Mathieu Benoit

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Occupancy studies for CLIC_ILD inner layer and Update on Digitization : Tuning with data, Lorentz angle effects. Mathieu Benoit. Outline. First results on Occupancy for the inner layer of CLIC_ILD Following design from workshop - PowerPoint PPT Presentation

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Occupancy studies for CLIC_ILD inner layer and Update on Digitization: Tuning with data, Lorentz

angle effects

Mathieu Benoit

Outline

• First results on Occupancy for the inner layer of CLIC_ILD Following design from workshop

• Inclusion of Magnetic Field effects in Digitization

• DESY 2-4 GeV electrons data using Timepix single chip card

(sub) Barrel 0 orLeft Outer barrel

(sub) Barrel 1 orLeft inner barrel

(sub) Barrel 2 orCentral barrel

(sub) Barrel 3 orRight inner barrel

(sub) Barrel 4 orRight Outer barrel

Simulation• For Now simulation of layer 0+1, results here for layer 0 , the most critical at r=29

mm• Simulation with Livermore Low EM Physics list

– Max Step-size in Silicon =1 um– Include detla rays , fluorescence

• Geometry : – Magnetic Field = 4 T– Berylium beam pipe (600um)– Inside beampipe : air at 1 e-2 bar

• Timepix-Like digitization– 20x20um pixels– 50 um thickness– Resistivity = 10 kOhm cm– Threshold = 500e

– Lorentx angle not taken into account here

• Plots are preliminary, need to include actual gap in phi – Module 90 (top right) missing, being processed

mini workshop on engineering aspects of the CLIC vertex detectors

5

Barrel layout (layer 0+1)

• To ensure hermeticity, layer 0+1 need to be placed closer to IP than MC model– Option 1:

• Radius(layer 1) = 29 mm (31mm before)• Radius(layer 2) =30.87mm (32.87mm before) • To avoid volume overlap, slightly tilt the ladders (here 1.5°)

– Option 2: • Tilt sensors by lorentz angle (ex: 15 deg)• Add 1-2 ladders (here , 2-> Icosagon !)• Move back to larger radius (here 31.221 mm)

15/03/12

mini workshop on engineering aspects of the CLIC vertex detectors

6

Barrel layout (layer 0+1, option 1)

An option to option 1: Shifting layer 2 vs layer 1 (here 1mm), ladder per ladder to avoid overlapping gaps

Single hitsDouble layer, holding on the same mechanical structure not shown here

15/03/12

Event Display (1k primary tracks)

HitMap in Layer 0

Hitmap Layer 0 (per Train per Chip)

Occupancy per module in layer 0%

Occupancy per module in layer 0 (polar view)

%

Cluster size subbarrel 0 layer 0

Cluster size subbarrel 1 layer 0

Cluster size subbarrel 2 layer 0

Cluster size subbarrel 3 layer 0

Cluster size subbarrel 4 layer 0

HitMap in Layer 1

HitMap (per Train per mm2)

Occupancy per module in layer 1%

Occupancy per module in layer 0 (polar view)

%

Cluster size subbarrel 0 layer 0

Cluster size subbarrel 1 layer 0

Cluster size subbarrel 2 layer 0

Cluster size subbarrel 3 layer 0

Cluster size subbarrel 4 layer 0

Occupancy Simulation

• 2 Scenario : – 20 um pixels, same geometry + B-Field effect, layer

0-5

– 25 um pixels, layer back by 4mm in r + B-field effects layer 0-5

• In both scenario we need to add hadronic components, disks

mini workshop on engineering aspects of the CLIC vertex detectors

27

Lorentz angle• Lorentz angle depends on mobility which depends on Electric

field and eventually on dopant concentration

• In a 50um 10kOhmcm p-type wafer, 10V bias, E≈[1600,2700]V/cm– Vary with resistivity, bias voltage

• In a planar sensor, E is proportional to V applied– V applied is proportional to thickness2 (Full depletion voltage)– For thin sensor, at full depletion voltage, Electric field is very low– To be investigated : How much over Full depletion can we apply voltage

15/03/12

Lorentz angle effects in Digitization

• I have added as an option in the digitizer to tak into account the Magnetic field in the motion equation of the charge in the sensor.

– The Lorentz angle is calculated at each integration step taking into account :• Local mobility and electric field • Hall Scattering factor

Lorentz angle effects (0 degrees incidence, B=4T)

Lorentz angle effects (75 degrees incidence, B=4T)

Lorentz angle effects (0 degrees incidence, B=4T), tilted by Lorentz angle

Lorentz angle effects (0 degrees incidence, B=4T), tilted by Lorentz angle

Lorentz angle effects (Cluster Size)

!!

Lorentz angle increases cluster size (in average) -> Increase occupancy

DESY data with low energy (2-4 GeV) electrons

• We were allowed to join ATLAS DBM testbeam at DESY to acquire some data with Timepix using low energy electrons (2-4 GeV) (No Tracking)– 6M Frames at 100V 0 deg– 5K Frames at 0,25,50,75 deg– 5k Frames at 0deg, 5V, 10V, 50V– 5k Frames at Ikrum 25,50,100

• In average 500 clusters per frame• ToT mode

Some DESY plots (cluster size)

Some DESY plots (cluster size)

Conclusion

• Detailed simulation of inner layer for CLIC_ILD new design show higher occupancies than CDR numbers : – Layer is 4 mm closer than before -> Higher occupancy– Phi dependence observed in the end-of-stave chips– Next simulation to be perfomed with B-Field effects included,

larger pixels

• Lorentz angle effects have been encoded in the digitizer– Debugged using the new event display feature of the digitizer– Ready for use in occupancies studies