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Muon Identification and Reconstruction. Stefano Rosati INFN – Roma 1. Muon Detectors for LHC. Aspects of central relevance: Trigger: reduce the event rate from the initial 40 MHz to the ~200 Hz affordable by the event storage system

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muon identification and reconstruction
Muon Identification and Reconstruction

Stefano Rosati

INFN – Roma 1

S. Rosati - MC Workshop

muon detectors for lhc
Muon Detectors for LHC

Aspects of central relevance:

  • Trigger: reduce the event rate from the initial 40 MHz to the ~200 Hz affordable by the event storage system
    • Organized over more levels, the first one has to operate a fast (<10 ns) choice and identification of the Region of Interest
    • Following levels process a limited subset of data (only from the RoI) with higher resolution and detail
    • Final level very close to offline reconstruction, running online on RoI data.
  • Offline reconstruction: provide optimal muon identification and momentum resolution over the pT range 5-1000 GeV
    • Standalone reconstruction can exploit the cleanerenvironment of the muon system
    • Combination with inner tracking detectors to improve resolution

S. Rosati - MC Workshop

atlas and cms experiements
ATLAS and CMS Experiements

Two approaches for the two experiments:

  • ATLAS:
    • 3 Air-core Toroids (one barrel, two endcaps), mean field 0.6 T with excellent standalone capabilities – complemented by a 2T Central Solenoid)
    • Different bending planes for Inner Detector and Muon Spectrometer (f and h)
    • Stringent requirements on tracking detectors resolution, calibration and alignment
    • Combined reconstruction gives optimal resolution in a certain momentum range
  • CMS:
    • Muon Detectors in the return yoke of the 4 T inner solenoidal field
    • Resolution dominated by Multiple Scatteringup to ~200 GeV pT
    • Combined reconstruction neededto achieve optimal resolution
    • Less stringent requirements on muon tracking detectors resolution, and on their calibration and alignment

S. Rosati - MC Workshop

atlas muon trigger lvl1
ATLAS Muon Trigger – LVL1

Barrel Trigger

Uses dedicated detector system based on RPCs and TGCs

Selection of events with muons above a given pT threshold (up to six programmable thresholds)

Coincidence of hits in space (both h and f) and time within geometrical windows in different trigger detector layers

S. Rosati - MC Workshop

atlas level 1 trigger
ATLAS – Level 1 Trigger

Endcap Efficiency vs pT Threshold – acceptance up to |h|<2.4

Example trigger menus and final rates, after also LVL2 and Event Filter (for L=2•1033 cm-2s-1):1m 20 GeV, 2m 10 GeV (40 Hz)2m 6 GeV (25 Hz)

Valid for both Barrel and Endcap

S. Rosati - MC Workshop

muon reconstruction in atlas

3 points

Initial layout

angle-angle

B~0

B

angle-point

B

sometimes

angle-angle

Ribs

Ribs

Muon Reconstruction in ATLAS

S. Rosati - MC Workshop

atlas combined reconstruction

Initial layout

Detector acceptance

ATLAS - Combined Reconstruction
  • Tracks are back-extrapolated to the IP
  • Parameters corrected for energy losses and multiple scattering
  • Energy loss ~3 GeV at h=0
  • Look for match with tracks reconstructed in the ID
    • Combined refit of the two tracks
    • or: statistical combination oftrack parameters
  • Inner Detector in a Solenoidal Field of 2 T.

Combined reco efficiency

S. Rosati - MC Workshop

atlas p t resolution
ATLAS – pT Resolution

Resolution vs pT

  • m-Spectrometer Standalone:~10%*pT 2 to 3% (pT in TeV)

150 X0 Calo Material:non-gaussian tails when back-extrapolated

  • Inner Detector Standalone:~40%*pT 1.5 % (|h|<1.9)~200%*pT 3% (|h|=2.5)(pT in TeV)
  • Combination dominated by the Inner Detector below the cross-over point~40 to 80 GeV (20 GeV in forward region)

S. Rosati - MC Workshop

atlas p t resolution1
ATLAS – pT Resolution
  • Muon Standalone reconstruction in brief: - 10% resolution up to 1 TeV requires 50 mm sagitta resolution

- Single point resolution ~80mm(MDT tracker – r-t calibration needed) - ~25 measurement points over the 3 stations

  • Alignment and calibration contribution becomes relevant above ~200 GeV
  • Alignment through optical system + alignment with tracks(e.g. data with field off/on)

required ~20 mm alignment precision obtained during TB of a full-scale slice

Contributions to the standalone resolution

S. Rosati - MC Workshop

low p t muon reconstruction

pT (MeV)

Low pT MuonReconstruction

Low pT muons (pT5 GeV) do not reach the outer muon stations

Extrapolate ID tracks and match with patterns of hits in the muon chambers

s=40 MeV

Efficiency

S. Rosati - MC Workshop

atlas muon isolation

HZZ*4l

Zbb

tt

GeV

GeV

GeV

ATLAS - Muon Isolation

Calorimeter Isolation - transverse energy

ID Isolation, SpT

  • Isolation energies in a DR = 0.2 cone
  • Correlation between Inner Detector and Calo isolation

ID vs Calo isolation

S. Rosati - MC Workshop

atlas muon isolation1
ATLAS - Muon Isolation

Mean value of the transverse EM energy vs cone size

Low and High Luminosity Pileup

S. Rosati - MC Workshop

impact parameter

Signal

Zbb

tt

Impact Parameter

Example:

d0 significance in HZZ*4l event selection

Reject Zbb and tt backgrounds

d0 w.r.t. primary interaction vertex fitted

s=13 mm

Highest significance

2nd Highest

S. Rosati - MC Workshop

atlas cavern background
ATLAS - Cavern Background
  • High background level expected in the ATLAS experimental hall
  • Background particles originating from p+phadrons + interactions in:
    • ATLAS shielding, forward detectors, machine elements
  • Relevant for trigger (fake coincidences), reconstruction (pattern recognition), detectors ageing (~0.7 C/cm after 10 years LHC on MDT wires)

Cavern background composition

Rates

S. Rosati - MC Workshop

cavern background

10 keV

Cavern Background

Tracking detectors sensitivities to neutral particles- photons ~1% - neutrons ~0.1%

Safety factors included in simulations to account for model uncertainties

High rates of uncorrelated hits:e.g. at L=1034cm-2s-1, safety factor 5,30K hits in MDT chambers(~10% occupancy)

Forward processes critical for the correct estimation of background production

Propagation of low-energy g and n

Energy distribution

S. Rosati - MC Workshop

atlas performance

Zmm

Muon Standalones=3.0 GeV

ATLAS - Performance

Mass resolutions for benchmark physics processes

Zmm fundamental to determine the detector mass scale with the first data, MS and MS-ID data

HZZ*4m(M=130 GeV)s=1.9 GeV

MuonCombined

Zmm

MuonCombined

s=2.5 GeV

S. Rosati - MC Workshop

cms muon system
CMS Muon System

4 measurement stations interleaved with the iron yoke slabs

4T field in the Solenoid

Drift Tubes and RPC in the Barrel

CSC and RPC in endcap, RPC coverage up to |h|=1.6

S. Rosati - MC Workshop

cms lvl1 trigger
CMS LVL1 Trigger

Two independent and redundant systemsDT+CSC or RPC, can be combined, together with calorimeters in a global trigger (GMT)

Trigger coverage for single muons up to |h|=2.1

RPC Trigger will cover up to |h|=1.6 at the startup

S. Rosati - MC Workshop

cms muon reconstruction
CMS Muon Reconstruction

Tracks are reconstructed in the muon spectrometer and back-extrapolated to the inner silicon tracker

GEANE package for the propagation through calo and coil material

Combined refit with vertex constraint

S. Rosati - MC Workshop

slide20

CMS Muon Identification

  • Muon Compatibility Values for two algs:
    • matching tracks with deposits in outer hadron calo
    • matching tracks with patterns in the inner muon chambers, not used for a standalone track fit
  • Cuts on discriminating values tunable for efficiency/purity

Calorimeter Match

Muon Detectors Match

S. Rosati - MC Workshop

slide21

CMS Muon Identification

Reconstruction+identification efficiency for muons in b-jets (pT>5 GeV)

Outside-in approach

Inside-out approach(track in Inner Detectormatched with muon hits)

S. Rosati - MC Workshop

cms p t resolution
CMS - pT Resolution

s(q/pT) for various momenta

Combined reconstruction

Standalone reconstruction

S. Rosati - MC Workshop

cms p t resolution1
CMS pT Resolution

Dp/p resolution in barrel and endcap

S. Rosati - MC Workshop

cms muon isolation
CMS Muon Isolation

b-jet muon rejection vs efficiency for Wmn identification

Three independent isolation criteria:- Energy deposits in calorimeters- Hits in pixel detector- Tracks reconstructed in inner tracker

S. Rosati - MC Workshop

cms performance
CMS - Performance

S. Rosati - MC Workshop

cms performance1
CMS - Performance

Zmm , reconstructed mass - 1 day of data taking at L=2•1033 cm-2s-1 - QCD background and pileup included

Z’(1 TeV)mmin three scenarios: - Ideal geometry - First data misalignment - Long term misalignment

Alignment exploiting inclusive single muons with pT>40 GeV and Zmm

S. Rosati - MC Workshop

in conclusione competenze italiane
In conclusione: competenze italiane
  • ATLAS-Muon (Bologna, Cosenza, Frascati, Lecce, Napoli, Pavia, Roma 1, Roma 2, Roma 3)
    • Trigger (Livello 1 barrel, Livello 2, Event Filter)
    • Calibrazione ed allineamento MDT
    • Simulazione del rivelatore, studi sul fondo di caverna
    • Ricostruzione standalone e combinata, online e offline, Analysis Software Framework
    • Analisi (Z+jets, HZZ*4l, A/hmm, Susy searches )
  • CMS-Muon (Bari, Bologna, Napoli, Padova, Torino)
    • Trigger di Livello 1 con I DT
    • Simulazione/digitizzazione, trigger RPC
    • Ricostruzione, High Level Trigger, Analysis Software Framework
    • Analisi (HWW2m2n, HZZ2e2m, hmm, WW scattering)
  • Grazie a Ugo Gasparini per tutta la documentazione su CMS

S. Rosati - MC Workshop

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