Alcator C-Mod Weekly Highlights August 6, 2001 Plasma operations continued at Alcator C-Mod last week, the final week of the 2001 Experimental Campaign. Five run days were scheduled and completed. All runs were extended by an extra two hours in order to maximize the data obtained from each experiment. A total of 107 plasma shots were produced with a startup reliability of over 87%. Experiments carried out included two MP's related to double barrier/ITB formation, a study of pedestal parameters and the QC mode in EDA H-mode discharges, exploitation of C-Mod's long-pulse capabilities, and plasma operation at 8T for the first time since 1998. Having completed the 2001 experimental campaign, C-Mod is now entering an extended period of maintenance, inspections, and facility upgrades. Physics ------- This week was extremely successful from the standpoint of learning more about plasma conditions under which the density barrier and internal transport barrier (ITB) modes can be produced in C-Mod. The density barrier mode was produced with off-axis ICRF heating (70 MHz) on BOTH the tokamak high field side (HFS) at 3.9 T and the low field side (LFS) at 5.4 T. Preliminary attempts were also made at heating the LFS density barrier with on-axis ICRF power at 80 MHz. The density barrier mode was first produced at lower B_t = 3.9 T using 1.5 MW of off-axis ICRF heating power from the J-port antenna, driven at 70 MHz. The central density was observed to rise to ne(0) = 6 X 10^20 m^{-3} and the toroidal rotation velocity (v_tor) from HIREX decreased to zero and reversed direction, becoming counter-current. Interestingly, the value of B_t where the barrier formed at 70 MHz, scales nicely from the critical B_t for barrier formation at 80 MHz, that is: B_t = (70 MHz / 80 Mhz) * 4.5 T = 3.93 T. This places the minority hydrogen cyclotron resonance at the same minor radius on the high field side (12 cm) as it was at 4.5 T and 80 MHz. A density barrier was also produced with the 70 MHz ICRF resonance on the low field side (LFS) at 5.4 T. Only 1.35 MW of ICRF power from J-port was necessary. ITB formation was again characterized by peaking density profile with ne_TS(0) = 6X10^20m^{-3} and ne(0) / ne(ave) > 2. Formation of the density barrier at both 3.9T and 5.4T was preceeded by a transition to an H-mode phase, and the H-mode edge is maintained throughout the ITB evolution. We also attempted to heat the LFS density barrier mode at 5.4 T using the available 80 MHz ICRF power from D & E ports. There was some evidence of heating within the barrier from the 80 MHz power (at the 0.5 MW level). The neutron rate more than tripled and the central density increase was arrested at ne_TS(0) = 3.5 X 10^20 m^{-3} during application of the on-axis ICRF power. These results are not conclusive, however, because there were two H->L back transitions which prevented the initial barrier mode from becoming well - developed. Operations ---------- The runs on Thursday and part of Friday were devoted to extending the plasma pulse lengths in C-Mod. These experiments succeeded in extending the end-of-flattop (EOF) from 1.5sec to 3.0sec (3.2 sec for the TF), more than doubling the flattop time in these inductively-driven discharges. The long-pulse experiments were carried out at 5 tesla, with line-averaged density in the range 0.3e20