A Prototype Diamond Detector for the Compton Polarimeter in Jefferson lab, Hall C - PowerPoint PPT Presentation

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A Prototype Diamond Detector for the Compton Polarimeter in Jefferson lab, Hall C

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... chose Diamond (artificially grown by Chemical Vapor Deposition) for the detector ... (tail truncated) to avoid overlapping of signals coming one after the other. ... – PowerPoint PPT presentation

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Title: A Prototype Diamond Detector for the Compton Polarimeter in Jefferson lab, Hall C


1
A Prototype Diamond Detector for the Compton
Polarimeter in Jefferson lab, Hall C
Medium Energy Physics Group http//ra.msstate.edu/
dd285/mep.html
Amrendra Narayan Mississippi State University
JLab, Hall C, Compton Polarimeter Collaboration
2
Outline
  • The Compton Polarimeter
  • Diamond as a Detector
  • Electronic Setup
  • Preliminary Results
  • Future Tasks

Thanks Few Slides adapted from the talk of Roger
Carlini
3
The Compton Polarimeter
A high precision Compton Polarimeter is under
construction at Hall-C for a non-destructive
continuous monitoring of the e- beam polarization
during the Qweak experiment and all other
polarized e- scattering experiments to follow
after the upgrade to 12 GeV capacity.
4
Diamond A Closer look
Silicon is a typical choice for a multi-strip
position sensitive electron detector
Advantages lower leakage current, faster, lower
noise and rad. hard
Disadvantages smaller signal 40 smaller
Thanks Dr. R. Wallny (UCLA)
5
The Diamond Detector
  • Diamond is known for its radiation hardness
  • We chose Diamond (artificially grown by Chemical
    Vapor Deposition) for the detector

How does it work?
  • Operation of Diamond Detectors
  • Bias voltage 1000 V,
  • Charge collection distance 250m

6
A Prototype Diamond Detector
  • 10x10 mm2
  • 500 µm thick
  • 15 strips 450 µm wide

Metallization, Lithography wire bonding done in
High Energy Physics Lab at Ohio State University.
Thanks Prof. Harris Kagan and his group at OSU.
7
Schematic of the Electronic Setup
Timing signal created only for signals gt
V_threshold
Analog to Digital Converter Histograming of the
digital signal
Charge pulse converted to a voltage signal and
amplified
The raw signal, a charge pulse
Signals accepted only in co-incidence with the
signal from timing filter amp
Timing Filter Amp
Ortec 928
Pre- amp
Linear Gate
MCA
Electron detector
Discriminator
Ortec 926
MPR - 16
STM 16
The signal is shaped (tail truncated) to avoid
overlapping of signals coming one after the other.
Shaping Amp
Visual display
counts
Channel number
A typical display
8
Spectrum obtained by the Diamond detector
Threshold Voltage was low 50 mV
Shaping Amplifier _at_20 gain
9
pedestal suppressed  spectra from diamond
threshold set to 150 mV to suppress the background
10
Triggering with a Scintillator
Measuring only the minimum ionizing particles.
Only those beta particles would be detected which
pass the detector and reach the Scintillator.
11
Schematic of the Electronic Setup
Analog to Digital Converter Histograming of the
digital signal
Charge pulse converted to a voltage signal and
amplified
The raw signal, a charge pulse
Signals accepted only in co-incidence with the
signal from Scintillator
Ortec 928
Pre- amp
Linear Gate
MCA
Electron detector
Discriminator
Ortec 926
MPR - 16
The signal is shaped (tail truncated) to avoid
overlapping of signals coming one after the other.
Shaping Amp
Visual display
counts
Channel number
A typical display
Instead of Self-trigger, we are now triggering
with the Scintillator
12
Calibrating MCA
For Silicon dE/dx 1.664 MeV/(g/cm2) ?
2.33 g/cm3 Energy per e-h pair 3.6 eV
Thickness of the Si detector 300 µm
The mean Energy deposited then comes out to be
116.31 keV
Corresponds to
32310 e-h pairs
From particle physics data book
13
Triggering with a Scintillator
Only those beta particles would be detected which
pass the detector and reach the Scintillator.
Measuring only the minimum ionizing particles.
14
Response of the Diamond Detector
For Diamond ? 3.5 g/cm3 Z/A 0.499
Energy per unit e-h pair 13 eV
Positive bias
Counts
The Mean of 852 MeV
Channel
With the calibration by Si Corresponds to
Mean 708
4742 e-h pairs (expect 9000 e- for 220 µm CCD)
Negative bias
A 220 µm CCD was measured for this diamond with
a metalized dot
15
Next Steps
  • Repeat the measurements in a real electron beam
  • (Detector has been shipped to TRIUMF, tests
    scheduled for mid-June)
  • Build the full size Diamond Detector
  • (4 planes, 21 x 21 mm2, 200mm pitch)
  • An order for 4 planes placed with E6, delivery
    expected in 2 weeks.
  • Quotes obtained from an E6 Spin-off to do
    metallization, the same company has expressed
    interest in making the carrier plates and doing
    the wire-bonding (turn key detector).
  • Build the read-out electronics
  • Build the DAQ
  • Mississippi State Univ., Univ. of Winnipeg,
    Univ. of Manitoba, TRIUMF

16
THANK YOU
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