The ACIS instrument uses MIT Lincoln Laboratory CCID 17 Devices.[4]
These CCDs consist of a 1024 x 1026 pixel imaging section, with a separate 1024 x 1026
shielded frame store region. The pixels are 24m square, and when coupled
with the focusing optics, will provide resolution of 0.5 arcseconds.
The frame store for these devices has a novel architecture, with two separate
sections that feed into two independent serial registers (see Figure 1).
This design permits charge to be clocked in either direction and
makes possible non-standard readout configurations. For example output nodes
A and B can be both be readout through output A, while nodes C and D are both
readout through C (AC mode).[4]
Both front-illuminated (incident photons pass through the gate structure) and back-illuminated (incident photons incident directly into the depleted silicon) devices have been made for ACIS. Back-illuminated devices (BI) offer the advantage of higher quantum efficiency at lower energies, but have significantly lower spectral resolution than the front-illuminated (FI) devices.[5]
Figure 1: Schematic of CCID 17