Saturation and blooming are phenomena which occur in all CCDs and which affect both their quantitative and qualitative imaging characteristics. If each individual pixel can be thought of as a well of electrons, then saturation refers to the condition where the well is full. The amount of charge which can be accumulated in a single pixel is largely determined by its area. However, due to the nature of the potential which holds charge within a pixel, there is less probability of trapping an electron within a well that is approaching saturation. Therefore, as a well approaches its limit, the linear relationship between light intensity and signal degrades. As a result, the apparent responsivity of a "saturated" pixel drops. At saturation, pixels lose their ability to accommodate additional charge. This additional charge will then spread into neighboring pixels, causing them to either report erroneous values or also saturate. This spread of charge to adjacent pixels is known as blooming and appears as a white streak or blob in the image. As various CCDs contain different architectures, saturation and blooming can be defined and controlled in many ways :
Mean Deviance Full Well (MDFW)
As the well starts to over fill, the photometric response of the pixel departs from linearity. The point at which this deviation exceeds an acceptable level is defined as MDFW. Cameras are usually constructed so that this signal level fills the full (12 or 16 bit) dynamic range of the analog to digital converter.
One can see signs of saturation even before the MDFW condition is reached. As the wells fills, the random noise ( signal) starts to be clipped at the top end. As a result, a condition termed noise clipping can be observed where the signal noise starts to decrease even though the signal is still increasing.
Output Stage Saturation
When many pixels on the CCD are saturated, or when extensive parallel and serial binning is being performed, the output stage may saturate. Under extreme conditions (for instance, daylight illumination of a scientific camera), the charge overload in the output node can cause the output amplification chain to collapse, resulting in a zero (completely dark) image. It should be noted that in all CCD devices, wells can hold more than they can transfer. When they begin to over fill, the saturation we observe is actually caused by approaching this maximum charge transfer condition.
Blooming can be controlled in a number of ways. For instance, a multi-phase CCD can be partially clocked during integration to eliminate image blooming. During integration, two of the three clock voltage phases used to transfer charge between neighboring pixels are alternately switched. When a pixel approaches saturation, extra charge is forced into the barrier between the Si and SiO2 layers, where it is confined. As the phases are switched, this confined charge is released and lost, while the signal charge within the well is preserved. As long as the switching period is fast enough to keep up with overflow signal generation, charge will not spread into neighboring pixels. Known as clocked anti-blooming, this technique is most appropriate for low light applications and is just now being considered for use in standard camera configurations.
Anti-blooming is more traditionally controlled by specific CCD architecture design. Cameras, such as Photometrics' PXL 1300 and ImagePoint, utilize CCDs that have charge drains running in a strip between every other column. Excessive charge that would normally cause blooming is siphoned off into this drain. Although such an architecture causes a reduction in the effective quantum efficiency and modulation transfer function (MTF), these devices are invaluable when light intensities span many orders of magnitude within a single image.