Abstract

We present the calculation of the order αs2\alpha_s^2 corrections to the coefficient functions contributing to the longitudinal (FL(x,Q2)F_L(x,Q^2)) and transverse fragmentation functions (FT(x,Q2)F_T(x,Q^2)) measured in electron-positron annihilation. The effect of these higher order QCD corrections on the behaviour of the fragmentation functions and the corresponding longitudinal (dσL(x,Q2)/dxd\sigma_L(x,Q^2)/dx) and transverse cross sections (dσT(x,Q2)/dxd\sigma_T(x,Q^2)/dx) are studied. In particular we investigate the dependence of the above quantities on the mass factorization scale (MM) and the various parameterizations chosen for the parton fragmentation densities DpH(x,M2)D_p^H(x,M^2) (p=q,gp=q,g; H=π±,K±,P,PˉH=\pi^\pm, K^\pm, P, \bar{P}). Our analysis reveals that the order \alpha_s^2 contributions to FL(x,Q2)F_L(x,Q^2) are large whereas these contributions to FT(x,Q2)F_T(x,Q^2) are small. From the above fragmentation functions one can also compute the integrated cross sections σL\sigma_L and σT\sigma_T in an independent way. The sum σtot=σL+σT\sigma_{tot} = \sigma_L + \sigma_T, corrected up to order \alphastwo, agrees with the well known result in the literature providing us with an independent check an our calculations.Comment: 69 pages, latex2e, uses mcite, amsfonts. PostScript version available at http://rulgm4.leidenuniv.nl/preprints/transfrag.p

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    Last time updated on 02/01/2020