Detection Techniques

IRAR:

Direct Detection

Direct-detection receivers employ a square-law device which produces an electrical signal proportional to the intensity of the incident optical signal (e.g., a photodiode)---the signal's power is measured directly. Since any optical phase information is lost in the process, direct detection cannot be used to measure the Doppler frequency shift of the radar echo, and direct detection is subject to thermal and dark current noises in the receiver and to background light incident on the detector. Under certain conditions of limited signal strength, direct detection therefore offers sensitivity inferior to that of coherent detection. However, direct detection has advantages over coherent detection when either source temporal coherence or the spatial phase characteristics of the received signal cannot be strictly controlled, or when complexity or cost are important design issues.
















IRAR:

Coherent Detection

Coherent optical detection is analogous to the detection technique used for decades in superheterodyne radio receivers, but is much more difficult to implement at optical frequencies. The received field is beat against a local oscillator field of nearly the same frequency, and the output signal is proportional to the received field strength. The proportionality of the beat term to the local oscillator field strength provides essentially noiseless pre-detection gain in the ideal case, so that thermal and dark-current noises inherent to the photodetector and pre-amplifier are dwarfed by the quantum noise inherent in the signal itself. Thus coherent detection techniques provide superior sensitivity to direct detection under ideal conditions when signal strength is limited. Coherent detection also makes possible measurement of the small Doppler frequency shifts associated with velocities of interest for ground targets. Coherent detection places strict requirements on the spectral purity of the source and requires that the received signal and the local oscillator have spatial phase fronts which are nearly perfectly aligned over the active area of the detector.