- Albert, J;
- Bajic, A;
- Bard, R;
- Beaulieu, M;
- Blinov, V;
- Boyarski, A;
- Broomer, B;
- Coupal, D;
- Dal Corso, F;
- Dolinsky, S;
- Dorfan, D;
- Dow, S;
- Dubrovin, M;
- Dusatko, J;
- Erdos, E;
- Facciai, R;
- Fernandez, JP;
- Ford, WT;
- Galeazzi, F;
- Haller, G;
- Innes, W;
- Jawahery, A;
- Kreig, H;
- Lankford, AJ;
- Levi, M;
- Von Der Lippe, H;
- MacFarlane, DB;
- Martin, J-P;
- Momayezi, M;
- Morandin, M;
- Morii, M;
- Nelson, D;
- Nguyen, P;
- Palrang, M;
- Roy, J;
- Sadrozinski, H;
- Schumm, B;
- Sciolla, G;
- Seiden, A;
- Smith, AJS;
- Spencer, E;
- Soha, A;
- Taras, P;
- Varnes, E;
- Weinstein, A;
- Wilson, F;
- Yushkov, A
The central drift chamber for the BaBar detector at the SLAC B-factory is based on a hexagonal cell design with 7104 cells arranged in 40 layers and drift gas Helium:isobutane (80%:20%). Performance optimization and integration requirements led to an electronics design that mounts the amplifier-discriminator and digitizing circuitry directly on the endplate. High channel density is achieved using a 4-channel custom amplifier-discriminator IC and an 8-channel custom CMOS TDC/FADC IC on a single circuit board. Data read from the front ends are multiplexed on 4 fiber optic links, and prompt trigger data are sent out continuously on 24 links. Analysis of cosmic ray data demonstrates that the electronics design meets the performance goals for the BaBar drift chamber. The final electronics were installed on the drift chamber in July, 1998. Installation of BaBar on beamline is scheduled for March, 1999. © 1999 IEEE.