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
Summary
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.
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