new ionization chamber technology
DESCRIPTION
NEW Ionization Chamber Technology. Anne Dabrowski Results on behalf of Mayda Velasco’s Hardware Research group . P. Ball 3 , A. Darowski 1 , G. Graham 3 , C. Kendziora 2 , F. Krueger 2 G. Tassotto 2 , G. Ünel 1 , M. Velasco 1 - PowerPoint PPT PresentationTRANSCRIPT
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NEWNEW Ionization Chamber Technology
Anne Dabrowski
Results on behalf of Mayda Velasco’s Hardware Research group.
P. Ball 3, A. Darowski 1, G. Graham 3, C. Kendziora 2, F. Krueger 2
G. Tassotto 2, G. Ünel 1, M. Velasco 1
1 Northwestern University,2 Fermilab,3 Richardson Electronics
Lunch Bag Seminar 1 May 2002
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Why the need for new Hardware?
• Modern High Energy Experiments – High intensity beams > 1011 particles/ micro
second– Radiation Hard– Once-off calibration– Monitor beam line position / background
particle flux
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• Solution:– Ceramic radiation hard ionization chambers.
– Either Gas sealed or Vacuum – SEM (secondary
emission monitor)
Q = I * d * e*A * n * M current read by chamber
I – beam intensity (cm-2 s-1) (<1011 cm-2 s-6)
d – gap size (cm) (~1mm)
e – electron charge
M – multiplication factor (~1)
N – tot num of ion/electron pair/cm (8 for He at atm 98 for Ar at 1 atm)
A – elecrode area (cm2) (1 cm2)
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Basic Description of Design
• Chamber filled with Gas -- Ionization SIC (< 1011/p/cm2/s)• Chamber in Vacuum -- Secondary Emission Monitor SEM (above 1010 /p/cm2/s)
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Basic Chamber Design
•Fixed volume, Temperature and Pressure changes do not affect calibration•Radiation Hard Materials (> 1010 Rads) – Ceramic (AL2O3, 94%, 96%) – Kovar (nickel, iron, cobalt)
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Engineering drawing
Tolerances:
•Gap = 1mm +/- 0.001”
•guard-to-collector = 0.5 mm+/- 0.002”
•Flatness 0.001”
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SIC prototypes
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Timeline for Design Development• 2000 Richardson Electronics (REL) made Glass Chambers
(Inspired by V. Falaleev Design). – Detection observed– Design studies– Change to ceramic because of high tolerances
• Ceramic design – Electrode changed from round edges to edges square D1 – D2– Flat for signal collector & guard ring.
• Multiple chambers produced (7 in all)– gas refilling tested.– Found occasional shorts on due to metal filings inside the chamber…
tooling redesign.
• Believe have the final design– (testing by producing several chambers….already under construction).
• successful– mass production will start at the rate of 10 chambers/week.
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How do they Behave ?
Electron SourceI ~e8 - e9
ATF(BN L)
Photon Em ission424 R /hr
R adiation C alib ration Facility(FN AL)
Proton Source1e11 - 1e12
Booster(FN AL)
P rev iew T E S T IN G fac ilities
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Radiation Physics Calibration Facility (RPCF)
Photon Emission 424 R/hr
• Check chamber quality– Plateau, ionization response, reproducibility
• Lead to design improvements
• Determined operational modes– operational voltage, gain voltage, gas type
• Do pre-calibration before operating in other facilities.
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Radiation Physics Calibration Facility (RPCF,FNAL)
“Flat mounting”
“Side Mounting”
•Two new Cs137 sources:
•Max:1600 Rad/Hr
•The old source was
•424 Rad/Hr
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Results (RPCF)Note Slope !!
Electrode edges
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What Changed?Design 1 vs. Design 2
The electrode edge … Curved Flat
Effected slope of plateau … reduced by ~ 70 %
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Results D2 vs. D4 Signal
> Electrode area
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Setup to test chambers at the RPCF– pre-calibration for all SICs
•Investments: A Keithly
electrometer
•Sensitivity 2 nC
•Resolution of 0.1 pC
•Bias current of < 3fA
•Output of electrometer via GPIB to computer running LabView to a data file.
•Procedure almost automatic Good for grad students when calibrating in the summer
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Chamber Characterization show no radiation damage after XX protons
Chamber filled withHe for more than a year
No change…
Reproduce calibrations
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Summary of RPCF Results:
• Good reproducibility
• Can measure both small and large currents.
•Keithley Electrometers and Powers Supplies allows to do good measurements of knee of plateau need to test gas quality of chambers… no degradation see so far.
•LABview DAQ – user enter customized measurement parameters – automated DAQ
•Slopes good – but not quite flat… we believe we understand it.
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Tests at ATF (BNL) low energy electron
beam No saturation below 8*109/p/cm2
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Booster (FNAL) proton source ~1e9 to 1e12
Old Toroid only for Flux measurement
New Toroid +chamber for Flux measurement &
Longitudinal movement for alignment
SIC Only1mm Wire Chamber & SIC
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Booster (FNAL) HaloHigh intensity ~ 1e9 proton source
1.5 s per spill … halo see 1/100 of total beam
ONLINE OFFLINE
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Booster (FNAL)Plateau in the beam (1.8e11)---saturation (same effects present with design 4) shortens plateau—space charge
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Booster (FNAL) – Intensity Scan
SEM-like SIC-like
No saturation even At 1012 ppp(10-5 torr)
Clear …Saturation
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Of the beam
Beam Moved
Need to repeatWith vertical movement
Beam Profile fromWire chamber
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Summary of results from Booster Saturate above e11 in SIC-mode, but no
saturation in SEM-mode.
• When making plateaus: gain observed at 200 V in the beam center, but not seen at 350 V in the “halo” like in the RPCF tests
• use SWIC electronics for both low and high currents just change capacitors
• So far no signs of radiation damage … or helium leakage
• To do… add vertical movement to get proper alignment.
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Secondary Emission Monitor– SIC chamber in vacuum
•Getter - Place a strip of barium under the collector and activate it at about 1000 degree C.
•Ion Bombardment - Apply a voltage across the electrodes while pumping for reducing atmosphere of H2.
–Richardson used this process on vacuum tubes to 10-8 torr
This look like a very promising way of operating The chambers for >1011 ppp
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Permeation Test– test run for 3-4 days … Helium is not leaking….
• The ion chamber was then put in side of a small vacuum chamber and tested using a Dupont Mass Spectrometer leak detector the total leak rate was found to less than 2X10 –10 STD CC P/S.
• Then the temperature was raised slowly to 100 degree C.
• Max leak rate < 40X10 –10 STD CC P/S
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Conclusion
Believe to have a working design that can be operated at :
• I<1011 ppp in SIC-mode• I>1010 ppp in SEM-mode
200 chambers to be build with the new tooling design.