dpf2006 and jps2006 joint conference sheraton waikiki hotel, honolulu, hawaii october 30, 2006

25
The Detector Performance Study for the Barrel Section of the ATLAS Semiconductor Tracker (SCT) with Cosmic Rays Yoshikazu Nagai (Univ. of Tsukuba) For the ATLAS SCT Collaboration DPF2006 and JPS2006 joint conference Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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The Detector Performance Study for the Barrel Section of the ATLAS Semiconductor Tracker (SCT) with Cosmic Rays. Yoshikazu Nagai (Univ. of Tsukuba) For the ATLAS SCT Collaboration. DPF2006 and JPS2006 joint conference Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006. Contents. - PowerPoint PPT Presentation

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Page 1: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

The Detector Performance Study for the Barrel Section of the ATLAS Semiconductor Tracker (SCT) with

Cosmic Rays

Yoshikazu Nagai (Univ. of Tsukuba)

For the ATLAS SCT Collaboration

DPF2006 and JPS2006 joint conference Sheraton Waikiki Hotel, Honolulu, Hawaii

October 30, 2006

Page 2: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

2

Contents• Introduction A Toroidal LHC Apparatus (ATLAS)

ID Barrel Combined Cosmic Ray Test

• SCT Analysis

• Summary

1. Track reconstruction 2. SCT Module Efficiency3. Track Residual4. Time of Flight Analysis

Page 3: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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•Inner Detector

Pixel : the pixel detector

SCT : the semiconductor tracker

TRT : the transition radiation tracker

• Calorimeter

• Muon Systems

• Magnet systems

A Toroidal LHC ApparatuS (ATLAS)

Tile HDLAr EM

LAr HEC

LAr HEC

Muon Systems

42m

23m

Magnet systems

Overall weight : 7000 Tons

Tracker :

Calorimeter :

2.5

4.9

Page 4: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

4

S3

S2

S1

trigger: or 1 2 3S S S 1 2S S

TRT

SCT

ID Barrel Combined Cosmic Ray Test

SCT + TRT Combined Run• The test was performed during

5 weeks on early summer ’06• Corrected ~0.5M cosmic triggers

• Number of functional channels in SCT Barrel : 99.7 +- 0.03%

For this study, we use ~130K events(~25% of total triggered events)

Page 5: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

5

layer 0

layer 3

layer 1

layer 2

Top

Bottom

Outer

Inner

y

Barrel Configuration of Cosmic test

No magnetic field12 modules

: 6 : 6

# of Modules =468 (out of 2112 modules)(Top=252, Bottom=216)(layer 0,1,2,3) = (84/108/144/132)

Page 6: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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ID Barrel Combined Cosmic Ray Test

First combined test of ID with realistic geometry !!

• Test SCT 4 barrels with operating TRT

• Check detector efficiency, noise level, alignment study, tracking study

• etc …

• The detector performance aspects

Goals of combined cosmic ray test

• Detector operation & commissioning of system

• Gain experience with detector operation

• Test combined detector operation• Commission offline software• etc …

Page 7: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

7

SCT Analysis

1.Track reconstruction 2.SCT Module Efficiency3.Track Residuals4.Time of Flight Analysis

Page 8: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

8

1. Track Reconstruction

Tracks are reconstructed in ATHENA (ATLAS software) frame work.

It includes 2 processes, which are

pattern finding and fitting procedure

pattern finding

• Space point formation

• Straight line fitting

• Track candidates formation

fitting procedure

• Re-fitting track candidates with strip hits

• Fitting with minimization

Page 9: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

9

• Track candidates are built by fitting these space points with straight- line

Pattern finding procedure• Space point is formed for every intersection of the strips on the front

and back side of a module with SCT stereo information

-> Space points have the 3-D position information

SCT

Space point definition

40mrad

1 module

strip pitch = 80 m

track candidate

muon

Page 10: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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Fitting Procedure

if track candidates are found, then

• Track candidates are re-fitted by hits (single or a few strips)

if the track has chi^2 / ndof < 40,

it is accepted !!

(Here, tracks are roughly cut)

1 module

track SCT hit position definition

strip fired strip pitch = 80 m

hit

Page 11: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

11

• For accepted tracks• remove one layer hits (e.g. remove hits in layer 0)• refit the track

if refitted track fills : chi^2 / ndof < 10 &

Hits in Top sector >= 4 & Hits in Bottom sector >= 4

this track is used for efficiency calculation

2. SCT Module Efficiency

black : real data

red : sim data

chi^2 / ndofmm

real data with no alignment

remove hit

hit

track

sigma ~m

SCT residuals Reduced chi^2

res = track position – hit position

Page 12: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

12

Efficiency Calculation

strip fired

predicted hit position

1.5mm

Hit Observed !!

• extrapolate the refitted track to the module surface which hits removed

= predicted hit position• search hits from the predicted hit position within 1.5mm

= observed hit or not

• Efficiency

Eff = # of observed hits / # of predicted hits

strip fired

predicted hit position

1.5mm

No Hit !!

mm

Page 13: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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SCT Module Efficiency

layer 1 Outer layer 1 Inner

Top

Bottom Bottom

Top

layer 0

layer 3

layer 1

layer 2

Top

Bottom Most of modules show good performance !!

No magnetic field

12 modules

: 6 : 6

Page 14: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

14

laye

r 0

Inne

rla

yer

1 O

uter

laye

r 2

Out

er

laye

r 1

Inne

r

laye

r 2

Inne

rla

yer

3 O

uter

laye

r 3

Inne

r

Average efficiency for each layer / side

Nominal efficiency of layer 0,1,2 are ~ 99% without modules’ alignment

(dead channels are included for this calculation)

laye

r 0

Out

er

maybe due to cabling mistaken (fiber swap)

SCT Module Efficiency

Page 15: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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layer 1 Outer layer 1 Inner

Mean : 0.025 mm

Sigma : 0.074 mm

Mean : 0.017 mm

Sigma : 0.090 mm

3. Track Residual

With perfect alignment MC simulation

Mean : ~0.00 mm Sigma : ~0.050 mm are expected.

The real data with no alignment shows good agreement with MC simulation

Real data with no alignment

Page 16: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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(mm

)

laye

r 0

Inne

rla

yer

1 O

uter

laye

r 1

Inne

r

laye

r 0

Out

er

laye

r 2

Out

erla

yer

2 In

ner

laye

r 3

Out

erla

yer

3 In

ner

(mm

)

laye

r 0

Inne

rla

yer

1 O

uter

laye

r 1

Inne

r

laye

r 0

Out

er

laye

r 2

Out

erla

yer

2 In

ner

laye

r 3

Out

erla

yer

3 In

ner

Mean Sigma

Perfect alignment Perfect alignment

Summary of Track Residual

The SCT barrel detector is already well aligned without specific alignment.

Page 17: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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Top scint.

Middle scint.

Bottom scint.

5.54 m

2.19 m

3.86 m

4. Time of Flight Analysis

Purpose

Select high momentum muons for the efficiency and alignment study

• Distance between top and middle scint. is 3.86 m, v=c gives ToF 12.9ns.

Method

Check dependence between ToF and track residual

• Resolution of scintillator is ~ 0.5ns

Page 18: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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ToF between top and middle scintillator

ToF (ns)

We observe residual increase for larger ToF (lower momentum) probably because of multiple scattering effect.

ToF

Residual vs ToF

Page 19: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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Summary

• SCT+TRT barrel cosmic test was performed at CERN in early summer ’06.

• Functional channels are ~99.7 +- 0.03%• This study gives ~99% module efficiency, seems SC

T modules are healthy (in spec).• Modules are well aligned without modules alignmen

t.• ToF analysis gives the possibility to select high mom

entum muons.

Page 20: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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back up

Page 21: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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Layer 0 residual for selected track

layer 0 Outer

layer 0 Inner

Page 22: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

22

Layer 1 residual for selected track

layer 1 Outer

layer 1 Inner

Page 23: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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Layer 2 residual for selected track

layer 2 Outer

layer 2 Inner

Page 24: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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Layer 3 residual for selected track

layer 3 Outer

layer 3 Inner

Page 25: DPF2006 and JPS2006 joint conference  Sheraton Waikiki Hotel, Honolulu, Hawaii October 30, 2006

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ToF between top and bottom scintillator

ToF (ns)

ToF

Residual vs ToF