Abstract

In this paper we show that the intrinsic heavy-quark QCD mechanism for the hadroproduction of heavy hadrons at large x_F can resolve the apparent conflict between measurements of double-charm baryons by the SELEX fixed-target experiment and the LHCb experiment at the LHC collider. We show that in fact both experiments are compatible, and that both can be correct. The observed spectroscopy of double-charm hadrons is in agreement with the predictions of supersymmetric light front holographic QCD.

Highlights

  • The first experimental evidence for the existence of doublecharm baryons was published by the SELEX collaboration

  • SELEX and LHCb we will utilize the predictions of the supersymmetric light front holographic QCD (SUSY LFHQCD)

  • Using both theoretical and experimental arguments, we have shown that the SELEX and the LHCb results for the production of doubly charmed baryons can both be correct

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Summary

Introduction

15 years ago [1,2,3,4,5,6]. By utilizing the Fermilab negative and positive charged beams at 600 GeV/c to produce charmed particles in a thin foil of copper or on a diamond target, the SELEX collaboration observed two different decay channels for the |dcc state at a mass close to 3520 MeV/c2. In QED, positronium has an analogous |e+e−μ+μ− Fock state due to the insertion of light-bylight scattering in the positronium self-energy amplitude In such an “intrinsic charm” Fock state |uudcc , the maximum kinematic configuration occurs at minimum invariant mass, where all quarks are at rest in the hadron’s rest frame; i.e., at equal rapidity in the moving hadron. The operator product expansion predicts that the probability of intrinsic heavy-quark Fock states |uud Q Qto scale as If such a Fock state interacts in a hadronic collision, the comoving udc of the projectile proton can readily coalesce. It is natural to hadro-produce a double-charm baryon |qcc at high xF from the materialization of the double-intrinsic charm |uudcccc Fock state of the projectile proton, since the qcc quarks can coalesce at the same rapidity [21]. In this paper we review the hadroproduction mechanisms of double-charm baryons for the different experimental environments and reinterpret the SELEX and LHCb results

Production rate and the kinematics of the
Mass difference
Suppression of the radiative decay
Findings
Summary
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