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Learn about signals, noise, and balanced detection in coherent laser radar systems. Explore advantages, mixing equations, noise issues, and implementations of coherent detection techniques. Enhance SNR and dynamic range while resolving phase ambiguities.
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ECEG287 Optical Detection Course NotesPart 11: Coherent Detection Profs. Charles A. DiMarzio and Stephen W. McKnight Northeastern University, Spring 2004 Charles A. DiMarzio, Northeastern University
Overview • Coherent Detection Fundamentals • Signals and Noise • Balanced Detection • Resolving Ambiguities • Heterodyne • Offset Homodyne • Optical Quadrature Charles A. DiMarzio, Northeastern University
Coherent Laser Radar Optional Pulsed Amplifier l/4 Laser l/2 Charles A. DiMarzio, Northeastern University
Mixing Equations Charles A. DiMarzio, Northeastern University
Coherent Detection Advantages mW nW fW • SNR Enhancement wrt Detector Noise • Dynamic Range Reduction • Phase Information (at least partial) Charles A. DiMarzio, Northeastern University
Coherent Detection Model Signal Local Oscillator Noise: hnB Detector Noise Charles A. DiMarzio, Northeastern University
Coherent Detection Noise Issues 10000 Signal 8000 4kTB 6000 4000 Quantum Noise 2000 0 0 20 40 60 80 100 P sig 4 x 10 6 Dotted Lines: Higher LO 5 4 3 2 1 0 0 20 40 60 80 100 P sig Charles A. DiMarzio, Northeastern University
Balanced Mixing 4Re(sig*ref*) |sig-ref|2 Subtract =|sig|2+|ref|2- 2Re(sig*ref*) sig-ref sig+ref ref |sig+ref|2 =|sig|2+|ref|2+ 2Re(sig*ref*) sig Charles A. DiMarzio, Northeastern University Stopped Mon 23 Feb 04
Balanced Mixing Implementation sig-ref sig+ref ref sig Charles A. DiMarzio, Northeastern University
Another Implementation sig-ref sig+ref ref sig Charles A. DiMarzio, Northeastern University
Direction (Phase) Ambiguity Transmitter Transmitter LO LO Signal (Postive Doppler) Signal (Postive Doppler) (Negative Doppler) (Negative Doppler) f 0 Charles A. DiMarzio, Northeastern University
Offset Local Oscillator Transmitter Transmitter LO LO Signal (Postive Doppler) Signal (Postive Doppler) f 0 Charles A. DiMarzio, Northeastern University
Offset LO Implementation (1) Optional Pulsed Amplifier l/4 Laser l/2 Laser Charles A. DiMarzio, Northeastern University
Offset LO Implementation (2) Optional Pulsed Amplifier l/4 Laser l/2 Bragg Cell Charles A. DiMarzio, Northeastern University
A Very Simple Laser Radar Laser i Current Monitor t Charles A. DiMarzio, Northeastern University
Quadrature Demodulation I Signal LO (Ref) 90 Deg z=I+iQ Q Charles A. DiMarzio, Northeastern University
Optical Quadrature Demodulation (End View of Polarization) Reference (Circular Polarization) Signal (Linear Polarization) Charles A. DiMarzio, Northeastern University
Optical Quadrature and Balanced Mixing To Cameras • Based on Mach-Zehdner interferometer. • Signal Arm: 45-Degree Linear Polarization (Ex=Ey) • Local Oscillator: Circular Polarization (Ex=iEy) • Both Interferometer Outputs used for balanced detection (common mode rejection) • Light source is low power HeNe or diode laser. Objective Condenser LO SIG From Laser /4 Charles A. DiMarzio, Northeastern University
60 50 40 30 20 10 0 60 40 n=1.6 d=53 mm -10 20 0 -20 -40 -60 Optical Quadrature Microscope Unwraped Phase from Experiment, Radians . Charles A. DiMarzio, Northeastern University