Mini-prototype

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 [math]ArCO_2[/math] (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([math]\mu[/math]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. We will use the large area 7 cm by 50 cm paddles with the Russian PMTs operating at 1300 V and threshold > 150 mV to select on energetic cosmic rays. We will arrange the paddles so that the are perpendicular to one another so that looking from above it will have 7 cm by 7 cm overlap. This will allow for testing the chamber along its length

scope pulses

Tony, what do you mean by scope pulses??

Planned tests

We will use the scintillator paddles with cosmic rays.

Tests:

1. Efficiency along length of chamber with overlapping array of scint. paddles optimized for normal incidence. 2. Efficiency as a function of discriminator threshold, i.e. what is the required energy of the cosmic ray. 3. Efficiency as a function of angle. Count rates will decrease so we will have to determine the best overlapping configuration of the paddles.

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 [math]\mu[/math]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

We will need to bring the electron beam to the experimental testing cell. [Picture of IAC here].

We will need to butt an evacuated pipe from the business end of the LINAC to the collimator entrance at the wall. Cole will be responsible for the design and safety concerns of implementing the pipe. The wall is 8' thick, which is 6' of packed earth sandwiched between 1' of concrete on either side. Upon he electron beam will travel 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.

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