Abstract

We present a new calculation of the energy distribution of high-energy neutrinos from the decay of charm and bottom hadrons produced at the Large Hadron Collider (LHC). In the kinematical region of very forward rapidities, heavy-flavor production and decay is a source of tau neutrinos that leads to thousands of charged-current tau neutrino events in a 1 m long, 1 m radius lead neutrino detector at a distance of 480 m from the interaction region. In our computation, next-to-leading order QCD radiative corrections are accounted for in the production cross-sections. Non-perturbative intrinsic-kT effects are approximated by a simple phenomenological model introducing a Gaussian kT -smearing of the parton distribution functions, which might also mimic perturbative effects due to multiple initial-state soft-gluon emissions. The transition from partonic to hadronic states is described by phenomenological fragmentation functions. To study the effect of various input parameters, theoretical predictions for {D}_s^{pm } production are compared with LHCb data on double-differential cross-sections in transverse momentum and rapidity. The uncertain- ties related to the choice of the input parameter values, ultimately affecting the predictions of the tau neutrino event distributions, are discussed. We consider a 3+1 neutrino mixing scenario to illustrate the potential for a neutrino experiment to constrain the 3+1 parameter space using tau neutrinos and antineutrinos. We find large theoretical uncertainties in the predictions of the neutrino fluxes in the far-forward region. Untangling the effects of tau neutrino oscillations into sterile neutrinos and distinguishing a 3+1 scenario from the standard scenario with three active neutrino flavours, will be challenging due to the large theoretical uncertainties from QCD.

Highlights

  • JHEP06(2020)032 produce large fluxes of tau neutrinos in the forward direction [12,13,14,15]

  • We present a new calculation of the energy distribution of high-energy neutrinos from the decay of charm and bottom hadrons produced at the Large Hadron Collider (LHC)

  • We find that NF = 1.44 and kT = 2.23 GeV is the best fit in that case when NR = 1, with χ2/DOF=2.68 and with corresponding predicted σccfor 1 GeV< pT < 8 GeV and 2.0 < y < 4.5 amounting to 87% of the central value of the experimental result by the LHCb collaboration, which they extrapolate from Ds data

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Summary

Overview of forward neutrino detection geometry

A forward detector along a line tangent to the LHC beam line necessitates calculations in high-pseudorapidity regimes. The compact source means the assumed detector radius of 1 m and distance of 480 m from the interaction point translates to a maximum angle relative to the beam axis for the tau neutrino three-momentum of θmax = 2.1 mrad (ηmin = 6.87) This same constraint applies to the momenta of muon and electron neutrinos from heavy-flavor decays. [18], an evaluation of the number of νμ + νμ events in a detector of 25 cm × 25 cm cross sectional area finds that most of the events below 1 TeV come from charged pion and kaon decays that occur within 55 m of the interaction point and stay within the opening of the front quadrupole absorber with inner radius of 17 mm This corresponds to light-meson momenta lying within 1 mrad from the beam axis.

Forward heavy-flavor production and decay at the LHC
Tau neutrinos
Muon neutrinos
New physics
Conclusions
Findings
A Decay distributions
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