Charge Transfer Structure is a critical component in CCD detector arrays that enables sequential transfer of photogenerated electrons through potential wells for signal readout.
| Parameter | Typical range | Notes & selection driver |
|---|---|---|
| Dark Current | <1 nA/cm² at 25°C | |
| Charge Capacity | 100,000-1,000,000 electrons per pixel | |
| Clock Frequency | 1-50 MHz | |
| Electrode Pitch | 5-20 μm | |
| Number Of Phases | 2, 3, or 4 phase designs | |
| Operating Voltage | 5-15 V clock pulses | |
| Transfer Efficiency | >99.99% per transfer | |
| Operating Temperature | -50°C to +80°C |
Ranges are indicative industry figures for RFQ preparation, not a supplier commitment. Confirm every value and standard with the legal manufacturer before ordering.
This component is used in the following industrial products
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The primary function is to transport photogenerated electrons from individual pixels to the output amplifier with minimal loss or distortion, enabling the sequential readout of image information while maintaining spatial and charge integrity.
High transfer efficiency (>99.99%) is achieved through optimized electrode geometry, precise doping profiles, carefully controlled oxide thickness, and sophisticated clocking waveforms that minimize charge trapping at interfaces and ensure complete charge packet movement between potential wells.
Common failures include charge transfer inefficiency due to interface states, dark current increase from contamination, electrode breakdown from voltage spikes, and clock feedthrough interference. These are mitigated through cleanroom manufacturing, proper passivation, and robust drive circuitry design.
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