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hi all, Today's discussion led to the following plan: Each MET correction (muon and track) will store a bool and two floats for each muon in the event. The muon correction will store, for each muon, (Ex, Ey) where Ei is the ith component of the energy removed from the calorimeter due to the MIP. The tcMet correction wiill store, for each muon, (Ex, Ey) where Ei is the ith component of the energy removed from the calorimeter assuming the muon were corrected as a pion using the response function. Attached below is a tex file containing some equations trying to clarify the words above. From here, we agree to take the implementation of the corrections as is and freeze them until testing is done. In the next week, we (myself and Puneeth) will create a first attempt to implement and store the above values and validate them against the current implementation. If things check out, we will commit and tag. The muon experts from UCSB will then decide upon and submit improved baseline muon selections. While this is going on: Filip, Claudio, and Avi will take care of politics and everything will be great. ------------------------------------------------------------------------------------- Before ending, Avi and I talked a bit more on this morning's meeting and want to put forward a slight change to the proposed plan of work. Rather than just storing a bool, we think it would be worthwhile to store an int. This would serve the purpose not only of telling the user whether or not a muon was corrected but also which momentum (global, tracker, standalone) was used in the correction. Thus, we suggest replacing the bool with: 0 - muon was not corrected 1 - muon was corrected using global momentum 2 - muon was corrected using track momentum 3 - muon was corrected using standalone momentum Responses to this proposal would be greatly appreciated. I think that summarizes this morning's meeting and our work for the next week. Anything missed or errantly reported? Cheers, Frank | |||||||
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then, using the beamspot and the normal vector the corrected impact point is {bx + d0corr sin(phi), by - d0corr cos(phi)} from which the corrected impact parameter angle is d0corrPhi = atan( {by - d0corr cos(phi)}/{bx + d0corr sin(phi)} ) | ||||||||
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> > | d0corrPhi = atan( -cot(phi) ) ok, so i realized after writing this up that something is still unclear to me: is the corrected impact parameter angle measured from the displaced beam spot (physics origin) or the detector origin (0,0)? if the first one, then the second expression is correct, if the latter, then the first expression for d0corrPhi is the right one | |||||||
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use linear approximation to model track as y cos(phi) - x sin(phi) + d0 = 0, where phi is the azimuthal angle of the momentum vector at the impact point and d0 is the uncorrected impact parameter (measured from origin) NOTE: the sign convention used for d0 (and hence the sign on d0 above) was determined by trial and error now, the displaced beamspot is at (bx, by) and we can define a unit vector perpendicular to the track {-sin(phi), cos(phi)} using this the corrected impact parameter is then d0corr = d0 - bx sin(phi) + by cos(phi) then, using the beamspot and the normal vector the corrected impact point is {bx + d0corr sin(phi), by - d0corr cos(phi)} from which the corrected impact parameter angle is d0corrPhi = atan( {by - d0corr cos(phi)}/{bx + d0corr sin(phi)} ) | |||||||
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Hi all: Below are brief minutes of today's informal meeting. Filip -- will you be available on Saturday or Sunday to have another informal meeting with Avi and Frank? For example .. Sunday at 10:30/central, 8:30/California, 17:30/CERN? The discussion items are operational issues, namely how to deliver the tcMET code by when. Please let me know if you are flexible.. Teruki (1) Feb 28 ... deadline of Feb 28 for approving analysis plots with 2_2_x I believe this is a soft deadline set by Peter and Daniel (JetMET conveners) to proceed the appovale process (JetMET to CMS) by May or so. "May or so" is a hard deadline. I will check with Filip and Peter/Daniel to understand the procedure. (2) BIG Picture: provide tcMET as a package for CMS for physics analysis namely the code implementation. (*) CMSSW package ? ... 3_0_0? (*) When? ... May? or later?? (*) How? Technical issues such as "configurable" calorimeter responce functions <Frank, could you list big items?> (3) Frank has been working on tcMET with 2_2_x and 3_0_0. Note that those codes are based on hard-coded calorimeter response functions. (There will be many technical issues that I should know. But this is one of them that Frank told me today.) So we have to address those issues (related to (2) above). Other than that, Frank can have updated plots of tcMET using 2_2_x by early next week. (4) Golden Plot(s) ... see the attachment for the starting point of the discussion We have to discuss about Golden Plots to demonstrate the performance of tcMET visually well. Filip and I picked MET and tcMET ditributions for Z(-->mumu) and W (-->mu nu) events based on Avi's and Frank's suggestion. Avi and Frank also suggested the same plots, but with Z(-->ee) and W (-->e nu). But I picked muon channels, because it will be one of fast validation process at CMS. J/psi --> mumu, Z --> mumu, Z --> tau tau --> mu + tau_h, etc.. So in my mind, if I had to choose, the muon-channels are my choice. Please correct/add as necessary.
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> > | February 20089 February 2008
fgolf@uaf-6:crab$ crab -publish -c WJets-madgraph_Fall08_IDEAL_V9_v1 crab. crab (version 2.4.3) running on Mon Feb 9 12:12:51 2009 crab. Working options: scheduler glite job type CMSSW working directory /home/users/fgolf/snt_nm2/CMSSW_2_2_3/crab/WJets-madgraph_Fall08_IDEAL_V9_v1/ crab. <dbs_url_for_publication> = http://ming.ucsd.edu:8080/DBS1/servlet/DBSServlet Traceback (most recent call last): File "/code/osgcode/ucsdt2/Crab/CRAB_2_4_3/python/crab.py", line 839, in ? crab.run() File "/code/osgcode/ucsdt2/Crab/CRAB_2_4_3/python/crab.py", line 796, in run if act in self.actions.keys(): self.actions[act].run() File "/code/osgcode/ucsdt2/Crab/CRAB_2_4_3/python/Publisher.py", line 234, in run if reports[0].status == "Success": IndexError: list index out of range
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