University of Iowa
-
Upload
jacqueline-chapman -
Category
Documents
-
view
23 -
download
0
description
Transcript of University of Iowa
![Page 1: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/1.jpg)
Slide N 1
University of Iowa
HF sourcing – Histograming mode
Alexi Mestvirishvili
ECLIPSE 06Antalya, Turkey
![Page 2: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/2.jpg)
Slide N 2
HF minus
Ten 10o sectors – 28 – 36 and 1 analyzed so far
Signal+Pedeatal
QIE counts vs position
Expected signal – 0.01
Main calibrationHTR running in histograming mode, QIEs running in normal scale. Reading out of one spigot at the time (24 channels, 12EM, 12HAD)During sourcing source was stopped in three different location First and last – for safety reasons. Second stop for 3 minutes – to accumulate data. Position of second stop point was chosen in the way to have both long and short fibers illuminated.
x10
![Page 3: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/3.jpg)
Slide N 3
Signal + pedestal and pedestal separation and signal versus tower
EM fibers
HA fibers
Small peak – pure pedestalHigh peak – Signal+pedestal
Gaussian fit applied
For these distributionsare 0.0018.
5 wedges 24 tower each
![Page 4: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/4.jpg)
Slide N 4
Problems
Gaussian fit sigma for S+P vs Tower
EM channels
HAD channels
Run 1566 & 1567Tower 12, phi 36Run 1490
Tower 23, phi 33
![Page 5: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/5.jpg)
Slide N 5
Problems (run 1566)
Red signal + pedestalGreen pedestal
Four different capacitors
![Page 6: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/6.jpg)
Slide N 6
Calibration Precision
Calibration precision is limited by several factor
1. Statistical precision of signal (relative error on signal)
2. Pedestal stability
3. Internal nonlinearities of absorber and fibers (believed to be at the level 5%, not studied for this presentation)
4. etc.
![Page 7: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/7.jpg)
Slide N 7
Statistical PrecisionPhi=29, tower=16, QIE ch 2,8
a) b)
a) Signal + pedestal Nentries = 14290Mean = 5.05Sigma = 0.0018Err on Mean /sqrt(Nentries) =1.5x10-5
b) PedestalNentries = 3408Mean = 5.039Sigma = 0.0018Err on mean = 3x10-5
= 5.05 – 5.039 = 0.011 = 3.3x10-5
X axis units – linearized QIE counts
/=0.3%
![Page 8: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/8.jpg)
Slide N 8
Relative error on signal
Small towers has smaller signals hence big error
![Page 9: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/9.jpg)
Slide N 9
Pedestal stability
Pedestal stability can be studied from same data. In one 10o
24 channels (12EM, 12HAD) are read out during sourcing ofone tube. Either 16 or 15 tubes are in one phi sector. In eachrun only two channels (1EM, 1HAD) caries signal. All otherchannels gives pure pedestal, provided adjacent towers of one which is sourced are excluded from data samples
One can easily select samples for the same channel and wellseparated in time. App 5 minute is necessary to source onetube. For example, two samples for tower 5, when source is in tube 1 (tower 1) and in tube 16 (tower 12) are separated by more than one 1 hour.
![Page 10: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/10.jpg)
Slide N 10
Pedestal stability
1,1,,1,1, kkkjjji
– tower for which pedestal is determined
– towers which are sourced, they are
separated in time as far as possible
ikj,
Condition which has to be fulfilled to avoid contributionFrom energy leakage from tower to tower
Measure of pedestal stabilityis width of pedestal distribution ij, ik
![Page 11: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/11.jpg)
Slide N 11
of pedestal distributionstower 1 to 12
Tow 12,=36
Smallest tower Is noisy as well
![Page 12: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/12.jpg)
Slide N 12
of pedestal distribution
towers 13 to 24
Tow 12,=36
Small tower noisy as well
![Page 13: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/13.jpg)
Slide N 13
Geometrical corrections
Geometrical corrections has to be applied to signals from each tower to exclude the differences in towershape.
Coefficients were taken from Monte Carlo. They arecalculated with respect to the response of infinitesize tower taken into account actual tower geometry
Coefficients are available in HF monitoring databaseand they were calculated in CMS IN 2004/002
i
iicorr GC
SigSig ,
![Page 14: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/14.jpg)
Slide N 14
Geometrical correction how they work (problems ?)
for HAD towers
for EM towers
High Medium Low
PMT gains
Gains in each groupare more or less equal
Uncorrected, pedestalsubtracted signal forphi = 28
For towers having two source tubes geometrical correction should bringtwo points close to each other
![Page 15: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/15.jpg)
Slide N 15
Geometrical corrections how they work (problems)
pedestal subtracted,Corrected,
signal for phi = 28
Same as on previous slide
High Medium Low
PMT gains
Points in red ovalsmove in oppositedirection
Points in last groupbehaves as it should
![Page 16: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/16.jpg)
Slide N 16
SUMMARY
1. In general, data quality is good, signal can be separated well even for small towers2. Statistical precision of HF calibration will be very high, less than 1%. 3. Stable pedestal4. Some problems were identified – bad capacitors, noisy channels5. Geometrical scale factors has to be recalculated with correct tower geometry (!!!!!!!!!)
![Page 17: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/17.jpg)
Slide N 17
Backup slides
![Page 18: University of Iowa](https://reader030.fdocuments.us/reader030/viewer/2022033108/56812bba550346895d8ffca3/html5/thumbnails/18.jpg)
Slide N 18
Stability of pedestal Mean
RMS = 0.00046 RMS = 0.00034 RMS = 0.00027 RMS = 0.00034
),min( ijik MM
MM ikij – tower for which pedestal is determined
– towers which are sourced, they are
separated in time as far as possible
ikj,