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Cerenkov detector calibrations

Cerenkov detector calibrations

There are two part of Cerenkov detector calibrations: The goal of the amplitude calibrations is to link the measured amplitude in channels to the total number of photoelectrons detected in PMTs.

The goal of the time calibrations is to define for each channel the factor, linked the measured TDC in channels to the value in nsec, and to define the time delay constants, so that the measured time for electrons from the target to the Cherenkov detector will be the trajectory length divided by light velocity.

Amplitude calibrations

The amplitude in photoelectrons is calculated by

A_phe = (A_ch - A_pedest)/A_ope

where A_phe is a number of photoelectrons, A_ch is a measured amplitude in channels, A_pedest is a pedestal value, A_ope is a amplitude in channels for one-photoelectron peak. All values are specific for each PMT

So, to make calibrations, we need to define A_pedest and A_ope.

Pedestal calibrations

Pedestal calibration procedure is a part of pedestals calibrations for all detector groups, - CC, SC, EC and LAEC. There is a special pedestal run, it should be performed and analyzed at the beginning of every new run period, at the end of whole run period, and once per 1-2 weeks otherwise. Before starting this special run you need to check that HV is ON and HV settings are correct.

After this special run is performed, you need to analyze it, using program PEDMAN

To ana-Lise it, you have to

One photoelectron amplitude definition.

To define the position of the one photoelectron peak, you need to proceed another special run. You need not any beam, but it will be best if you'll have the working magnetic field, standard HV setting must be ON. Single photoelectron amplitude calibration is a unique procedure, used for CC only. The idea is to use self-triggering of Cerenkov detector to see the noise function and to define the position of ONE photoelectron.

To take a CC_CALIB run usually takes ~40 min with typical event rate about 10000/sec.

After the end of the run you'll have about 3 files on /raid/stage_in with names clas_cc_XXXXXX.A0Y, where XXXXX - run number, and Y = 0,1,2

To analyze this runs, you'll better copy them from /raid/stage_in to some work disk, say /work/clas/disk2. To measure the SPE positions we need simply to fill ADC distribution histograms for every PMT. It is possible to do that by any program, say RECSIS, but it takes a lot of time. Simplified code to do that was written and checked under cvs in the cc_cal directory.

The (good) example of ADC distribution is shown here:



This peak can be fitted by simple Gaussian, and the position of this peak is One-Photoelectron position.

Unfortunately, there are some channels, where apart from Gaussian you see the noise , exponentially decreased with A, but visible. Those channels need to have some special fitting, using both functions to extract the OPE values. ( Ask Mauri ;-)

Time calibrations

There are two parts in the time calibration:

T1 calibrations

Program to analyze the run is in CLAS standard place under cvs in the utilities/TDC_cal directory. So you need :

T0 calibrations

Recently the CC package was rewrote in order to use the time information from CC properly.

There are no standard procedure under cvs for T0 calibrations. ( Under way )

Here are the steps needed to make this kind of calibrations:


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