mm gain measurements with mbt3/4 chambers
DESCRIPTION
MM Gain measurements with MBT3/4 chambers. By using an MiniX -Ray Gun (Ag), we want to measure the gain in the MBT3 and MBT4 chambers used in ATLAS during 2012 run. - PowerPoint PPT PresentationTRANSCRIPT
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MM Gain measurements with MBT3/4 chambers
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MM Gain measurements with MBT3/4 chambers
• By using an MiniX-Ray Gun (Ag), we want to measure the gain in the MBT3 and MBT4 chambers used in ATLAS during 2012 run.
• The X-Ray generated by the MiniX-Ray system are more penetrating than the X-Ray produced by the Cu X-Ray gun, this allow us to measure the gain of the MBT3/4 at the same time under different X-Ray flux conditions but with the same environmental conditions.
• We need to estimate the rate of the “primary electrons” generate by the flux of the incoming X-Ray.
• The MMs gain is measured as a function of the HV.
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MBT chambers layoutGas Distribution
HV 9 mm
4.5 mm 4.5 mm
Common Drift Electrode
2 APV card used for each MBT chamber (256 channels).Channels map organized in order to reconstruct X coordinate from 1-200 ch. and V ch. from 201 to 256.
2D Readout system, X and V coordinate
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X-Ray / MM chamber setup
MM
HV Side
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MBT3/4 Scanning conditions
• The chambers were scanned using the MiniX-Ray gun.
• To apply HV on the resistive strips and the drift, the CAEN SY2527 and A1821 boards were used.
X-Ray gun:HV = 30.00kVBeam intensity = 12 microA
HV-resistive strips = +450 to +550VHV-drift = -300V(monitored by power supply)
• Two HV scans have been performed with MBT3 or MBT4 in front of the X-Ray gun.
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Collected DataHV [Volt]
MBT4 (1° chamber) MBT3 (1° chamber)
450 200605 200681460 200606 200682470 200607 200683480 200608 200684
490 200609 200685
495 200610 xxxxx
500 200611 200686
505 200612 xxxxx
510 200613 200687515 200614 200688520 200615 200689525 200616 200696530 200617 200697535 200618 200692540 200619 200693545 200620 200694550 200621 200695
100 K events for each run
Total readout window for run 0.0675 s
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Amplification Current Vs HV
440 450 460 470 480 490 500 510 520 530 540 550 5600
500
1000
1500
2000
2500
f(x) = 0.000742661106903644 exp( 0.0272075724291114 x )
f(x) = 0.000139426197612421 exp( 0.0292224888624651 x )
Amp. Current Vs HV
MBT3Exponential (MBT3)MBT4
HV [Volts]
Cu
rre
nt [
nA
]
440 450 460 470 480 490 500 510 520 530 540 550 560 5700
500
1000
1500
2000
2500
3000
3500
Amplif. Current Vs HV
MBT3 Current
MBT4 current
HV [Volts]
Cu
rre
nt [
nA
]
MBT4 in front to the X-Ray Gun
MBT3 in front to the X-Ray Gun
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Gain MeasurementsG = Cf/ Ci
For a single event we define the GAIN as follow:Cf = Final ChargeCi = Initial Charge
We can extract the total Final Charge from the current delivered by the power supply.
The number of reconstructed clusters (per second) gives us the rate of the converted X-Ray
From each converted X-Ray we expect ~ 500 electrons (13 KeV / 26 eV)
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Initial Cluster selection“ True” Clusters
“ True” Clusters
“ Noise” Clusters
Applied cut “cl qmax>100” andCluster size > 1, to remove noise clusters
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Initial Cluster selection
440 450 460 470 480 490 500 510 520 530 540 550 560 5700
20000
40000
60000
80000
100000
120000MBT3 Cluster Vs HV
MBT3 cl_width>1MBT3 nclu cl_qmax > 100
HV [Volts]
Clu
ste
r [C
ou
nts
]
440 450 460 470 480 490 500 510 520 530 540 550 560 5700
50000
100000
150000
200000
250000
MBT4 Cluster Vs HV
MBT4 nclu cl_qmax > 100
MBT4 cl_width>1
HV [Volts]
Clu
ste
r [C
ou
nts
]
MBT4 close to the X-Ray gun
MBT3 far from the X-Ray gun
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Initial Cluster selection
MBT4 far from the X-Ray gun
MBT3 close to the X-Ray gun
440 450 460 470 480 490 500 510 520 530 540 550 560 5700
50000
100000
150000
200000
250000
MBT3 Cluster Vs HV
MBT3 cl_width>1MBT3 nclu cl_qmax > 100
HV [Volts]
Clu
ste
r [C
ou
nts
]
440 450 460 470 480 490 500 510 520 530 540 550 560 5700
20000
40000
60000
80000
100000
120000MBT4 Cluster Vs HV
MBT4 nclu cl_qmax > 100
MBT4 cl_width>1
HV [Volts]
Clu
ste
r [C
ou
nts
]
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Chamber Gain Vs HV
440 450 460 470 480 490 500 510 520 530 540 550 560 5700
2000
4000
6000
8000
10000
12000
14000
MBT3/MBT4 Gain Vs HV
Gain MBT3
Gain MBT4
HV [Volts]
Ga
in
440 460 480 500 520 540 5600
2000
4000
6000
8000
10000
12000
14000
MBT3/4 Gain
Gain MBT3
Gain MBT4
HV[Volts]
Ga
in
MBT3 close to the X-Ray gun
MBT4 close to the X-Ray gun
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Summary A first MM gain measurement, using Ag Mini X-Ray system as been done with
MBT3/4 chamber. First source of uncertainty for this measure come from the incoming charge
estimation:•Number of conversion for second.•Number of “primary” electrons for each conversion.
A small difference of gain, equivalent to 10 Volts, seems to be present between MBT3/MBT4 ( the effect is more evident in the second scan).
The gain has not been corrected for the possible HV drop as a consequence of the high current generate by the high flux and for environmental variations between the two different scans.
Same measurements can be performed with Cu X-Ray gun, in this case we can study only one chamber for each scan.
Next steps: •Evaluation of the voltage drop effect on.•Gain measurements and characterization as a function of the environmental conditions.•Gain measurements for T and L chambers.