A new reduction strategy for special negative sectors of planar two-loop integrals without Laporta algorithm, arXiv:1812.05622
A. Kardos, A new reduction strategy for special negative sectors of planar two-loop integrals without Laporta algorithm, arXiv:1812.05622
-
[60]
B¨ ohm, A
J. B¨ ohm, A. Georgoudis, K. J. Larsen, M. Schulze, and Y. Zhang, Complete sets of logarithmic vector fields for integration-by-parts identities of Feynman integrals , Phys. Rev. D98 (2018), no. 2 025023, [ arXiv:1712.09737]
2018 arXiv
-
[61]
Singular 4-1-1 — A computer algebra system for polynomial computations
W. Decker, G.-M. Greuel, G. Pfister, and H. Sch¨ onemann, “Singular 4-1-1 — A computer algebra system for polynomial computations.” http://www.singular.uni-kl.de, 2018
2018
-
[62]
Pfreundt and M
F.-J. Pfreundt and M. Rahn, GPI-Space, 2018. Fraunhofer ITWM Kaiserslautern, http://www.gpi-space.de/
2018
-
[63]
Wasser, Analytic properties of Feynman integrals for scattering amplitudes , M.Sc
P. Wasser, Analytic properties of Feynman integrals for scattering amplitudes , M.Sc. (2016) [https://publications.ub.uni-mainz.de/theses/frontdoor.php?source opus=100001967]
2016
-
[64]
P. A. Baikov, Explicit solutions of the three loop vacuum integral recurrence relations , Phys. Lett. B385 (1996) 404–410, [ hep-ph/9603267]
1996 arXiv
-
[65]
R. N. Lee, Modern techniques of multiloop calculations , in Proceedings, 49th Rencontres de Moriond on QCD and High Energy Interactions: La Thuile, Italy, March 22-29, 2014 , pp. 297–300, 2014. arXiv:1405.5616
2014 arXiv
-
[66]
Zhang, Lecture Notes on Multi-loop Integral Reduction and Applied Algebraic Geometry ,
Y. Zhang, Lecture Notes on Multi-loop Integral Reduction and Applied Algebraic Geometry ,
-
[67]
http://github.com/cbouilla/spasm
The SpaSM group, SpaSM: a Sparse direct Solver Modulo p, v1.2 ed., 2017. http://github.com/cbouilla/spasm
2017
-
[68]
E. W. Mayr and A. R. Meyer, The complexity of the word problems for commutative semigroups and polynomial ideals , Advances in Mathematics 46 (1982), no. 3 305 – 329
1982
-
[69]
B¨ ohm, W
J. B¨ ohm, W. Decker, A. Fr¨ ubis-Kr¨ uger, F.-J. Pfreundt, M. Rahn, and L. Ristau,Towards massively parallel computations in algebraic geometry , arXiv:1808.09727
-
[70]
Jordan, M
C. Jordan, M. Joswig, and L. Kastner, Parallel enumeration of triangulations , Electron. J. Combin. 25 (2018), no. 3 Paper 3.6, 27
2018
-
[71]
Ristau, Using Petri nets to parallelize algebraic algorithms , 2019
L. Ristau, Using Petri nets to parallelize algebraic algorithms , 2019. Ph.D. Thesis
2019
-
[72]
Reinbold, Computation of the GIT-fan using a massively parallel implementation , 2018
C. Reinbold, Computation of the GIT-fan using a massively parallel implementation , 2018. Master’s Thesis
2018
-
[73]
Bendle, Massively parallel computation of tropical varieties , 2018
D. Bendle, Massively parallel computation of tropical varieties , 2018. Bachelor’s Thesis
2018
-
[74]
Z. Bern, E. Herrmann, S. Litsey, J. Stankowicz, and J. Trnka, Logarithmic Singularities and – 31 – Maximally Supersymmetric Amplitudes , JHEP 06 (2015) 202, [ arXiv:1412.8584]
2015 arXiv
-
[75]
Arkani-Hamed, J
N. Arkani-Hamed, J. L. Bourjaily, F. Cachazo, and J. Trnka, Local Integrals for Planar Scattering Amplitudes, JHEP 06 (2012) 125, [ arXiv:1012.6032]
2012 arXiv
-
[76]
Chicherin, T
D. Chicherin, T. Gehrmann, J. M. Henn, N. A. Lo Presti, V. Mitev, and P. Wasser, Analytic result for the nonplanar hexa-box integrals , JHEP 03 (2019) 042, [ arXiv:1809.06240]
2019 arXiv
-
[77]
Chicherin, T
D. Chicherin, T. Gehrmann, J. M. Henn, P. Wasser, Y. Zhang, and S. Zoia, All master integrals for three-jet production at NNLO , Phys. Rev. Lett. 123 (2019), no. 4 041603, [arXiv:1812.11160]
2019 arXiv
-
[78]
Lykke Jacobsen, Y
J. Lykke Jacobsen, Y. Jiang, and Y. Zhang, Torus partition function of the six-vertex model from algebraic geometry, JHEP 03 (2019) 152, [ arXiv:1812.00447]
2019 arXiv
-
[79]
Jiang and Y
Y. Jiang and Y. Zhang, Algebraic geometry and Bethe ansatz. Part I. The quotient ring for BAE, JHEP 03 (2018) 087, [ arXiv:1710.04693]
2018 arXiv
-
[80]
Zippel, Probabilistic algorithms for sparse polynomials , vol
R. Zippel, Probabilistic algorithms for sparse polynomials , vol. 72, pp. 216–226, 01, 1979
1979
-
[81]
Ben Or and P
M. Ben Or and P. Tiwari, A deterministic algorithm for sparse multivariate polynomial interpolation, Proceedings of the 20th Annual STOC (01, 1988)
1988
-
[82]
Kaltofen, W.-s
E. Kaltofen, W.-s. Lee, and A. Lobo, Early Termination in Ben-Or/Tiwari Sparse Interpolation and a Hybrid of Zippel’s Algorithm* , Proceedings of the International Symposium on Symbolic and Algebraic Computation, ISSAC (05, 2001). – 32 –
2001
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