Difference between revisions of "First look at TOF calibration"
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*# for each event plot for each paddle in plane k: <math> MT^{n}_{plane k} + MT^{i}_{plane j} </math> | *# for each event plot for each paddle in plane k: <math> MT^{n}_{plane k} + MT^{i}_{plane j} </math> | ||
*# [[File:example_mtdiff.gif|400px]] | *# [[File:example_mtdiff.gif|400px]] | ||
+ | *# and after using the correction timing conversion: | ||
+ | *# [[File:mantimediff_goodtiming.png|400px]] | ||
*# fit the meant time peak of each projection: | *# fit the meant time peak of each projection: | ||
*# [[File:Fit_projection_example1.gif|400px]] example 1 | *# [[File:Fit_projection_example1.gif|400px]] example 1 |
Revision as of 08:38, 17 April 2015
First Look
- first select data sample with the following conditions:
- only consider hits within 50ns of the timing peak both for ADC data and TDC data
- only consider paddles that have hits on both ends
- take care of the 6fold trigger timing shift in the TDC (24ns window)
- Do a rough determination of the walk correction by using the time in the ADC as reference.
- Do mean time comparison between different planes
- calculate MeanTime of Paddle i in plane j:
- calculate MeanTime for all Paddles n in plane k:
- for each event plot for each paddle in plane k:
- and after using the correction timing conversion:
- fit the meant time peak of each projection:
- example 1
- example 2
- Do this for each paddle in the first plane as reference paddle.
- Choose one paddle in the first plane as THE REFERENCE PADDLE
- Calculate the difference between the fit results of each paddle in the first plane w.r.t. THE REFERENCE PADDLE and fit the distribution
- average difference of mean time to REFERENCE PADDLE
- Now we have offsets for the Mean-Time for all Paddles w.r.t. THE REFERENCE PADDLE
- Do time difference comparison of one paddle with the paddle number in the other plane
- calculate time difference:
- plot this time difference vs. paddle number of paddles that got hit in the other plane
- again look at each projection and fit the peak
- example fits
- now one can also plot the fit results as a function of paddle number. The inverse slope is the speed module paddle pitch
- one can also plot the difference between symmetric paddles around the beam hole
- choose the intersection at zero for the time difference offset
- Now we have offsets for time difference (TD) and mean time (MT)
- offset for the left pmt:
- offset for the right pmt:
- as a bonus we get the effective speed of light for each paddle.