Abstract

Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb$^{-1}$ of proton--proton collisions at $\sqrt{s}=8$ TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.

Highlights

  • These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity

  • In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino

  • Due to the simultaneous fit, the uncertainty on the W +jets estimation decreases by 10% with respect to the numbers in table 9, while the uncertainties on the remaining non-multi-jet backgrounds vary by less than 2% depending on the signal regions (SR)

Read more

Summary

SUSY scenarios

SUSY scenarios characterised by the presence of light charginos, next-to-lightest neutralinos and sleptons can be realised in the general framework of the phenomenological Minimal Supersymmetric Standard Model (pMSSM) [44,45,46]. “Simplified models” [47, 48] characterised by χ±1 χ02 and χ±1 χ∓1 production, where the charginos and neutralinos decay with 100% branching fraction to final states with taus, are considered. In both simplified models the lightest neutralino is the LSP, and the only light slepton is the stau partner of the left-handed tau (τL). If charginos and next-to-lightest neutralinos are too heavy to be produced at the LHC, direct production of stau pairs [49] might become the dominant electroweak production process in the pMSSM. Final states containing hadronically decaying taus are considered in this search

The ATLAS detector
Data sample
Monte Carlo simulation
Standard Model processes
SUSY processes
Event reconstruction
Event selection
Standard Model background estimation
Multi-jet background estimation
Estimation of irreducible backgrounds
Fitting procedure
Systematic uncertainties
10 Results
11 Interpretation
11.1 Simplified models: chargino-neutralino and chargino-chargino production
11.2 Direct stau production
11.3 The pMSSM model
12 Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call