daniel s levin um/tau/is/ornl meeting with ge sept 27, 2012 university of michigan
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PPS Overview & Experimental Results. Daniel S Levin UM/TAU/IS/ORNL meeting with GE Sept 27, 2012 University of Michigan. Outline. Overview of desired PPS attributes Basic physics of PPS Proof-of-principle experiments & Establishing basic attributes - PowerPoint PPT PresentationTRANSCRIPT
Daniel S Levin
UM/TAU/IS/ORNL meeting with GE
Sept 27, 2012
University of Michigan
PPS Overview & Experimental Results
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1. Overview of desired PPS attributes2. Basic physics of PPS3. Proof-of-principle experiments & Establishing basic attributes4. Laboratory setups and prototype testing
Hit rates with source and background Signals, pixel capacitance, HV, Pashen potential etc Cosmic Muons Saturation measurement Spatial measurements Test Beam
Outline
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Plasma Panel Detector Overview
Inherits many operational and fabrication principles common to PDPs:
• A dense micro-array of gas discharge cells or pixels
• Pixels bias for gas electrical discharge- Geiger mode operation
• Pixels are enclosed in hermetically-sealed glass panel
• Uses non-reactive, radiation-hard materials:
glass substrates, refractory metal electrodes, inert gas mixtures.
Anticipate eventual device fabrication as low-mass detectors
A high gain and inherently digital device
Potential for:
• < 1 ns response times
• high granularity
• Position resolution < 100 um
• low power consumption
• large area with low cost
• 2D readout
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Plasma Television Display Panel (PDP)
As a detector PPS remove or replace specific elements:
No phosphors
No MgO layer
No dielectric layers
We add a quench resistor to the pixels that terminates the discharge
D.S. Levin University of Michigan
Single pixel: Principles of operation
Muon track
(-) High Voltage
cathode
anode
50-100
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Single pixel: Principles of operation
Muon track
(-) High Voltage
cathodeIonizing particle creates ion pair clusters along trackCluster formation dictated by Poisson statistics
Arfor
barcmclusterspairsionprimaryn
en
nP
i
n
i
30~
/!
)(
Cluster statistics: ni= >1 ion-pair. avg is about 3, with long exponential tail
anode
50-100
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Single pixel: Principles of operation
Muon track
(-) High Voltage
cathode
---------
++++++++++
Electron drift & acceleration in initiates avalancheHigh E –fields lead to streamers & gas breakdown according to Paschen’s Law :
P= pressured= gap sizeV=voltagea,b = gas specific parametersanode
50-100
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Minimum voltage occurs when
Wikipedia: Paschen entry.
A.K. Bhattacharya, GE Company, Nela Park, OH Phys. Rev. A, 13,3 (1975)
Small variations in Penning gas mixtures can dramatically affect breakdown voltage
Paschen discharge potential
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discharge cell: important gas processes
primary ionization
metastable generation
Excitation Penning ionization
Image from: Flat Panel Displays and CRTs (Chapter 10) L. Tannas, Jr,
photon emission
Metastable ejection
ion ejected electron
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Rquench
Rterm
Cpixel
Electrical description
During discharge cell becomes conductiveThe E field drops, discharge self-terminates
HV Supply
cathode - + anode
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The quench resistance on each pixel (or pixel chain) : 1) impedes E field rise until ions and meta-stables are neutralized2) maintains HV on all other cells so that they are enabled for hits
signal
start with simplified schematic of single PPS discharge cell
{ResNi}
More realistic cell model
Cpixel
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include stray capacitances, line resistance, self inductance (More details in Robert Varner’s presentation)
Proof-of-principle & other tests with modified PDPs
1. Formation of discharge above Paschen potential2. Self-termination3. Response to a source4. Gas hermetic envelope5. Signal characteristics6. Rate from radioactive source vs background7. Discharge spreading8. Response with various gases9. Detection of CR Muons10. Position sensitivity along a one coordinate axis11. Proton beam tests12. Response to multiple, simultaneous sources
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Yiftah Silver talk
Rout
Quench
50 Termination
Discriminator @ 2-4 V
SnO2
Ni
collimator
22 cm
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Lecroy 574Abandwidth 1 GHz
90Sr106Ru
High Voltage
Panel A: Xe @ 650 torr Filled: Aug 2003
Panel B: Ar + CO2 (7%, 1%)
Lab setup
dielectric
Demonstration using Commercial DC-PDPs
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+ + + + + + + + +
- --Discharge gap
glass
Ni anode 800 m
glass
220-340 m
SnO2 280 m cathodes
E field at pixel (COMSOL calculation)
At critical (Paschen) voltage (~700 V) discharges appear in Xe.
O(ns) rise time (for ~ 1 mm dimensions)
Large amplitude indicates discharge of 5-10 pf effective capacitance
Increase voltage amplitude increase & hit rate increase (next slide)
Observed signals are single pulses quenching works
Panel filled and sealed in 2003- gas containment works
Clear response to 90Sr (beta) source
Low discharge spreading: 2% to a single neighbor pixel in open structure
Signal from Xe filled panel
Signal (attenuated) from Ar-CO2 filled panel
proof-of-principle tests
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Rate Measurements using source
Rate increases as expected with HV Response to source is ~100 Hz with very low background
Response to Source vs HV
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Rate Measurements using source
Rate increases as expected with HV and depends on Quench resistanceHigh Rquench (high RC time constant) causes pixel to saturate
Response to source is ~100 Hz with very low background
Rquench
Response to Source vs Rquench
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1/Rquench
Detection Setup of Cosmic Ray Muons
PMT1PMT2
Panel tested with CF4 or SF6 at 600, 200 torr
Events triggered with 3-fold coincidence
Signals collected with DRS-4 fast waveform digitizer
Scaler & waveform digitizer
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Both pure CF4 and SF6 gases shows a signal with a very fast response time.
Arrival time is defined with respect to the hodoscope trigger
Timing jitter is 5 ns
Arrival Time Measurement of Cosmic Ray Muons
20
About 8% of triggers were associated with signal from the panel
This factor represents a convolution of several factors:
Geometric acceptance ion-pair probability intrinsic efficiency
net = Ag AE P(l,p,r) (r) = 8 %
Ag = geometric acceptance of pixel (wrt to trigger area*solid angle)
AE = Pixel area enhancement from fringe E field P(l) = Probability to produce at least one ion-pair at distance R
from anode (r) = efficiency: probability to generate a discharge for ion-pair
created at distance R from anode.
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Detection of Cosmic Ray Muons & Efficiency
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Response to two simultaneous sources (setup)
D.S. Levin University of Michigan
Side view
Sr90 top
Ru106 bottom
Top view
HV=815VRO lines
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RO 24
RO 1
HV lines 1 20 100 110 128
Pickoff card100x
attenuation
HV=815VR=400
MΩ
VPA 600 Torr Ar 99%CO21%Filled Feb 15, 2012
Discriminator
-150 mVOR Scalar
Ru106
Sr90
RO lines 3-6
Expectation: rate with two sources = sum of the two rates in single mode until the sources starts (partially) overlapping
Response to two simultaneous sources (setup)
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Response to 2 simultaneous sources (Results)
Result: Panel responds independently to each source until they nearly overlap and saturate a line
Summary
Using off-the-shelf commercial Plasma Panels we have demonstrated
Producing fast, self-terminating, high gain pulse
Sensitivity to charged particles betas (also muon, protons)
Good timing jitter using triggered muons
Sensitivity to independent sources
Spatial resolution commensurate with the high granularity of the electrode pitch (Yiftah’s talk)
Panels sealed with gas in 2003 produce signals 9 years later
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