Difference between revisions of "Mini-prototype"
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===Efficiency -vs- Distance=== | ===Efficiency -vs- Distance=== | ||
| + | The secondary electron beam will be moved towards the drift chamber endplate while the efficiency is measured. | ||
The results of our tests will be placed below. | The results of our tests will be placed below. | ||
==== Plastic feedthrough==== | ==== Plastic feedthrough==== | ||
Revision as of 02:30, 19 August 2007
Drift Chamber prototypes were constructed to evaluate drift chamber designs for CLAS12
Mini-prototype Performance Measurements
Description of General Operation
Chamber Ionization Gas
Our initial plan will be to use (75/25) flowing though the chamber at a flow rate high enough to exchange the volume once a day.
high Voltage supply
A CAEN 4 channel high voltage supply (N470) will be used to supply HV to the drift chambers. The supply is capable of monitoring currents at the microAmp(A) level and voltages at the Volt (V) level.
Signal Processing
The output signals from the drift chamber will be processed through several
NIM based modules.
Dan or Phil: Insert specs of amplifier needed to see DC signals
A descriminator from Lecroy whith a threshold range from 30 mV up to 1.5 Volts will be used to create a stop pulse for TDCs that are started by scintillators which detect either an electron, during tests at the IAC, or cosmic rays, during tests at the LDS (see below). Hall B has loaded the ISU group a TDC module for the drift chamber studies. Pulse height studies may also be done using an ADC. The DAQ system to manage the signal processing electronics is described below.
DAQ System
The DAQ system is described here
Cosmic tests
Apparatus
Place chamber between two plastic scintillator paddles to check signals.
scope pulses
Planned tests
Electron test facility
IAC 25 MeV electron accelerator
The Idaho Accelerator Center (IAC) operates a 25 MeV Linac capable of delivering instantaneous electron currents of 80 mA/pulse. Pulse widths range from 80 ns to 2 s and repetition rates from single shot to 1 kHz. Drift Chamber testing will use this accelerator to create a secondary electron beam as described below.
secondary electron beam setup
Description of collimation system goes here as well as lead pencil target. Description of how beam size will be measured or why it isn't needed.
stepper device
Drift Chamber efficiency measurements
Efficiency -vs- Distance
The secondary electron beam will be moved towards the drift chamber endplate while the efficiency is measured. The results of our tests will be placed below.
Plastic feedthrough
| Distance (mm) | Efficiency |
| 2 | |
| 4 | |
| 6 | |
| 8 | |
| 10 | |
| 12 | |
| 14 |