Abstract

Within the most recent extension of the quark-jet hadronization framework, we explore the transverse-polarization-dependent dihadron fragmentation functions (DiFFs) $H_1^\sphericalangle$ and $H_1^\perp$ of a quark into $\pi^+\pi^-$ pairs. Monte Carlo (MC) simulations are employed to model polarized quark hadronization and calculate the corresponding number densities. These, in turn, are used to extract the Fourier cosine moments of the DiFFs $H_1^\sphericalangle$ and $H_1^\perp$. A notable finding is that there are previously unnoticed apparent discrepancies between the definitions of the so-called interference DiFF (IFF) $H_1^\sphericalangle$, entering the cross sections for two-hadron semi-inclusive electroproduction, and those involved in the production of two pairs of hadrons from back-to-back jets in electron-positron annihilation. This manuscript completes the studies of all four leading twist DiFFs for unpolarized hadron pairs within the quark-jet framework, following our previous work on the helicity-dependent DiFF $G_1^\perp$.

Highlights

  • The study of the transverse-polarization-dependent dihadron fragmentation functions (DiFFs) [1,2], and of the interference DiFF (IFF) in particular, has gained a lot of attention in recent years, both in theory and in experiment

  • In this paper we studied the two DiFFs describing the correlations between the transverse polarization of the fragmenting quark and the transverse momenta of a produced hadron pair in the hadronization process

  • The Fourier decomposition of these DiFFs only contains the cosine moments that were defined in Eqs. (14)–(17)

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Summary

INTRODUCTION

The study of the transverse-polarization-dependent dihadron fragmentation functions (DiFFs) [1,2], and of the interference DiFF (IFF) in particular, has gained a lot of attention in recent years, both in theory and in experiment. [8,9] used BELLE measurements [10] of the azimuthal asymmetry involving IFF H∢1 in inclusive dihadron pair production in back-to-back jets emanating from eþe− annihilation, along with input from Monte Carlo (MC) simulations for the unpolarized DiFF, to fit both the unpolarized DiFF D1 and the IFF H∢1 These fits were used to extract the transversity PDFs from the SIDIS measurements at HERMES [11]. We studied DiFFs [24,25,26] within the framework, with a simplistic treatment of the quark polarization to access the so-called single-hadron Collins fragmentation function and the IFF.

Kinematics and definitions
Fourier moments of DiFFs
EXTRACTING DIFFS FROM MONTE CARLO SIMULATIONS
THE QUARK-JET MODEL RESULTS
VALIDATION OF MC RESULTS
CONCLUSIONS
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