Abstract

The effect of nonperturbative and higher order perturbative corrections to all the free nucleon structure functions ($F_{iN}(x,Q^2); i=1-5$) in the DIS of $\nu_\tau/{\bar\nu}_\tau$ on nucleon is studied. The target mass correction (TMC) and higher twist (HT) effects are incorporated following the works of Kretzer et al. and Dasgupta et al., respectively. The evaluation of the nucleon structure functions has been performed by using the MMHT 2014 parameterization of the parton distribution functions (PDFs). The calculations have been performed at the next-to-leading(NLO) order. These nucleon structure functions (SF) are used to calculate the DIS cross section by further including the kinematical corrections due to $\tau$-lepton mass. Due to the inclusion of lepton mass two additional structure functions $F_{4N}(x,Q^2)$ and $F_{5N}(x,Q^2)$ become non-negligible. The results for the nucleon structure functions, differential and total scattering cross sections are presented. The various effects considered in this work are effective in the different regions of $x$ and $Q^2$, and quite important in the energy region of $E_{\nu_\tau/{\bar\nu}_\tau} < 15$ GeV. A comparative study of our results with the existing results in the literature for the cross sections is made in the energy region of interest for the DUNE, SHiP, DsTau and HyperK experiments proposed to be done in the near future.

Highlights

  • With the discovery of the τ-lepton in 1975 by the Stanford Linear Accelerator Center–Lawrence Berkeley Laboratory (SLAC-LBL) collaboration [1], predictions were made for the existence of its weak isospin neutral partner ντ

  • We have presented the results for the free nucleon structure functions, the differential and the total scattering cross sections obtained by using the formalism discussed in the previous section

  • The difference in the results of free nucleon structure functions FiNðx; Q2Þ; ði 1⁄4 1–5Þ evaluated at next-to-leading order (NLO) with and without the target mass corrections (TMC) effect at x 1⁄4 0.3 is 5%ð3%Þ in F1Nðx; Q2Þ, 2%ð< 1%Þ in F2Nðx; Q2Þ, 7%ð∼3%Þ in F3Nðx; Q2Þ and 4%ð∼2%Þ in F5Nðx; Q2Þ for Q2 1⁄4 2ð5Þ GeV2

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Summary

INTRODUCTION

With the discovery of the τ-lepton in 1975 by the Stanford Linear Accelerator Center–Lawrence Berkeley Laboratory (SLAC-LBL) collaboration [1], predictions were made for the existence of its weak isospin neutral partner ντ. We have presented and discussed in some detail the effect of τ-lepton mass on the total and differential cross sections arising due to the kinematic corrections in the contribution of F1Nðx; Q2Þ, F2Nðx; Q2Þ and F3Nðx; Q2Þ as well as due to the presence of additional structure functions F4Nðx; Q2Þ and F5Nðx; Q2Þ by comparing the στ and σμ cross sections for various energies in the DIS region of ντ=ντ − N scattering. We will discuss the higher order perturbative QCD corrections

NLO evolution
RESULTS AND DISCUSSION
E dσ dy vs y at
SUMMARY AND CONCLUSIONS
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