Notes - instrumentation/Beam physics Meeting March 16, 2005 Agenda: 1) Main Injector Batch by Batch Intensity(BBI) Monitor - Alexei Semenov 2) TeV Synchlight Status - Randy 3) Tev FW status - Nathan Action Items: MI BBI 1) Get the BBI output for NUMI beam permit setup 2) Validate calibration with respect to DCCT. Synclite 1) Study new camera and, if waarented, replace existing cameras with new ones. 2) check gain scale switch on pbar camera and remeasure relevant distances when there is a appropriate downtime 3) Seriously crosscheck with flying wires since emittance are now about as good as Randy knows how to make them. 4) Vladimir expressed interest in seeing the raw distributions to check for off axis ellipses due to coupling. Tev FWs 1) Push on getting the wires flown during stores 2) Add standard array for centroids to OAC. (average two passes and 37 elemts with (0) element as the (intensity weighted?) average. What about amplitudes? Other 1) Consider providing for "SBD-Like" viewers for flying wire profiles that are stored on log files and the synclite 2-d images. 2) corrected raw data button for Tev SBD. 3) something about the wall current monitor in MI? Details: 1) Mi Batch by Batch intensity Monitor - Alexei Alexei's talk is in the doc db as doc xyz. 2) Sync lite a) The variation of sigma with intensity has been measured and a correction is being applied in the fronteend. Plot can be found where?) b) Randy varied the camera distance from the lens for both p and pbar. He showed plots of the horizontal and vertical beam sigmas as a function of the camera longitudinal position for data and the simulation. There is very good agreement between data and simulation. Salient features are: 1) the horizontal and vertical sigmas don't show the same features. It's tricky to do this correctly. 2) for pbars, the full dipole and half dipole edges have different focal points. 3) The proton focal point is at the very limit of the camera's adjustment. 4) He set the cameras where the simultion indicated, and, for pbars, for the half dipole light. 5) When possible, he wants to measure the distances in the tunnel one more time. c) The repaired new camera is back and Randy will study it the bench to see if it has the same variation of sigma with intensity as ones in the tunnel. d) There is a gain selector switch on the cameras(?) that is prably set differently for pbars and protons. This could explain the factor of 4 difference in gain for the two systems - something to check next time there is a tunnel access. 3) Flying wires