Solid-State Imaging with Charge-Coupled Devices by A.J. Theuwissen

By A.J. Theuwissen

Solid-State Imaging with Charge-Coupled Devices covers the total imaging chain: from the CCD's basics to the purposes. The publication is split into 4 major elements: the 1st offers with the fundamentals of the charge-coupled units quite often. the second one explains the imaging suggestions in shut relation to the classical tv software. half 3 is going into element on new advancements within the solid-state imaging global (light sensitivity, noise, machine architectures), and half 4 rounds off the dialogue with numerous purposes and the imager know-how.
The booklet is a reference paintings meant for all who take care of a number of elements of strong- country imaging: the academic, medical and commercial global. Graduates, undergraduates, engineers and technicians drawn to the physics of solid-state imagers will locate the solutions to their imaging questions. due to the fact each one bankruptcy concludes with a brief part `Worth Memorizing', examining this brief precis permits readers to proceed their analyzing with out lacking the most message from the former part.

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Extra resources for Solid-State Imaging with Charge-Coupled Devices

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Once the electrons are trapped in these surface states, they will not recombine because there are no holes in which are needed to do so. On the other hand, however, these electrons do not remain trapped in the surface states but after a while are released again. 13, freed electrons can easily move to a potential containing a charge packet different from the charge packet where the freed electron originally came from. This charge packet might already have moved further on. The processes of trapping and "detrapping" the electrons into the surface states are not related to each other.

The gate voltage necessary to achieve flat bands in the silicon (or to counterbalance all internal effects which influence the effective gate voltage) is also modified by the oxide charge Qox. This charge consists of fixed oxide charges and mobile oxide charges (alkali ions). The value of Qox depends on the crystal orientation of the silicon bulk material, but is also very sensitive to the processing conditions. This charge is always positive and is usually represented at the silicon-silicon oxide FUNDAMENTALS OF CHARGE-COUPLED DEVICES 19 interface.

Field underneath the gate biased at 5 V is almost zero; - B-B’ : at a certain (small) depth in the silicon the influence of the neighboring gates on the electric field underneath the middle gate (at 5 V) is at its highest level. The minimum fringing field is at its maximum value; - C-C’ : burying deeper in the silicon bulk will lead to a decreasing influence of the fields generated by the neighboring gates. At these depths the various gates are almost the same distance apart, and the minimum value of the fringing field will decrease.

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