Improving α QED ( M 2 Z ) and the charm mass by analytic continuation
نویسنده
چکیده
The standard determination of the QED coupling on the Z pole is performed using the latest available data for R. The direct application of analytic continuation techniques is found not to improve the accuracy of the value of α(M2 Z). However they help to resolve an ambiguity in the values of R in the energy region √ s ∼ 2 GeV, which, in turn, reduces the uncertainty in α(M2 Z). Moreover, they provide a sensitive determination of the mass of the charm quark. The favoured solution, which uses the inclusive data for R for √ s ∼ 2 GeV, has a pole mass mc = 1.33− 1.40 GeV and α−1(M2 Z) = 128.972± 0.026; whereas if the sum of the exclusive channels is used to determine R in this region, we find α−1(M2 Z) = 128.941 ± 0.029.
منابع مشابه
Massive Quark Production in Electron Positron Annihilation to Order α 2 s †
Recent analytical and numerical results for the three-loop polarization function allow to present a phenomenological analysis of the cross section for massive quark production in electron positron annihilation to order α 2 s. Numerical predictions based on fixed order perturbation theory are presented for charm and bottom production above 5 and 11.5 GeV, respectively. The contribution from thes...
متن کاملA new determination of the QED coupling α ( M 2 Z ) lets the Higgs off the hook
We use the available data on e+e− → hadrons to determine the value of the QED coupling at the Z pole. The inclusion of recent preliminary BES-II data in the analysis is found to reduce the ambiguity in the determination of the coupling, particularly that arising from the use of either exclusive or inclusive data in the energy region √ s ∼ 2 GeV, in favour of a larger value of α(M2 Z) −1 = 128.9...
متن کاملPlanar box diagram for the ( N F = 1 ) 2 - loop QED virtual corrections to Bhabha scattering
In this paper we present the master integrals necessary for the analytic calculation of the box diagrams with one electron loop (N F = 1) entering in the 2-loop (α 3) QED virtual corrections to the Bhabha scattering amplitude of the electron. We consider on-shell electrons and positrons of finite mass m, arbitrary squared c.m. energy s, and momentum transfer t; both UV and soft IR divergences a...
متن کاملPredictions for g − 2 of the muon and α QED ( M 2 Z )
We calculate (g − 2) of the muon and the QED coupling α(M 2 Z), by improving the determination of the hadronic vacuum polarization contributions and their uncertainties. We include the recently re-analysed CMD-2 data on e + e − → π + π −. We carefully combine a wide variety of data for the e + e − production of hadrons, and obtain the optimum form of R(s) ≡ σ 0 had (s)/σ pt (s), together with i...
متن کاملLeading log radiative corrections to deep inelastic production of heavy quarks
O(α) QED radiative corrections to neutral current deep inelastic production of heavy quarks are calculated in the leading log approximation and compared with the corresponding corrections assuming a massless charm parton. Besides the inclusive case, corrections to the semi-inclusive dσ/dxdydz and the effect of z-cuts are studied. In the latter case, the massless corrections differ from the corr...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2000