Email from Roger:
Date: Fri, 01 Oct 2004 16:08:02 -0400 From: Roger D. CarliniTo: Juliette Mammei , Yongguang Liang , Dave Mack , Mark Pitt , Jim Birchall , Klaus Grimm , Neven Simicevic , Greg Smith , Allena Opper , Tony Forest , Norman Morgan , Mike Finn , David Armstrong , Shelley Page , Richard Jones Cc: carlini@jlab.org Subject: Collimator/quartz optimization [ The following text is in the "windows-1252" character set. ] [ Your display is set for the "ISO-8859-1" character set. ] [ Some characters may be displayed incorrectly. ] Hi Folks: The pdf's attachments in the previous message were too large for some email addresses. They are much smaller now. Sorry for the duplication. I took Juliette's plots from yesterday for Neven^Òs ^Ósculptured^Ô and "unsculptured" downstream collimator and superimposed 15 and 18 cm wide quartz bars with a tilt angle of 3 degrees just to see what they actually look like. See attached pdf files. If we were to use only a moderately "sculptured" collimator to suppress the large phi large theta events then the combined effect might be very clean. I suggest an algorithm to converge to an optimum collimator shape: First select several bar sizes and shapes. Then generate a contour plot at the z location of the collimator for each bar selection which contains the ratio of "elastics/in-elastics" for events which hit the quartz. Select a contour to give us the suppression factor desired. Then model this shape in GEANT to estimate the edge scraping component. Cut the collimator holes to the shape associated with the selected bar. Best Regards Roger Roger's attachments: NevensSculptured.pdf NevensUnsculptured.pdf