Limits...
Identification and energy calibration of hadronically decaying tau leptons with the ATLAS experiment in pp collisions at [Formula: see text][Formula: see text].

Aad G, Abbott B, Abdallah J, Abdel Khalek S, Abdinov O, Aben R, Abi B, Abolins M, AbouZeid OS, Abramowicz H, Abreu H, Abreu R, Abulaiti Y, Acharya BS, Adamczyk L, Adams DL, Adelman J, Adomeit S, Adye T, Agatonovic-Jovin T, Aguilar-Saavedra JA, Agustoni M, Ahlen SP, Ahmadov F, Aielli G, Akerstedt H, Åkesson TP, Akimoto G, Akimov AV, Alberghi GL, Albert J, Albrand S, Alconada Verzini MJ, Aleksa M, Aleksandrov IN, Alexa C, Alexander G, Alexandre G, Alexopoulos T, Alhroob M, Alimonti G, Alio L, Alison J, Allbrooke BM, Allison LJ, Allport PP, Aloisio A, Alonso A, Alonso F, Alpigiani C, Altheimer A, Alvarez Gonzalez B, Alviggi MG, Amako K, Amaral Coutinho Y, Amelung C, Amidei D, Amor Dos Santos SP, Amorim A, Amoroso S, Amram N, Amundsen G, Anastopoulos C, Ancu LS, Andari N, Andeen T, Anders CF, Anders G, Anderson KJ, Andreazza A, Andrei V, Anduaga XS, Angelidakis S, Angelozzi I, Anger P, Angerami A, Anghinolfi F, Anisenkov AV, Anjos N, Annovi A, Antonaki A, Antonelli M, Antonov A, Antos J, 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J, Zhu Y, Zhuang X, Zhukov K, Zibell A, Zieminska D, Zimine NI, Zimmermann C, Zimmermann R, Zimmermann S, Zimmermann S, Zinonos Z, Ziolkowski M, Zobernig G, Zoccoli A, Zur Nedden M, Zurzolo G, Zutshi V, Zwalinski L - Eur Phys J C Part Fields (2015)

Bottom Line: An uncertainty on the offline reconstructed tau energy scale of 2-4 %, depending on transverse energy and pseudorapidity, is achieved using two independent methods.The offline tau identification efficiency is measured with a precision of 2.5 % for hadronically decaying tau leptons with one associated track, and of 4 % for the case of three associated tracks, inclusive in pseudorapidity and for a visible transverse energy greater than 20 [Formula: see text].The performance of the tau algorithms, both offline and at the trigger level, is found to be stable with respect to the number of concurrent proton-proton interactions and has supported a variety of physics results using hadronically decaying tau leptons at ATLAS.

View Article: PubMed Central - PubMed

Affiliation: CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France.

ABSTRACT

This paper describes the trigger and offline reconstruction, identification and energy calibration algorithms for hadronic decays of tau leptons employed for the data collected from pp collisions in 2012 with the ATLAS detector at the LHC center-of-mass energy [Formula: see text] [Formula: see text]. The performance of these algorithms is measured in most cases with [Formula: see text] decays to tau leptons using the full 2012 dataset, corresponding to an integrated luminosity of 20.3 fb[Formula: see text]. An uncertainty on the offline reconstructed tau energy scale of 2-4 %, depending on transverse energy and pseudorapidity, is achieved using two independent methods. The offline tau identification efficiency is measured with a precision of 2.5 % for hadronically decaying tau leptons with one associated track, and of 4 % for the case of three associated tracks, inclusive in pseudorapidity and for a visible transverse energy greater than 20 [Formula: see text]. For hadronic tau lepton decays selected by offline algorithms, the tau trigger identification efficiency is measured with a precision of 2-8 %, depending on the transverse energy. The performance of the tau algorithms, both offline and at the trigger level, is found to be stable with respect to the number of concurrent proton-proton interactions and has supported a variety of physics results using hadronically decaying tau leptons at ATLAS.

No MeSH data available.


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Correction factors needed to bring the offline tau identification efficiency in simulation to the level observed in data, for all tau identification working points as a function of . The combinations of the muon and electron channels are also shown, and the results are displayed separately for a 1-track and b 3-track candidates with . The combined systematic and statistical uncertainties are shown
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Fig11: Correction factors needed to bring the offline tau identification efficiency in simulation to the level observed in data, for all tau identification working points as a function of . The combinations of the muon and electron channels are also shown, and the results are displayed separately for a 1-track and b 3-track candidates with . The combined systematic and statistical uncertainties are shown

Mentions: Results from the electron- and muon-tag analysis are combined to improve the precision of the correction factors, shown in Fig. 11. No significant dependency on the of the is observed and hence the results are provided separately only for the barrel () and the endcap () region, and for one and three associated tracks. Uncertainties depend slightly on the tau identification level and kinematic quantities. In Table 3, the most important systematic uncertainties for the working point used by most analyses, medium tau identification, are shown, together with the total statistical and systematic uncertainty. Uncertainties due to the underlying event (UE) are the dominant ones for the signal template, and are estimated by comparing alpgen-Herwig and Pythia simulations. The shower model and the amount of detector material are also varied and included in the number reported in Table 3. The W+jets shape uncertainty accounts for differences between the W+jets shape in the signal and control regions and is derived from comparisons to simulated W+jets events. The jet background fraction uncertainty accounts for the effect of propagating the statistical uncertainty on the jet misidentification rates.


Identification and energy calibration of hadronically decaying tau leptons with the ATLAS experiment in pp collisions at [Formula: see text][Formula: see text].

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J, Zhu Y, Zhuang X, Zhukov K, Zibell A, Zieminska D, Zimine NI, Zimmermann C, Zimmermann R, Zimmermann S, Zimmermann S, Zinonos Z, Ziolkowski M, Zobernig G, Zoccoli A, Zur Nedden M, Zurzolo G, Zutshi V, Zwalinski L - Eur Phys J C Part Fields (2015)

Correction factors needed to bring the offline tau identification efficiency in simulation to the level observed in data, for all tau identification working points as a function of . The combinations of the muon and electron channels are also shown, and the results are displayed separately for a 1-track and b 3-track candidates with . The combined systematic and statistical uncertainties are shown
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Fig11: Correction factors needed to bring the offline tau identification efficiency in simulation to the level observed in data, for all tau identification working points as a function of . The combinations of the muon and electron channels are also shown, and the results are displayed separately for a 1-track and b 3-track candidates with . The combined systematic and statistical uncertainties are shown
Mentions: Results from the electron- and muon-tag analysis are combined to improve the precision of the correction factors, shown in Fig. 11. No significant dependency on the of the is observed and hence the results are provided separately only for the barrel () and the endcap () region, and for one and three associated tracks. Uncertainties depend slightly on the tau identification level and kinematic quantities. In Table 3, the most important systematic uncertainties for the working point used by most analyses, medium tau identification, are shown, together with the total statistical and systematic uncertainty. Uncertainties due to the underlying event (UE) are the dominant ones for the signal template, and are estimated by comparing alpgen-Herwig and Pythia simulations. The shower model and the amount of detector material are also varied and included in the number reported in Table 3. The W+jets shape uncertainty accounts for differences between the W+jets shape in the signal and control regions and is derived from comparisons to simulated W+jets events. The jet background fraction uncertainty accounts for the effect of propagating the statistical uncertainty on the jet misidentification rates.

Bottom Line: An uncertainty on the offline reconstructed tau energy scale of 2-4 %, depending on transverse energy and pseudorapidity, is achieved using two independent methods.The offline tau identification efficiency is measured with a precision of 2.5 % for hadronically decaying tau leptons with one associated track, and of 4 % for the case of three associated tracks, inclusive in pseudorapidity and for a visible transverse energy greater than 20 [Formula: see text].The performance of the tau algorithms, both offline and at the trigger level, is found to be stable with respect to the number of concurrent proton-proton interactions and has supported a variety of physics results using hadronically decaying tau leptons at ATLAS.

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Affiliation: CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France.

ABSTRACT

This paper describes the trigger and offline reconstruction, identification and energy calibration algorithms for hadronic decays of tau leptons employed for the data collected from pp collisions in 2012 with the ATLAS detector at the LHC center-of-mass energy [Formula: see text] [Formula: see text]. The performance of these algorithms is measured in most cases with [Formula: see text] decays to tau leptons using the full 2012 dataset, corresponding to an integrated luminosity of 20.3 fb[Formula: see text]. An uncertainty on the offline reconstructed tau energy scale of 2-4 %, depending on transverse energy and pseudorapidity, is achieved using two independent methods. The offline tau identification efficiency is measured with a precision of 2.5 % for hadronically decaying tau leptons with one associated track, and of 4 % for the case of three associated tracks, inclusive in pseudorapidity and for a visible transverse energy greater than 20 [Formula: see text]. For hadronic tau lepton decays selected by offline algorithms, the tau trigger identification efficiency is measured with a precision of 2-8 %, depending on the transverse energy. The performance of the tau algorithms, both offline and at the trigger level, is found to be stable with respect to the number of concurrent proton-proton interactions and has supported a variety of physics results using hadronically decaying tau leptons at ATLAS.

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