Abstract

The B physics programme of the ATLAS experiment includes measurements of production cross sections, searches for rare B-decay signatures which are sensitive to new physics at the TeV energy scale and studies of CP violation effects in B-events, such as $B_{s}^{0}\rightarrow J/\psi \phi$ and $B_{d}^{0}\rightarrow J/\psi K_{s}^{0}$. The key to the detection of these B signals in ATLAS is to achieve a high trigger efficiency for low-$p_{T}$ di-muon events, whilst keeping an acceptable trigger rate. ATLAS developed two separate approaches for triggering on di-muon events from resonances such as $J/\psi$ and Upsilon ($\Upsilon$). The first approach is to start from a di-muon trigger selected at Level-1 while the second is based on dedicated Level-2 algorithms. The performance for these triggers has been studied using collision data at $\sqrt{s}=7$ TeV collected in 2011.

Highlights

  • The ATLAS detectors provide input to the three levels of the trigger system that provides fast filtering capabilities and capture events of interest to physics with high efficiency

  • Level 1, whilst the second is based on a dedicated Level 2 to deeply inspect the events for their acceptation

  • C Owned by the authors, published by EDP Sciences, 2012proton collisions

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Summary

Introduction

The ATLAS detectors provide input to the three levels of the trigger system that provides fast filtering capabilities and capture events of interest to physics with high efficiency. Trigger (HLT), and these are based on software algorithms on muon, di-muon or electron signatures were designed to accommodate the large statistics provided by LHC.

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