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# User Rev Content
1 friis 1.1 Tau lepton identification ($\tau$-ID) is a challenging but important endeavor
2     at hadron colliders. Standard Model (SM) Higgs boson searches and many new
3     physics scenarios Beyond the Standard Model (BSM) process have discovery
4     channels involving taus. In the Standard Model, the Higgs boson Yukawa
5     couplings are proportional to mass, resulting in decays to taus ten percent of
6     the time for scenearios where the higgs mass is below the diboson threshold.
7     In the Minimal Supersymmetric Model (MSSM), the coupling of members of the
8     Higgs sector doublet to the tau lepton is enhanced by a factor of $tan\beta$.
9    
10     The large mass of the tau makes it unique among the leptons in that can hadron
11     final states. These hadronic decays account for approximately 65\% of all tau
12     decays and have a signature of small number of collimated pions. The hadronic
13     decays are dominated by small number of collimated pions. This signature is
14     very similar QCD jet production, which in general has cross sections many
15     orders of magnitude larger than signal processes of interest. An additional
16     complication at hadron colliders is the presence of underlying event (UE), due
17     to secondary interactions in the $pp$ collision. These underlying event
18     particles are dominated by large numbers of soft pions which can overlap true
19     tau decays.
20    
21     The criterion for a successful $\tau$-ID is twofold: the algorithm must have
22     high tau efficiency to facilitate searches for rare new physics while
23     supressing the common backgrounds found at hadron colliders. This paper will
24     focus on novel algorithms designed to identify true hadronic tau decays and
25     reject common backgrounds.
26    
27     Tau identification in CMS is performed using objects from the ``Particle Flow''
28     algorithm. The particle flow algorithm provides a global and unique
29     reconstruction of the event. Signals in various subdectors are linked together
30     to reconstruct physics objects at particle granularity.