Summary of the MuCool Meeting on march, friday 26th 1999 Simulation Studies (Paul Lebrun) Paul Lebrun summarized the effort of using COSY as a beam optics code to design beam lines with solenoids,cavities and cooling stages. The has been a main issue for a number of weeks and in the optics meeting taking place regularly on mondays. Preliminary calculations showed that the emittance is dependant on the order of the taylor expansion. This can be problem of the code or a problem of the beam transport and has not been determined yet. The question is, with what order of the expansion we have to run cosy with in order to get good results. Another check of cosy can be done by using the dpgeant and track the same channel to see what the emittance growth is in this case. The first attempt failed because in the cosy simulation the canonical angular momentum was not taken into account. In addition, Paul will try to implement a new method of calculating the phase space and compare this to the standard method used so far, which is summing the squares of the particle offsets to get the standard deviation. With the method proposed by Dave Carey, the phase space is divided in bins and bins which are populated by one particle are contributing only the bin size and not the full deviation from the center. (Emittance= Nr. of nonempty cells x volume of the cells) Paul also presented emittance calculation with and without including tails to see the contribution. In the example he used, the non gaussian part was counted as losses. In addition to that the question was asked whether the aperture of the cavity could be decreased without significant increase in loss which would help the shunt impedance in the cavity a lot. So for aperture cuts were made in the low Beta region and from the simulation is seems that reducing the aperture is not possible. More detailed investigations will be done as soon as possible with aperture cuts in the cavity. A little confusion came up when the actual numbers where compared. Paul will do the simulation again. The next agenda point was an update on the cavity R&D in LBNL. Derun summarized the work going on. Poeple are preparing the cold test of the Beryllium window cavity. Also the tuning and measurement goes on. While the cell frequency of the cavity is too low by a few MHz the coupling cell shows a more significant deviation which can only be corrected by shimming. This will be done soon. Main reason is the use of round center conductors instead of square ones. The Q of the clamped cavity is only 6000 which seems very low. The natural Q should be around 20.000. For the Beryllium cavity design Neill Hartmann and Eric Wu started with the simulation of the window in the iris. Also the single cell (pill box) cavity design has been started already. Vincent Wu from Fermi will go to Berkeley for 4 weeks and work on couplers for the 3 cell test cavities. Next agenda item: Wedges and Rick Fernow rick uses the beam coming out of the simulation of a 15 Tesla solenoid channel (baseline design for mucool). The 6D emittance after the wedge is still growing by approximately 50 to 60 %. Following the advise to increase the field from 3.5 to 5 Tesla and the dipole field from 1.5 to 2 Tesla shortens the Lamor wavelength and increases the number of Lamor wavelength in the channel. The optimum angle is between 53 and 135 deg. Still the is an emittance growth of 40 %. The check suggested to see how much aberration is produced by the bent solenoid (check by sending it through another bent solenoid to cancel the effect) does not work. It seems like the emittance filaments much faster. Next agenda item: Alan Bross: TPC report most of the components are on order. Lab 6 will be used for the test setup. For the design the electric field contour will have to be optimized to reach the goal of having the super high timing precision. The field integral on all path should be constant in the TPC. For test a 7 to 60 GHz bandwidth is required. The laser, used in A0 to drive the Electron rf gun could be used for that. next agenda item: Steve Kahn: Investigation of the momentum resolution in the cooling experiment. The fit for the resolution so far delivers a value of 3 MeV. for the sigma while originally .15 was required. Steve will go on with the simulations.