MUCOOL Meeting Notes, May 7 News: Al moretti says that modulator construction has started in Lab G and the drawings of the magnet and cryostat being assembled at LBL by Mike Green are here. Evidently the drawings imply safety requirements for the pressure vessel are going require some effort. Al Moretti has new keys for Lab G. Paul: In one slide Paul outlined an argument that Dave Carey made about chromatic effects in plasma and Lithium lenses being half as bad as in solenoids and quads. The reason being that the current causes the field that directly focuses, rather than focusing being a more indirect result of the fields. In any case quad systems with large apertures and small beta*'s are very tough to build. Wishi is trying to put bent solenoids in COSY. Valery: Valery and Nikolai have put out a note on a bunched beam line designed around a quadrupole channel, with some space for rf cavities. The average beta is about 2 m for quad spacings of about 1 m and 15 cm. The line is presumed to be at 0 degrees to the proton beam, and is assumed to capture 500 MeV/c +- huge dp, pion momenta, A 90 degree FODO with waists provides some room for cavities. The quads are grouped in pairs, but the average beta is still roughly two times the complete cell length, and there is 1 m of space for linacs in every cell. The acceptance of the channel goes like R^4, and the mu/pi ratio goes like R so the number of Muons goes like R^5. Cavities should be large also, and since the decay to the muon introduces more perpendicular momentum than anything but a very thick window, it should be possible to use thin al or cu foils between the sections of the rf cavity without degranding the beam. Collision lengths are relatively long and collisions don't contribute, to first order. Valery and Nikolai presented monte carlo results showing the pion and muon distributions after the capture and decay section showing the dependence on R and momentum. (busybody note from J.N.: The proposed beam, with large momentum and angular acceptance, located at zero degrees in the lab, might have many high energy protons and other particles which would make experiments difficult. In general, beamlines use both momentum analysis with bending magnets, and some other method of separation to produce reasonably pure beams. High energy protons have enormous kenetic energy and produce meny secondaries. Better to be away from zero degrees.) Norbert: He presented a plan for the initial bunched beam cooling line to be in a tunnel parallel to the BOONE target enclosure. This muon line would be essentially an underground linac facility, supported by a klystron gallery on the surface. William: Leeson presented initial thoughts on the filtering the pions out of a muon beam. He would use perhaps 2 m of absorber which would intercept and scatter pions preferentially. Vincent and Derun: Both measurements of Q and resonant frequencies as a function of temperature and calculations of an rf coupler for a pillbox cavity were presented. At room temperature measurements of Q were about half of the theoretical predictions. At low temp the Q increases but less then expected. The resonant frequencies were about as predicted. As the temperature is lowered, the Q varies discontinuously, presumeably due to the way the copper cavity is contracting. The discontinuities seem to be due to the motion in the joints, and the anomalously small Q seems also due to effects relating to the joints. The feeling was that reassembling the cavity with would improve things. This will be underway soon. The coupler design is being done with MAFIA, using an algorithm that involves 1) finding the resonant frequency, 2) studying power flow on resonance and 3) adjusting the dimensions of the coupler until one obtains critical coupling. This is underway but not done.