181 research outputs found

    Numerical Implementation of Harmonic Polylogarithms to Weight w = 8

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    We present the FORTRAN-code HPOLY.f for the numerical calculation of harmonic polylogarithms up to w = 8 at an absolute accuracy of ∼4.9⋅10−15\sim 4.9 \cdot 10^{-15} or better. Using algebraic and argument relations the numerical representation can be limited to the range x∈[0,2−1]x \in [0, \sqrt{2}-1]. We provide replacement files to map all harmonic polylogarithms to a basis and the usual range of arguments x∈]−∞,+∞[x \in ]-\infty,+\infty[ to the above interval analytically. We also briefly comment on a numerical implementation of real valued cyclotomic harmonic polylogarithms.Comment: 19 pages LATEX, 3 Figures, ancillary dat

    Subleading Logarithmic QED Initial State Corrections to e+e−→γ∗/Z0∗e^+e^- \rightarrow \gamma^*/{Z^{0}}^* to O(α6L5)O(\alpha^6 L^5)

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    Using the method of massive operator matrix elements, we calculate the subleading QED initial state radiative corrections to the process e+e−→γ∗/Z∗e^+e^- \rightarrow \gamma^*/Z^* for the first three logarithmic contributions from O(α3L3),O(α3L2),O(α3L)O(\alpha^3 L^3), O(\alpha^3 L^2), O(\alpha^3 L) to O(α5L5),O(α5L4),O(α5L3)O(\alpha^5 L^5), O(\alpha^5 L^4), O(\alpha^5 L^3) and compare their effects to the leading contribution O(α6L6)O(\alpha^6 L^6) and one more subleading term O(α6L5)O(\alpha^6 L^5). The calculation is performed in the limit of large center of mass energies squared s≫me2s \gg m_e^2. These terms supplement the known corrections to O(α2)O(\alpha^2), which were completed recently. Given the high precision at future colliders operating at very large luminosity, these corrections are important for concise theoretical predictions. The present calculation needs the calculation of one more two--loop massive operator matrix element in QED. The radiators are obtained as solutions of the associated Callen--Symanzik equations in the massive case. The radiators can be expressed in terms of harmonic polylogarithms to weight {\sf w = 6} of argument zz and (1−z)(1-z) and in Mellin NN space by generalized harmonic sums. Numerical results are presented on the position of the ZZ peak and corrections to the ZZ width, ΓZ\Gamma_Z. The corrections calculated result into a final theoretical accuracy for δMZ\delta M_Z and δΓZ\delta \Gamma_Z which is estimated to be of O(30 keV) at an anticipated systematic accuracy at the FCC\_ee of \sim 100 keV. This precision cannot be reached, however, by including only the corrections up to O(α3)O(\alpha^3).Comment: 58 pages, 3 Figure

    The two-mass contribution to the three-loop pure singlet operator matrix element

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    We present the two-mass QCD contributions to the pure singlet operator matrix element at three loop order in x-space. These terms are relevant for calculating the structure function F2(x,Q2)F_2(x,Q^2) at O(αs3)O(\alpha_s^3) as well as for the matching relations in the variable flavor number scheme and the heavy quark distribution functions at the same order. The result for the operator matrix element is given in terms of generalized iterated integrals that include square root letters in the alphabet, depending also on the mass ratio through the main argument. Numerical results are presented.Comment: 28 papges Latex, 3 figure

    The Two-mass Contribution to the Three-Loop Gluonic Operator Matrix Element Agg,Q(3)A_{gg,Q}^{(3)}

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    We calculate the two-mass QCD contributions to the massive operator matrix element Agg,QA_{gg,Q} at O(αs3)\mathcal{O} (\alpha_s^3) in analytic form in Mellin NN- and zz-space, maintaining the complete dependence on the heavy quark mass ratio. These terms are important ingredients for the matching relations of the variable flavor number scheme in the presence of two heavy quark flavors, such as charm and bottom. In Mellin NN-space the result is given in the form of nested harmonic, generalized harmonic, cyclotomic and binomial sums, with arguments depending on the mass ratio. The Mellin inversion of these quantities to zz-space gives rise to generalized iterated integrals with square root valued letters in the alphabet, depending on the mass ratio as well. Numerical results are presented.Comment: 99 pages LATEX, 2 Figure

    Iterated integrals over letters induced by quadratic forms

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    An automated treatment of iterated integrals based on letters induced by real-valued quadratic forms and Kummer--Poincar\'e letters is presented. These quantities emerge in analytic single and multi--scale Feynman diagram calculations. To compactify representations, one wishes to apply general properties of these quantities in computer-algebraic implementations. We provide the reduction to basis representations, expansions, analytic continuation and numerical evaluation of these quantities.Comment: 14 pages LATEX, 1 anc. fil

    The 3-Loop Pure Singlet Heavy Flavor Contributions to the Structure Function F2(x,Q2)F_2(x,Q^2) and the Anomalous Dimension

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    The pure singlet asymptotic heavy flavor corrections to 3-loop order for the deep-inelastic scattering structure function F2(x,Q2)F_2(x,Q^2) and the corresponding transition matrix element AQq(3),PSA_{Qq}^{(3), \sf PS} in the variable flavor number scheme are computed. In Mellin-NN space these inclusive quantities depend on generalized harmonic sums. We also recalculate the complete 3-loop pure singlet anomalous dimension for the first time. Numerical results for the Wilson coefficients, the operator matrix element and the contribution to the structure function F2(x,Q2)F_2(x,Q^2) are presented.Comment: 85 pages Latex, 14 Figures, 2 style file

    Heavy Flavor Wilson Coefficients in Deep-Inelastic Scattering: Recent Results

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    We present recent analytic results for the 3-loop corrections to the massive operator matrix element AQg(3)A_{Qg}^{(3)}for further color factors. These results have been obtained using the method of arbitrarily large moments. We also give an overview on the results which were obtained solving all difference and differential equations for the corresponding master integrals that factorize at first order.Comment: 11 pages Latex, To appear in the Proceedings of: QCDEV2017, JLAB, Newport News, VA, USA, May 22-26, 2017; Po

    Calculating Three Loop Ladder and V-Topologies for Massive Operator Matrix Elements by Computer Algebra

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    Three loop ladder and VV-topology diagrams contributing to the massive operator matrix element AQgA_{Qg} are calculated. The corresponding objects can all be expressed in terms of nested sums and recurrences depending on the Mellin variable NN and the dimensional parameter ε\varepsilon. Given these representations, the desired Laurent series expansions in ε\varepsilon can be obtained with the help of our computer algebra toolbox. Here we rely on generalized hypergeometric functions and Mellin-Barnes representations, on difference ring algorithms for symbolic summation, on an optimized version of the multivariate Almkvist-Zeilberger algorithm for symbolic integration, and on new methods to calculate Laurent series solutions of coupled systems of differential equations. The solutions can be computed for general coefficient matrices directly for any basis also performing the expansion in the dimensional parameter in case it is expressible in terms of indefinite nested product-sum expressions. This structural result is based on new results of our difference ring theory. In the cases discussed we deal with iterative sum- and integral-solutions over general alphabets. The final results are expressed in terms of special sums, forming quasi-shuffle algebras, such as nested harmonic sums, generalized harmonic sums, and nested binomially weighted (cyclotomic) sums. Analytic continuations to complex values of NN are possible through the recursion relations obeyed by these quantities and their analytic asymptotic expansions. The latter lead to a host of new constants beyond the multiple zeta values, the infinite generalized harmonic and cyclotomic sums in the case of VV-topologies.Comment: 110 pages Latex, 4 Figure

    The massive 3-loop operator matrix elements with two masses and the generalized variable flavor number scheme

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    We report on our latest results in the calculation of the two--mass contributions to 3--loop operator matrix elements (OMEs). These OMEs are needed to compute the corresponding contributions to the deep-inealstic scattering structure functions and to generalize the variable flavor number scheme by including both charm and bottom quarks. We present the results for the non-singlet and Agq,QA_{gq,Q} OMEs, and compare the size of their contribution relative to the single mass case. Results for the gluonic OME Agg,QA_{gg,Q} are given in the physical case, going beyond those presented in a previous publication where scalar diagrams were computed. We also discuss our recently published two--mass contribution to the pure singlet OME, and present an alternative method of calculating the corresponding diagrams.Comment: 20 pages Latex, 5 Figures, different style file
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