Please refer to the CFT homepage for a general description of the Central Fiber Tracker project. The CFT Trigger homepage also has a lot of information.
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back to:Because the production of the Front End boards for the CFT has fallen too far behind schedule, it will not be possible to test the performance of the system in the real detector before we have beam. Clearly, it is important to test somewhere, at least once, what the performance of the CFT is likely to be in order to avoid (if possible) any huge problems. The prototype cylinder 3b was tested
The D0 silicon vertex detector dissipates about 3600W of power which is removed with -10oC water. Since this temperature is low enough to cause dew point condensation or even ice formation, it was decide to run the tracker in dry air (100% nitrogen). Ice formation and dew point condensation are serious concerns. Unfortunately, there is a conflict: the CFT needs to run in humid air with about 30% relative humidity because it was built in humid air. The builders of the CFT are convinced that drying it out will cause the fiber positions to shift enough to make the map which was made of the exact fibers positions useless (hence the only way to do alignment will be using tracks). Perhaps even more alarming, there is a CFT group prediction that the internal stress on the 1st CFT cylinder dried out will be at 80% of the value needed to physically (and therefore irreversibly) break it.
To test how drying out the CFT might change it's performance, the Lab 3, cylinder 3, proto-type CFT was dried out, and data was taken as it dried to check for deformation. Preliminary analysis results follow; they should be repeated once the new CMM data is available.
Results: (skip down to the resolution section to see plots)
My preliminary conclusion is that something was happening as the cylinder dried out, but I can't yet say exactly what.
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Clyinder 3b was a prototype cylinder. The setup consisted of flat ribbons on the top and bottom of the cylinder. The flat ribbons were used for tracking are were not dried out or moved during the test.
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For my analysis, there is no need to make a distincition between signlets and doublet, one simple looks for local maxima and checks if the local maxima passes a threshold cut or not (Incidentially, my alogrithm is slightly more efficiency than the Level 1 trigger algorithm which requires a strict isolation cut on the two neighbors making it more sensitive to noise). Nevertheless, as a cross-check, one can look at the local fiber coordinates and clearly see when the "singlets" and "doublets" are.
PLOT OF:Local Fiber Coordinates
The singlet peak, in the previous plot, centered at zero is what one would expect from simple geometrical considerations.
For reference, here is a plot of a typical PE Distribution (for this particular plot, there was a 2 PE pre-selection cut made to suppress the noise).
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The following table summarizes the global offsets and resolutions versus the number of days that the cylinder was dried. The fit error on all the number is the table is about 1 micron.
| time | Top Ribbon Offset | Top Ribbon Resolution | Bottom Ribbon Offset | Bottom Ribbon Resolution |
|---|---|---|---|---|
| humid, day 0 | 0 | 111 | 0 | 122 |
| dry, day 10 | -11 | 107 | 6 | 121 |
| dry, day 25 | -5 | 105 | 5 | 120 |
Now, after seeing the global shifts, one can look at the shifts along the length of a ribbon:
PLOT OF:Mean of residual versus the ribbon length (i.e. a Profile histogram).
PLOT OF:Gaussian fit to the mean of the residuals versus the ribbon length (i.e. a FitSlice histogram).
In the previous plots, one sees how the ribbons are not perfectly straight. There is structure. What is important, however, is the relative shifts. The profile method shows large local shifts whereas the fitslice method does not. At present, I do not understand the difference; it must somehow be related to the tails of the distribution. Hopefully, once the new CMM data is ready, the results can be clarified.
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In the axial layers, the odd fibers are the ones at smaller radius. The means given in the following tables are in units of photoelectrons. There appears to be know even and odd structure, i.e. the upper and lower layers are showing approximately the same light yield.
| time / fibers | L1 (flat) | L2 (flat) | L3 (axial) | L4 (axial) | L4 (axial) | L5 (flat) | |
|---|---|---|---|---|---|---|---|
| day 0 / even | 7.42 | 7.53 | 7.26 | 6.98 | 7.82 | 6.56 | |
| day 0 / odd | 7.20 | 7.52 | 7.40 | 6.96 | 7.69 | 6.42 | |
| day 10 / even | 7.24 | 7.52 | 7.63 | 7.47 | 7.61 | 6.40 | |
| day 10 / odd | 7.01 | 7.48 | 7.73 | 7.28 | 7.41 | 6.27 | |
| day 25 / even | 7.22 | 7.49 | 7.59 | 7.22 | 7.53 | 6.53 | |
| day 25 / odd | 7.06 | 7.39 | 7.70 | 7.15 | 7.40 | 6.39 |
Here are a few plots of the # of photo-electrons versus fiber # for all five of the layers:
| L1 | Flat ribbon |
| L2 | Flat ribbon |
| L3 | Cylinder 3b Axial |
| L4 | Cylinder 3b Axial |
| L5 | Flat ribbon |
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PLOT OF:Efficiency versus Light Yield in units of photoelectrons.
What one extracts from the previous plot is that the noise level must be low enough so that we can set a 1 PE threshold. Due to cassette production constraints, different sets of cassettes had to be used during the three runs. That may be the reason that the efficiencies vary for the three runs. Each VLPC has its own characteristic gain and spread of gain, and unless all of the bais voltages are correctly set for high efficiency (which can mean higher noise), the efficiency can suffer.
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There were 3 datasets taken:
| Days | Delta Days | Condition | Triggers | Selected | Preselected (strong) | Preselected (weak) |
|---|---|---|---|---|---|---|
| Aug 22-24 | 0 | humid | 1383312 | 43266 | 75319 | 107923 |
| Sept. 2-3 | 10 | dry | 1577729 | 51650 | 71212 | 99501 |
| Sept. 16-18 | 25 | dry | 1388932 | 46118 | 61742 | 78900 |
Each ribbon is connected to 4 SVX chips. One does see occasional common mode noise on a chip by chip basis.
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Send comments and suggestion to brsmith@fnal.gov
Last modified: Dec 1, 2000