Abstract

The existence of tiny neutrino masses and flavor mixings can be explained naturally in various seesaw models, many of which typically having additional Majorana type SM gauge singlet right handed neutrinos (N). If they are at around the electroweak scale and furnished with sizable mixings with light active neutrinos, they can be produced at high energy colliders, such as the Large Hadron Collider (LHC). A characteristic signature would be same sign lepton pairs, violating lepton number, together with light jets — pp → Nℓ±, N → ℓ±W∓, W∓ → jj. We propose a new search strategy utilising jet substructure techniques, observing that for a heavy right handed neutrino mass MN much above MW ±, the two jets coming out of the boosted W± may be interpreted as a single fat-jet (J). Hence, the distinguishing signal topology will be ℓ±ℓ±J . Performing a comprehensive study of the different signal regions along with complete background analysis, in tandem with detector level simulations, we compute statistical significance limits. We find that heavy neutrinos can be explored effectively for mass ranges 300 GeV ≤ MN ≤ 800 GeV and different light-heavy neutrino mixing |VμN|2. At the 13 TeV LHC with 3000 fb−1 integrated luminosity one can competently explore mixing angles much below present LHC limits, and moreover exceed bounds from electroweak precision data.

Highlights

  • W Z+j9881.3+7639.3 [100%]5496.6+5074.1 [60%]189.9+188.1 [2.2%]36.5+ 27.2 [0.4%]11.6+8.5 [0.1%] 5.9+5.2 [0.06%] WWZ +j252.1+240.4 [100%]208.0+193.4 [82%]24.2+ 19.6 [8.9%]14.14+12.4 [5.3%] 6.6+5.0 [2.3%] 3.0+2.8 [1.2%]

  • We propose a new search strategy utilising jet substructure techniques, observing that for a heavy right handed neutrino mass MN much above MW ±, the two jets coming out of the boosted W ± may be interpreted as a single fat-jet (J)

  • Seesaw models can naturally incorporate the existence of tiny neutrino masses and flavor mixings through simple extensions of the SM, many of which have Majorana RHNs

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Summary

Model and heavy Majorana neutrinos at the LHC

In the simplest model of seesaw, we only introduce SM gauge-singlet Majorana RHNs NRβ (where β is a flavor index). Of its mass (Left) The total pr√oduction cross section of the at the LHC with s = 13 TeV and normalised heavy Majorana neutrino as a by the |VμN |2. In our analysis we will consider Majorana RHNs having mass in the range 300 GeV ≤ MN ≤ 800 GeV In this mass range, the W ± boson from the leading decay mode N → W (see figure 2), will be boosted. These boosted W ± can decay hadronically to produce a fat-jet, with the characteristic final state μ±μ±J

Fat-jets and jet substructure for W -like jet tagging
Analysis setup and simulation
Results and discussion
Background
Conclusions
Full Text
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