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CMS Week Muon Alignment

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Presentation on theme: "CMS Week Muon Alignment"— Presentation transcript:

1 CMS Week Muon Alignment
James N. Bellinger University of Wisconsin at Madison 5-December-2006 DCOPS Data from MTCC2

2 CMS Week Muon Alignment
General notes With a better understanding of disk deformation and more time available we were able to align the lasers better for MTCC2. Although disk deformation results in a laser position change larger than the DCOPS aperture, COCOA can use lasers from opposite sides to reconstruct positions.

3 CMS Week Muon Alignment
Review of the structure of single SLM A typical SLM has 10 DCOPS along its line, with a crosshair laser pointing into the line from each end. This line is not perfectly radial. Each DCOPS has 4 CCDs arranged in a square. CCD numbers 1 and 3 measure something like “Rphi” and 2 and 4 measure “CMS Z.”

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What happens when the field is on The center of the disk is pulled inward and the rim of the disk pushed outward. This tilts the lasers backwards, so that the beam is redirected about 2 mrad inward towards the solenoid. For the DCOPS near the laser, the pull of the disk inward approximately compensates for the laser tilt, and we don’t see large deflections in Z. We see a large effect in DCOPS far from the laser.

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When the field is on Because the laser lines don’t go through the center of the disk, the laser tilt causes deflections in the “Rphi” as well as the “Z” measurements, so both are required to reconstruct the true rphi and z. Because the DCOPS are now in new locations with respect to each other and the laser, the CCD for one can shadow a downstream CCD and reduce the signal it sees.

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Field Off data: laser positions in 2 CCDs in DCOPS along an SLM 9 CCD3 Rphi 5 Laser Background of glare from laser 10 9 8 7 6 The laser position does not change much from position 1 to 5, but once past the midpoint it quickly goes offscale in Z. The “Rphi” variation is well contained. CCD4 Z 5 4 3 2 1 Laser This reflection is unique: rarely a problem

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Data Quality observations The double peak is a unique local reflection. The DCOPS next to the laser sees a substantial background due to glare. Some CCDs show a reasonable profile but have low signal strength (CCD 3 set, #9). Some show no signal (CCD 3 set, #5). Most profiles are perfectly useable.

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Field On Same SLM as before The changes in “Z” are easy to see, and there are changes in “Rphi” also. CCD3 Rphi Saturation Position offscale in other direction 6 CCD4 Z

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Deviations in Rphi Beam off – Beam on “Rphi” position in mm ME+2/SLM1 The trend of the deviations is consistent with the tilting of the laser. Relative position along the SLM in mm CCD has bad signal. Fit should have failed.

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Field Off Laser CCD3 RPhi This is the same SLM as before, but with the laser at the opposite end. The profiles are generally clean, and COCOA will be able to link together the measurements. 9 8 7 6 10 CCD4 Z Laser 5 4 3 2 1

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Field On 9 8 7 6 10 Laser CCD3 RPhi Same SLM as before. There appears to be some shadowing in CCD3 data, but the peaks are still detectable. 3 1 5 4 2 CCD4 Z Laser

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As you can see here the fit result is decent even when the profile has some saturation, as in CCD3 (lower left plot). I restrict the fit to a range around the peak. This is the DCOPS I numbered ’10’ in the previous sets of plots.

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This shows the Z-position of the laser peak as a function of field for 4 different Layer 2 chambers at ME+1. The overall deflection is O(.5mm): small because the disk bending and laser deflection are in the same direction.

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COCOA reconstruction of CSC center positions, from Gyongyi Baksay at FIT CMS Z position of the CSC center In mm, arbitrary origin Position along the SLM in mm

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CMS RPhi position of CSC Center In mm, arbitrary origin COCOA reconstruction of CSC center positions, from Gyongyi Baksay at FIT The error bars are smaller than the symbols. Position along SLM in mm

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Running Experience At irregular intervals a random terminal server port would lose connection with the DCOPS, and remain offline until the power was cycled at the LV crate. (This required a reboot of the analog system, as we belatedly discovered). 3 times during the month a telnet access to a terminal server port wedged, and ran in an infinite loop. We did not recover any instances of data corruption.

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The majority of the DCOPS data is available online in text form via the address above. It includes the fit information and the raw profiles.

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Near-term Plans Finish rewriting the core of the DAQ to get better speed. It isn’t complete, but I estimate that a full readout cycle will take less than 15 minutes. It addresses the hung port problem. Integrate the DAQ into the DCS/PVSS system. I think I can use DIM protocols, but need advice. Finish the code to retrieve and assemble DCOPS data from the database.

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Old Readout Scheme A bash script looped over the laser lines and submitted scripts which would telnet to the port for each DCOPS, issue the commands, and read back the raw profile. Another short program fit the profiles, if possible, and another shell script accumulated the resulting fit information and committed it to the omds database. Since this was sequential, the time required to complete a cycle for the +side was over an hour and a half, and a hanging process could stall the readout.

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New Readout Scheme A C++ program loops over the SLM Lines, forking a job to manage each Line and fork off subtasks to read out particular ports. The lowest level forked task is still a telnet invocation. I estimate that this part of the readout will take 9 minutes for all the SLMs, not just the +side ones. When the SLM jobs have completed or timed out, the Transfer Lines will be read. Then the profiles will be fit, data committed to the database, and the DIM service updated with the new results.


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