Report CTSL-29 CALIFORNIA INSTITUTE OF TECHNOLOGY Synchrotron Laboratory Pasadena, California PION PRODUCTION IN 300 GEV NUCLEON-NUCLEON COLLISIONS

Report CTSL-25 CALIFORNIA INSTITUTE OF TECHNOLOGY Synchrotron Laboratory Pasadena, California EFFECTS OF MAGNET NON-LINEARITIES ON BETATRON OSCILLATION FREQUENCIES FOR THE 300 BEV PROTON SYNCHROTRON

Report CTSL-19 CALIFORNIA INSTITUTE OF TECHNOLOGY Synchrotron Laboratory Pasadena, California BROKEN SYMMETRIES AND BARE COUPLING CONSTANTS

Report CTSL-30 CALIFORNIA INSTITUTE OF TECHNOLOGY Synchrotron Laboratory Pasadena, California A N ACHROMATIC INFLECTOR FOR T H E CALTECH SYNCHROTRON

Report CTSL-21 CALIFORNIA INSTITUTE OF TECHNOLOGY Synchrotron Laboratory Pasadena, California R.F. SYNCHRONIZATION DURING TRANSFER IN THE CASCADE SYNCHROTRON

If a low energy synchrotron is to be used as an injector for a 300 Bev machine, the problem may arise of synchronizing the two R.F. systems at transfer time in order that a bunch of protons in the injector may be transferred to a bucket in the main machine without loss of particles. A possible synchronization scheme is proposed and investigated here.

The chiral effective pion – nucleon Lagrangian of order p 4 # 1

We construct the minimal effective chiral pion–nucleon SU(2) Lagrangian at fourth order in the chiral expansion. The Lagrangian contains 114 in principle measurable and 4 contact terms needed for the renormalization. We develop both the relativistic as well as the heavy baryon formulation of the effective field theory. For the latter, we also work out explicitly all 1/m corrections at fourth or...