61 research outputs found

    The partially alternating ternary sum in an associative dialgebra

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    The alternating ternary sum in an associative algebra, abcacbbac+bca+cabcbaabc - acb - bac + bca + cab - cba, gives rise to the partially alternating ternary sum in an associative dialgebra with products \dashv and \vdash by making the argument aa the center of each term: abcacbbac+cab+bcacbaa \dashv b \dashv c - a \dashv c \dashv b - b \vdash a \dashv c + c \vdash a \dashv b + b \vdash c \vdash a - c \vdash b \vdash a. We use computer algebra to determine the polynomial identities in degree 9\le 9 satisfied by this new trilinear operation. In degrees 3 and 5 we obtain [a,b,c]+[a,c,b]0[a,b,c] + [a,c,b] \equiv 0 and [a,[b,c,d],e]+[a,[c,b,d],e]0[a,[b,c,d],e] + [a,[c,b,d],e] \equiv 0; these identities define a new variety of partially alternating ternary algebras. We show that there is a 49-dimensional space of multilinear identities in degree 7, and we find equivalent nonlinear identities. We use the representation theory of the symmetric group to show that there are no new identities in degree 9.Comment: 14 page

    \delta-derivations of n-ary algebras

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    We defined \delta-derivations of n-ary algebras. We described \delta-derivations of (n+1)-dimensional n-ary Filippov algebras and simple finite-dimensional Filippov algebras over algebraically closed field zero characteristic, and simple ternary Malcev algebra M_8. We constructed new examples of non-trivial \delta-derivations of Filippov algebras and new examples of non-trivial antiderivations of simple Filippov algebras.Comment: 12 page

    The anomalous magnetic moment of the muon in the Standard Model

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    194 pages, 103 figures, bib files for the citation references are available from: https://muon-gm2-theory.illinois.eduWe review the present status of the Standard Model calculation of the anomalous magnetic moment of the muon. This is performed in a perturbative expansion in the fine-structure constant α\alpha and is broken down into pure QED, electroweak, and hadronic contributions. The pure QED contribution is by far the largest and has been evaluated up to and including O(α5)\mathcal{O}(\alpha^5) with negligible numerical uncertainty. The electroweak contribution is suppressed by (mμ/MW)2(m_\mu/M_W)^2 and only shows up at the level of the seventh significant digit. It has been evaluated up to two loops and is known to better than one percent. Hadronic contributions are the most difficult to calculate and are responsible for almost all of the theoretical uncertainty. The leading hadronic contribution appears at O(α2)\mathcal{O}(\alpha^2) and is due to hadronic vacuum polarization, whereas at O(α3)\mathcal{O}(\alpha^3) the hadronic light-by-light scattering contribution appears. Given the low characteristic scale of this observable, these contributions have to be calculated with nonperturbative methods, in particular, dispersion relations and the lattice approach to QCD. The largest part of this review is dedicated to a detailed account of recent efforts to improve the calculation of these two contributions with either a data-driven, dispersive approach, or a first-principle, lattice-QCD approach. The final result reads aμSM=116591810(43)×1011a_\mu^\text{SM}=116\,591\,810(43)\times 10^{-11} and is smaller than the Brookhaven measurement by 3.7σ\sigma. The experimental uncertainty will soon be reduced by up to a factor four by the new experiment currently running at Fermilab, and also by the future J-PARC experiment. This and the prospects to further reduce the theoretical uncertainty in the near future-which are also discussed here-make this quantity one of the most promising places to look for evidence of new physics

    Finite Semisimple Loop Algebras of Indecomposable RA Loops

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    Units in finite loop algebras of RA2 loops

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