807 research outputs found

    Analytic treatment of the two loop equal mass sunrise graph

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    The two loop equal mass sunrise graph is considered in the continuous d-dimensional regularisation for arbitrary values of the momentum transfer. After recalling the equivalence of the expansions at d=2 and d=4, the second order differential equation for the scalar Master Integral is expanded in (d-2) and solved by the variation of the constants method of Euler up to first order in (d-2) included. That requires the knowledge of the two independent solutions of the associated homogeneous equation, which are found to be related to the complete elliptic integrals of the first kind of suitable arguments. The behaviour and expansions of all the solutions at all the singular points of the equation are exhaustively discussed and written down explicitly.Comment: 33 pages, LaTeX, v2: +1 figure; v3: changes in the conclusions; simplifications in the recurrences (6.3) and (6.9

    Analytic evaluation of Feynman graph integrals

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    We review the main steps of the differential equation approach to the analytic evaluation of Feynman graphs, showing at the same time its application to the 3-loop sunrise graph in a particular kinematical configuration.Comment: 5 pages, 1 figure, uses npb.sty. Presented at RADCOR 2002 and Loops and Legs in Quantum Field Theory, 8-13 September 2002, Kloster Banz, Germany. Revised version: minor typos corrected, one reference adde

    The analytic value of a 3-loop sunrise graph in a particular kinematical configuration

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    We consider the scalar integral associated to the 3-loop sunrise graph with a massless line, two massive lines of equal mass MM, a fourth line of mass equal to MxMx, and the external invariant timelike and equal to the square of the fourth mass. We write the differential equation in xx satisfied by the integral, expand it in the continuous dimension dd around d=4d=4 and solve the system of the resulting chained differential equations in closed analytic form, expressing the solutions in terms of Harmonic Polylogarithms. As a byproduct, we give the limiting values of the coefficients of the (d−4)(d-4) expansion at x=1x=1 and x=0x=0.Comment: 9 pages, 3 figure

    The analytic value of the sunrise self-mass with two equal masses and the external invariant equal to the third squared mass

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    We consider the two-loop self-mass sunrise amplitude with two equal masses MM and the external invariant equal to the square of the third mass mm in the usual dd-continuous dimensional regularization. We write a second order differential equation for the amplitude in x=m/Mx=m/M and show as solve it in close analytic form. As a result, all the coefficients of the Laurent expansion in (d−4)(d-4) of the amplitude are expressed in terms of harmonic polylogarithms of argument xx and increasing weight. As a by product, we give the explicit analytic expressions of the value of the amplitude at x=1x=1, corresponding to the on-mass-shell sunrise amplitude in the equal mass case, up to the (d−4)5(d-4)^5 term included.Comment: 11 pages, 2 figures. Added Eq. (5.20) and reference [4

    The analytical value of the electron (g-2) at order alpha^3 in QED

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    We have evaluated in closed analytical form the contribution of the three-loop non-planar `triple-cross' diagrams contributing to the electron (g-2) in QED; its value, omitting the already known infrared divergent part, is a_e(3-cross) = 1/2 pi^2 Z(3) - 55/12 Z(5) - 16/135 pi^4 + 32/3 (a4 + 1/24 ln(2)^4) + 14/9 pi^2 ln(2)^2 - 1/3 Z(3) + 23/3 pi^2 ln(2) - 47/9 pi^2 - 113/48. This completes the analytical evaluation of the (g-2) at order alpha^3, giving a_e(3-loop) = (alpha/pi)^3 { 83/72 pi^2 Z(3) - 215/24 Z(5) + 100/3 [( a4 + 1/24 ln(2)^4 ) - 1/24 pi^2 ln(2)^2 ] - 239/2160 pi^4 + 139/18 Z(3) - 298/9 pi^2 ln(2) + 17101/810 pi^2 + 28259/5184 } = (alpha/pi)^3 (1.181241456...).Comment: plain TeX, 16 pages, 2 figures. Submitted to Physics Letters B. Two postscript files (z2.ps, zx1gen.ps) are include

    Precise numerical evaluation of the two loop sunrise graph Master Integrals in the equal mass case

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    We present a double precision routine in Fortran for the precise and fast numerical evaluation of the two Master Integrals (MIs) of the equal mass two-loop sunrise graph for arbitrary momentum transfer in d=2 and d=4 dimensions. The routine implements the accelerated power series expansions obtained by solving the corresponding differential equations for the MIs at their singular points. With a maximum of 22 terms for the worst case expansion a relative precision of better than a part in 10^{15} is achieved for arbitrary real values of the momentum transfer.Comment: 11 pages, LaTeX. The complete paper is also available via the www at http://www-ttp.physik.uni-karlsruhe.de/Preprints/ and the program can be downloaded from http://www-ttp.physik.uni-karlsruhe.de/Progdata

    Numerical evaluation of the general massive 2-loop sunrise self-mass master integrals from differential equations

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    The system of 4 differential equations in the external invariant satisfied by the 4 master integrals of the general massive 2-loop sunrise self-mass diagram is solved by the Runge-Kutta method in the complex plane. The method, whose features are discussed in details, offers a reliable and robust approach to the direct and precise numerical evaluation of Feynman graph integrals.Comment: 1+21 pages, Latex, 5 ps-figure

    Two-Loop Heavy-Flavor Contribution to Bhabha Scattering

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    We evaluate the two-loop QED corrections to the Bhabha scattering cross section which involve the vacuum polarization by heavy fermions of arbitrary mass m_f >> m_e. The results are valid for generic values of the Mandelstam invariants s,t,u >> m_e^2.Comment: 13 pages, 6 figures. Equations in the appendix generalized to the heavy-quark cas

    Electroweak Fermion-loop Contributions to the Muon Anomalous Magnetic Moment

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    The two-loop electroweak corrections to the anomalous magnetic moment of the muon, generated by fermionic loops, are calculated. An interesting role of the top quark in the anomaly cancellation is observed. New corrections, including terms of order GΌαmt2G_\mu \alpha m_t^2, are computed and a class of diagrams previously thought to vanish are found to be important. The total fermionic correction is −(23±3)×10−11-(23\pm 3) \times 10^{-11} which decreases the electroweak effects on g−2g-2, predicted from one-loop calculations, by 12\%. We give an updated theoretical prediction for g−2g-2 of the muon.Comment: Corrected versio
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