Abstract

The possible non-standard interactions (NSIs) of neutrinos with matter plays important role in the global determination of neutrino properties. In our study we select various data sets from LHC measurements at 13 TeV with integrated luminosities of 35 ∼ 139 fb−1, including production of a single jet, photon, W/Z boson, or charged lepton accompanied with large missing transverse momentum. We derive constraints on neutral-current NSIs with quarks imposed by different data sets in a framework of either effective operators or simplified Z′ models. We use theoretical predictions of productions induced by NSIs at next-to-leading order in QCD matched with parton showering which stabilize the theory predictions and result in more robust constraints. In a simplified Z′ model we obtain a 95% CLs upper limit on the conventional NSI strength ϵ of 0.042 and 0.0028 for a Z′ mass of 0.2 and 2 TeV respectively. We also discuss possible improvements from future runs of LHC with higher luminosities.

Highlights

  • Long-baseline(LBL) experiments are the generation neutrino oscillation experiments for their sensitivity to neutrino mass ordering and CP violating phase δCP [37,38,39,40,41,42]

  • For non-standard interactions (NSIs) induced by heavy mediator with mass larger than the experimental energy scale, bounds on NSI parameters ranging from sub-percent level to a few percent level are obtained by a global fit to data from current oscillation experiments and the two scattering experiments [47], under assumption that NSI affects only up or down quark at a time

  • We focus on the aforementioned Z model and study constraints on NC NSI parameters based on various measurements at LHC 13 TeV with large missing transverse momentums in the final states

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Summary

Model assumptions and constraints

Phenomenologies of neutrino non-standard interactions can span an energy range from MeV in neutrino oscillations to TeV at high energy colliders, or even higher in reaction of cosmic neutrinos. We outline the simplified models used in our study and the constraints obtained with LHC data

Theoretical setup
Data selection
Constraints for effective operator
Constraints for simplified Z model
Theoretical uncertainties
Next-to-leading order QCD corrections
Constraints at NLO
LHC combination and projections
Projections for future run of LHC with integrated luminosities of
Findings
Conclusion
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