Table of Contents
Fetching ...

Power Corrections and Renormalons in $e^+e^-$ Fragmentation Functions

M. Dasgupta, B. R. Webber

TL;DR

The paper develops a dispersive, massive-gluon framework to estimate infrared power corrections to $e^+e^-$ fragmentation functions, focusing on the transverse, longitudinal, and asymmetric channels. It shows that leading nonperturbative corrections scale as $1/Q^2$ for individual coefficient functions, but gluon-induced small-$x$ singularities can promote some contributions to $1/Q$ in the separated cross sections, while these cancel in the total cross section. The authors derive explicit $x$-space and moment-space expressions for quark and gluon coefficient functions at $1/Q^2$ and discuss subleading $1/Q^4$ and beyond, highlighting how cancellations reconcile the dispersive approach with sum rules. The results clarify observed paradoxes in the data, connect with hadronization concepts, and provide a practical method to extract nonperturbative parameters such as $A_1$ from fragmentation observables.

Abstract

We estimate the power corrections (infrared renormalon contributions) to the coefficient functions for the transverse, longitudinal and asymmetric fragmentation functions in $e^+e^-$ annihilation, using a method based on the analysis of one-loop Feynman graphs containing a massive gluon. The leading corrections have the expected $1/Q^2$ behaviour, but the gluonic coefficients of the longitudinal and transverse contributions separately have strong singularities at small $x$, which cancel in their sum. This leads to $1/Q$ corrections to the longitudinal and transverse parts of the annihilation cross section, which cancel in the total cross section.

Power Corrections and Renormalons in $e^+e^-$ Fragmentation Functions

TL;DR

The paper develops a dispersive, massive-gluon framework to estimate infrared power corrections to fragmentation functions, focusing on the transverse, longitudinal, and asymmetric channels. It shows that leading nonperturbative corrections scale as for individual coefficient functions, but gluon-induced small- singularities can promote some contributions to in the separated cross sections, while these cancel in the total cross section. The authors derive explicit -space and moment-space expressions for quark and gluon coefficient functions at and discuss subleading and beyond, highlighting how cancellations reconcile the dispersive approach with sum rules. The results clarify observed paradoxes in the data, connect with hadronization concepts, and provide a practical method to extract nonperturbative parameters such as from fragmentation observables.

Abstract

We estimate the power corrections (infrared renormalon contributions) to the coefficient functions for the transverse, longitudinal and asymmetric fragmentation functions in annihilation, using a method based on the analysis of one-loop Feynman graphs containing a massive gluon. The leading corrections have the expected behaviour, but the gluonic coefficients of the longitudinal and transverse contributions separately have strong singularities at small , which cancel in their sum. This leads to corrections to the longitudinal and transverse parts of the annihilation cross section, which cancel in the total cross section.

Paper Structure

This paper contains 10 sections, 51 equations, 4 figures.

Figures (4)

  • Figure 1: Longitudinal fraction of the $e^+e^-{$e^+e^-$}$ hadronic cross section.
  • Figure 2: Coefficient of $1/Q^2$ correction to the total fragmentation function (solid), with quark (dashed) and gluon (dot-dashed) contributions shown separately.
  • Figure 3: Coefficient of $1/Q^2$ correction to the transverse fragmentation function (solid), with quark (dashed) and gluon (dot-dashed) contributions shown separately.
  • Figure 4: Coefficient of $1/Q^2$ correction to the longitudinal fragmentation function (solid), with quark (dashed) and gluon (dot-dashed) contributions shown separately.