Abstract

We consider unfavoured light quark/antiquark to D meson fragmentation. We discuss nonperturbative effects for small transverse momenta. The asymmetry for D+ and D- production measured by the LHCb collaboration provides natural constraints on the parton (quark/antiquark) fragmentation functions. We find that already a fraction of $q/\overline q \to D$ fragmentation probability is sufficient to account for the measured asymmetry. Large D-meson production asymmetries are found for large xF which is related to dominance of light quark/antiquark $q/\overline q \to D$ fragmentation over the standard c → D fragmentation. As a consequence, prompt atmospheric neutrino flux at high neutrino energies can be much larger than for the conventional c → D fragmentation. The latter can constitute a sizeable background for the cosmic neutrinos claimed to be observed recently by the IceCube Observatory.

Highlights

  • It is believed that the D mesons are produced dominantly via c → D fragmentation mechanism which leads to a symmetric production of mesons and anti-mesons

  • The production asymmetries were interpreted in Ref. [2] as due to meson cloud mechanism and specific structure of the proton Fock components

  • The string model approach to the problem of heavy meson production and asymmetries in the production of heavy mesons was discussed in extent in Ref. [3]

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Summary

Introduction

It is believed that the D mesons are produced dominantly via c → D fragmentation mechanism which leads to a symmetric production of mesons and anti-mesons. We consider a simple alternative phenomenological explanation using so-called unfavored fragmentation functions responsible for light quark/antiquark fragmentation to D mesons. Such unfavoured fragmentation functions are known to be important e.g. for K+/K− production and corresponding asymmetries obtained at SPS [5] and RHIC [6]. Such asymmetries for kaon production were nicely explained in the picture of subleading parton fragmentation at low energies [7]. Possible consequences for prompt atmospheric neutrino production will be discussed

A theoretical basis of the calculations
The LHCb production asymmetry
Cosequences for prompt atmospheric neutrinos
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