Production of $\Lambda_c$ baryons at the LHC within the $k_T$-factorization approach and independent parton fragmentation picture

TL;DR

This paper models $ ext{Lambda}_c$ baryon production at the LHC using $k_T$-factorization and independent fragmentation, finding challenges in explaining recent experimental data within this framework.

Contribution

It applies the $k_T$-factorization approach with modern gluon distributions to charm production and critically examines the independent fragmentation model for $ ext{Lambda}_c$ baryons against LHC data.

Findings

The model describes $D$ meson data well.

The $ ext{Lambda}_c$ fragmentation fraction needed is larger than in $e^+e^-$ or $ep$ experiments.

Independent fragmentation struggles to explain $ ext{Lambda}_c$ production data.

Abstract

We calculate cross section for production of $D$ mesons and $\Lambda_c$ baryons in proton-proton collisions at the LHC. The cross section for production of $c \bar c$ pairs is calculated within $k_T$-factorization approach with the Kimber-Martin-Ryskin unintegrated gluon distributions obtained on the basis of modern collinear gluon distribution functions. We show that our approach well describes the $D^0$, $D^+$ and $D_s$ experimental data. We try to understand recent ALICE and LHCb data for $\Lambda_c$ production with the $c \to \Lambda_c$ independent parton fragmentation approach. The Peterson fragmentation functions are used. The $f_{c \to \Lambda_c}$ fragmentation fraction and $\varepsilon_{c}^{\Lambda}$ parameter for $c \to \Lambda_c$ are varied. As a control plot we show transverse momentum distribution of different species of $D$ mesons assuming standard values of the $f_{c \to D}$ fragmentation fractions known from the literature. The fraction $f_{c \to \Lambda_c}$ neccessary to describe the ALICE data is much larger than the average value obtained from $e^+ e^-$ or $e p$ experiments. No drastic modification of the shape of fragmentation function is allowed by the new ALICE and LHCb data for $\Lambda_c$ production. We also discuss a possible dependence of the $\Lambda_c/ D^0$ baryon-to-meson ratio on rapidity and transverse momentum as seems observed recently by the ALICE and LHCb collaborations. Three different effects are considered: the value of $\varepsilon_c^{\Lambda}$ parameter in Peterson fragmentation function for $c \to \Lambda_c$, a kinematical effect related to the hadronization prescription and a possible feed-down from higher charmed-baryon excitations. It seems very difficult, if not impossible, to understand the ALICE data within the considered independent parton fragmentation scheme.