Difference between revisions of "Minutes-7-2-2015"

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# Engineering  
 
# Engineering  
 
# Other
 
# Other
 
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= Minutes =
 
= Minutes =
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- Lubomir presented two slides summarizing the FDC performance for the S&T Review. Comments about efficiency slide - the worst (package #3) is shown; each chamber reconstructs 3D hit which requires hits in both cathodes (with at least 3 strips fired) and the wire plane. Resolution - to show the average wire resolution; discussions about why two methods give different results for the cathode resolution and what is the effect of the multiple scattering. General remark - needs bigger axis labels.
 
- Lubomir presented two slides summarizing the FDC performance for the S&T Review. Comments about efficiency slide - the worst (package #3) is shown; each chamber reconstructs 3D hit which requires hits in both cathodes (with at least 3 strips fired) and the wire plane. Resolution - to show the average wire resolution; discussions about why two methods give different results for the cathode resolution and what is the effect of the multiple scattering. General remark - needs bigger axis labels.
  
- Results with 55Fe source for the avalanche position w.r.t. wire reconstructed from the cathodes. Z (perp. to chamber plane) coordinate calculated from the up/down total charge ratio. X coordinate (in plane perp. to wire) from the crossing of the up/down centroids. After applying centroid corrections and calibrating the channels one can see a hole for the wire and amazing resolution of ~80 microns in X and ~30 microns in Z. Interestingly the avalanche develops at ~130 microns from the wire, while on the drift chamber books one can find values of ~60 microns.       
+
- Results with 55Fe source for the avalanche position w.r.t. wire reconstructed from the cathodes. Z (perp. to chamber plane) coordinate calculated from the up/down total charge ratio. X coordinate (in plane perp. to wire) from the crossing of the up/down centroids. After applying centroid corrections and calibrating the channels one can see a hole for the wire and amazing resolution of ~80 microns in X and ~30 microns in Z. Interestingly the avalanche develops at ~130 microns from the wire, while on the drift chamber books it should be below 60 microns.       
 +
 
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- Luke and Lubomir are setting up the spare package in the tagger to scan it with 55Fe source.
  
 
== CDC update ==
 
== CDC update ==
  
- Mike showed his latest CDC alignment results using Millepede linked above . The scale varies +/-200 microns, some "structures" in the offsets are visible. After applying the offsets, the chi2 of the track fits improves; Mike will show more results next meeting. Simon's results are different in scale (+/-600microns). Mike will compare the two results channel by channel to see if there's some systematics.   
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- Mike on the CDC alignment with Millepede: using Monte Carlo he is varying the regularization parameter (that enters as an additional diagonal term) and looking how well the initial offsets are reconstructed. The attached slides above show the results, each slide for a different parameter value. When increasing the regularization term, there's a region where the offsets are best reproduced but then the diagonal term starts dominating forcing all the offsets to be zero.
 
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- Beni looked at the pedestals in the CDC varying different parameters: number of samples used, integer vs real number averaging, position of the pedestal window - all this explained in the above link. The main discussion was about the fact that Beni sees some slope (increase), when averaging over all the events, in the region before the real detector signal comes in case the signals are late. Mike suggested this may come from cross-talk from the other channels, but Beni has looked at this. Late signals can happen in cosmic showers (Eugene). Beni will do more studies when the computers are back.
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== Electronics ==
+
  
- All the electronics will be turned on on Monday. Before that Chris and Nick are going to clean the filters from the crates in the tagger; they are dirty. Eugene suggested consulting with the RadCon before duing this due to possible contamination.
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== Engineering ==
  
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- No problems reported as a result of the power outage, however most of the equipment is not turned yet on.

Latest revision as of 15:57, 7 July 2015

July 2, 2015 Drift Chamber meeting

Connection

  1. Instructions for Bluejeans meeting connection
  2. Meeting ID: 290664653
  3. To join via a Web Browser, go to the page [1] https://bluejeans.com/290664653.

Agenda

  1. CDC analysis update (Mike, Simon)File:MillepedeResults 2July2015.pdf
  2. FDC analysis update (Lubomir)
  3. Electronics (Fernando, Chris, Nick)
  4. Engineering
  5. Other

Minutes

Participants: Curtis, Mike(CMU), Sean(NU), Eugene, Luke, Dave, Chris, Nick, Simon, Beni, Sergey, and Lubomir (JLab).

FDC update

- Lubomir presented two slides summarizing the FDC performance for the S&T Review. Comments about efficiency slide - the worst (package #3) is shown; each chamber reconstructs 3D hit which requires hits in both cathodes (with at least 3 strips fired) and the wire plane. Resolution - to show the average wire resolution; discussions about why two methods give different results for the cathode resolution and what is the effect of the multiple scattering. General remark - needs bigger axis labels.

- Results with 55Fe source for the avalanche position w.r.t. wire reconstructed from the cathodes. Z (perp. to chamber plane) coordinate calculated from the up/down total charge ratio. X coordinate (in plane perp. to wire) from the crossing of the up/down centroids. After applying centroid corrections and calibrating the channels one can see a hole for the wire and amazing resolution of ~80 microns in X and ~30 microns in Z. Interestingly the avalanche develops at ~130 microns from the wire, while on the drift chamber books it should be below 60 microns.

- Luke and Lubomir are setting up the spare package in the tagger to scan it with 55Fe source.

CDC update

- Mike on the CDC alignment with Millepede: using Monte Carlo he is varying the regularization parameter (that enters as an additional diagonal term) and looking how well the initial offsets are reconstructed. The attached slides above show the results, each slide for a different parameter value. When increasing the regularization term, there's a region where the offsets are best reproduced but then the diagonal term starts dominating forcing all the offsets to be zero.

Engineering

- No problems reported as a result of the power outage, however most of the equipment is not turned yet on.