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Pixel Detector Simulation with Magnetic Field

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JC and Marina 12/18/00 Pixel Detector Simulation with Magnetic Field Effects with magnetic Field Deflection Effective mobility Non-constant Hall mobility – PowerPoint PPT presentation

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Title: Pixel Detector Simulation with Magnetic Field


1
Pixel Detector Simulationwith Magnetic Field
JC and Marina 12/18/00
  • Effects with magnetic Field
  • Deflection
  • Effective mobility
  • Non-constant Hall mobility
  • Comparison with magnet run

2
Magnetic Field
3
Deflection in Magnetic Field
Effect of magnetic field ? Effect of
incident angle
4
Deflection in Magnetic Field
Assumption mH constant meff m
The charge distributions are the same with B or q
5
Effective Mobility
  • Very small effect
  • B field ? Cloud drifts slower ? Larger Spread

6
E-dependent Mobility
Larger E ? Smaller mHall?? ? Smaller deflection
7
Effect of Magnetic Field
  • With non-constant mHall(E), and meff

The charge distributions are slightly different
8
Conclusion
We Dont expect the magnetic field will reduce
the ratio between two-pixel clusters and
one-pixel clusters
9
Magnet Run
  • Track at 1.3? angle ( 0.242 Tesla )
  • Measurement Rmin 0.193
  • Simulation ( Qth 2.5Ke ) Rmin 0.250

What is wrong ?
10
Magnet Run
Just to Play around
  • Track at 1.32? ( 23 mrad ) ( 0.245 Tesla )
  • Measurement Rmin 0.193
  • Simulation ( Qth 4.0Ke ) Rmin 0.197

But there is no other evidence that threshold was
wrong
11
Magnetic Field
  • Measured with Gauss meter 45A ? 0.585 Tesla
  • Assume overall scale of the magnetic field
    uncertain
  • Use MC simulation to fit ? 0.517 Tesla (error?)
  • Error of Hall factor (mHall/m 1.15) can make up
    the difference

12
Summary
  • MC simulation accurate both for drift and B
    field simulation
  • Magnet Run data is not fully understood yet

13
Lorentz Angle
  • Lorentz angle is not a constant along z,
    shown are overall effects
  • Larger bias voltage
  • ? Larger E field
  • ? Smaller mobility
  • ? Smaller Lorentz angle

14
Lorentz Angle Comparison
Magnetic field 1.4 Tesla Udepletion is
calculated with effective thickness of the sensor
15
Diffusion Constant
Einstein equation D k T m / q
  • Reduce Teff from 390K to 300K
  • ?
  • Reduce fraction of doublet by 1.4

16
Angular Fit with ? Distribution
FPIX0-Pstop Normal Incidence Data
  • MC 0.5? interval, interpolation between
    points
  • Normal incident data ? (1.77 ? 0.09)?

17
Angular Fit with ? Distribution
FPIX0-Pstop
18
Detector Inclination Angle
  • In Minuit fit, the beam is assumed to normal
    incident on the first SSD, the overall rotation
    of the detector can not be fitted
  • In ? fit, interpolation between MC points (0.5
    interval) is used
  • The error from the fit is about 0.1, which
    should be smaller than error from MC model
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