Top Banner
QGP France 20-23 sept 2010 Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1
19

QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

Jan 04, 2016

Download

Documents

Verity Pearson
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

1Sanjoy Pal QGP France 20-23 sept 2010

Performances of the tracking Chambers of the ALICE MUON Spectrometer

Page 2: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

2Sanjoy Pal QGP France 20-23 sept 2010

ALICE muon Spectrometer

x

y

z

muon Spectrometer

Physics Goals :Studying heavy quark production via their muonic and semi-muonic decay inForward rapidity (-4 < y < -2.5)Large quarkonia acceptance down to pT 0Measurement of Quarkonia production  - as a function of centrality (ZDC) - as a function of pT, rapidity 

St3 , St4 and St5 Slats type

St1 and St2Quadrants type

Muon Tracking System:Five stations Two detection planes for each station.

Detection plane consists of Multi wire proportional chambers with bi-cathode pad readout: bending and non-bending.  Expected Spatial resolution below 100 m in the bending plane, around 700 µm in the non-bending

Page 3: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

3Sanjoy Pal QGP France 20-23 sept 2010

Muon Tracking System

Muon Tracking System:The total area of covers about 100 m2

Total number of readout pads about 1 million

Gas Mixure : Ar + CO2 (20%)High Voltage : 1650 VoltWire diameter : 20 µmWire pitch : 2 mm for St1

: 2.5 mm for St 2,3,4 & 5Anode cathode gap : 2 mm for St1

: 2.5 mm for St 2,3,4 & 5

Pad width y direction for Bending Cathode 4 mm for St1 5 mm for St 2,3,4 & 5 Pad width x direction for Non-bending Cathode 6 mm for St1 7.5 mm for St 2,3,4 & 5

The chamber thickness : 0.03 X0

Muon Dipole Magnet (Bx) :

B=0.7 T, ∫Bdl ~ 3 Tm

Page 4: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

4Sanjoy Pal QGP France 20-23 sept 2010

Readout buspatches configuration for the NonBending plane

in red buspatchs which are present in configurationIn white buspatchs which are removed from configuration

Page 5: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

5Sanjoy Pal QGP France 20-23 sept 2010

Readout buspatches configuration for the Bending plane

5% of the Read out Channel are removed form configuration

Page 6: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

6Sanjoy Pal QGP France 20-23 sept 2010

Pedestal Bending (max 500 ADC Channel)

in black MANU`s which are also dead

Page 7: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

7Sanjoy Pal QGP France 20-23 sept 2010

Pedestal NonBending (max 500 ADC Channel)

Page 8: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

8Sanjoy Pal QGP France 20-23 sept 2010

Noise Bending (max 5 ADC Channel)

1 ADC Ch ~ 1000 e

Noise below 3 ADC Ch for most of the read out Channel and average around 1.5 Ch which is very good

Page 9: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

9Sanjoy Pal QGP France 20-23 sept 2010

Noise Non Bending (max 5 ADC Channel)

Noise is higher compare to bending plane but it is less critical

Page 10: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

10Sanjoy Pal

Zero-Suppression

QGP France 20-23 sept 2010

The pedestal and noise per readout channel give threshold for 0-suppression : critical parameter !

• Mean and sigma values of pedestals for each readout channel are calculated by DA over 400 event //

===========================================================================

// NEW File calculated by makeped//

===========================================================================

// * Statistics : 400// * # of MANUS : // * # of channels : ////---------------------------------------------------------------------------//format ://---------------------------------------------------------------------------// BUS_PATCH MANU_ADDR CHANNEL MEAN SIGMA//---------------------------------------------------------------------------1 4 0 112.572 0.8699521 4 1 207.938 0.8911541 4 2 212.385 1.069011 4 3 242.233 0.9770931 4 4 302.468 1.026151 4 5 221.775 0.9188991 4 6 263.75 1.008711 4 7 185.86 0.9840731 4 8 241.141 0.9439911 4 9 246.949 0.919999• 4 10 209.31 0.89883

Flat ASCII file

Zero-Suppression is performed by FEE (MARC).Pedestal and noise

distribution for one

plane of a quadrant

Page 11: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

11Sanjoy PalQGP France 20-23 sept 2010

High Voltage configuration

1400 V

Nominal HV = 1650 volt

1500 V

Page 12: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

12Sanjoy Pal

Total Cluster charge distributions in pp run 2010

Station 1 have relatively High gain Station 2 have relatively low gain compare to Station 3, 4 & 5

QGP France 20-23 sept 2010

Absolute values of gain are not important for position resolution calculation

Page 13: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

13Sanjoy Pal

No of pad hits in the B plane involved in a cluster for each chamber

QGP France 20-23 sept 2010

3 Pad hit in bending direction is needed for nominal position resolution

Page 14: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

14Sanjoy Pal QGP France 20-23 sept 2010

No of pad hits in the NB plane involved in a cluster for each chamber

Page 15: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

15Sanjoy Pal

Charge correlation between two cathodes

QGP France 20-23 sept 2010

Station 1Station 2

Station 3 Station 4 Station 5

Page 16: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

16Sanjoy Pal QGP France 20-23 sept 2010

Occupancy Bending (max 0.01)

Mean Occupancy ~ 0.002

Page 17: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

17Sanjoy Pal QGP France 20-23 sept 2010

Occupancy NonBending (max 0.01)

Page 18: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

18Sanjoy Pal

Condition to reconstruct a track :one hit among chambers 1 & 2.one hit among chambers 3 & 4.one hit among chambers 5 & 6.three hits among chambers 7, 8, 9 & 10.Total tracking efficiency for LHC10e : Total = 93.7 ± 0.9 %

QGP France 20-23 sept 2010

Chamber Efficiency

Page 19: QGP France 20-23 sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.

19Sanjoy Pal QGP France 20-23 sept 2010

Summary

• We have a quite stable read-out configuration with a busy time most often less than 500 μs ; baseline is 330 μs.• We have a quite stable HV configuration.• Excellent behavior of all the Muon Chambers was

achieved during pp run-2010.• Tracking efficiency ~95%• Ready for HI data taking.