Some First Artemis Standard Model Measurements Samira Hassani

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Some First Artemis Standard Model Measurements Samira Hassani Saclay 1 st Artemis Annuel Meeting

Some First Artemis Standard Model Measurements Samira Hassani Saclay 1 st Artemis Annuel Meeting Chalkidiki, 26 -28 September 2007 26/09/07 1 st Artemis Meeting

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26/09/07 1 st Artemis Meeting 2

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26/09/07 1 st Artemis Meeting 3

Muon Spectrometer Performance • Quantities measuring the spectrometer performance • Momentum resolution. • Track-reconstruction

Muon Spectrometer Performance • Quantities measuring the spectrometer performance • Momentum resolution. • Track-reconstruction efficiency. • Quantities deteriorating the performance • Chamber inefficiencies. • Miscalibration of the MDT chambers. • Misalignment of the MDT chambers. • Errors of the magnetic-field map. 26/09/07 1 st Artemis Meeting 4

Measurement of Efficiencies in Data Tag and Probe Method to determine Efficiencies in Data

Measurement of Efficiencies in Data Tag and Probe Method to determine Efficiencies in Data N. Benekos, M. Schott, A. Wilson • Tag Muon: Track in Inner Detector AND Muon Spectrometer (+Isolation and p. T-Cuts) • Probe Muon: Track in Inner Detector (+Isolation and p. T-Cuts) • If this di-muon mass is 91 Ge. V ± 15 Gev and Δφ>2, then the probe muon is assumed to be a real muon: • muon efficiency is given by the fraction of probe muons with tracks in the Muon Spectrometer 26/09/07 1 st Artemis Meeting 5

 Z→μμ Signal Selection • Main Backgrounds – QCD: dominated by the decay of

Z→μμ Signal Selection • Main Backgrounds – QCD: dominated by the decay of bb→μμ – W→μν+jets – Z→т т→μμ • Selection cuts – Track PT > 20 Ge. V – Number of Tracks in Halo < 5 – Jet ET in Cone with Radius 0. 5 < 15 Ge. V – Track Isolation < 5 Ge. V – Di. Muon. Mass: 91 Ge. V± 15 Ge. V – Δφ>2 26/09/07 1 st Artemis Meeting 6

 Efficiencies from Data 26/09/07 1 st Artemis Meeting 7

Efficiencies from Data 26/09/07 1 st Artemis Meeting 7

Determination of the p. T-Resolution with data • Idea: Use (again) the Z-Boson Resonance.

Determination of the p. T-Resolution with data • Idea: Use (again) the Z-Boson Resonance. • Try to smear the p. T of Monte-Carlo generated muons in such a way, that they will reproduce the measured Z -Boson distribution. • The smearing function can be taken from full simulation 26/09/07 1 st Artemis Meeting 8

Muon Isolation Efficiency • Use Tag and Probe Method to determine Muon Isolation Efficiency

Muon Isolation Efficiency • Use Tag and Probe Method to determine Muon Isolation Efficiency • Tag Muon: – – p. T>15 -20 Ge. V Isolated • Probe Muon: – – p. T>15 -20 Ge. V Together with Tag Muon gives Δφ>2 |91 Ge. V-Mμμ|<30 Test if probe muon is Isolated 26/09/07 1 st Artemis Meeting 9

From B-physics Working group: J/psi’s, Ypsilon expected with first 10 pb-1 Events 10 pb-1

From B-physics Working group: J/psi’s, Ypsilon expected with first 10 pb-1 Events 10 pb-1 including trig and offline efficiency pp J/y ( m 6 m 4 ) X 156 000 bb J/y ( m 6 m 4 ) X 78 000 pp ( m 6 m 4 ) 31 000 1 600 B+ → J/y K+ 900 N / 50 Me. V B 0 → J/y K*(K+p-) 105 Number of events with 10 pb-1 Results shown use mu 6 mu 4 triggers At 1031 cm-2 s-1 we may have more events with mu 4 triggers, but simulations not ready yet, so we show mu 6 mu 4 here. 104 103 26/09/07 1 st Artemis Meeting 10

From B-physics Working group: J/psi’s, Ypsilon with first 10 pb-1 One of first physics

From B-physics Working group: J/psi’s, Ypsilon with first 10 pb-1 One of first physics measurements may be the ratio of direct J/y to B →J/y and direct J/y to v Proper time use to measure ratio J/y direct/indirect (B-decays) v Free from uncertainties in luminosity and trigger efficiencies… v However needs validation of ID alignment to enable good vertexing ‘Mix’ sample is direct and indirect J/y combined 26/09/07 1 st Artemis Meeting 11

From B-physics Working group: Reference channel B+ J/y. K+ to be used as ID

From B-physics Working group: Reference channel B+ J/y. K+ to be used as ID alignment tester already with 10 pb-1 Petridou, . Anastopoulos • B mass - lifetime fit – sensitive tests of detector alignments • No vertex displacement cuts (especially online) until ID alignments understood and validated. (2. 2%) B+ proper lifetime fit red B+ signal, black 26/09/07 background, blue all 1 st Artemis Meeting 12 World precision today (0. 67%)

First Artemis SM Measurement • For the Muon Spectrometer, we will be able to

First Artemis SM Measurement • For the Muon Spectrometer, we will be able to evaluate the: – Muon reconstruction efficiency – Muon isolation efficiency – Precision of Muon p. T-Resolution – Muon performance for low p. T muon from Jpsi and • For the Inner Detector, we can study the ID alignment using : – B+ proper lifetime measurement 26/09/07 1 st Artemis Meeting 13