The document presents an overview of heterodyne and homodyne detection methods in optical fiber communication, emphasizing the signal processing techniques used to mix frequencies and detect signals. Heterodyne detection allows for improved application in various technologies such as Doppler velocimeters and laser range finders, while homodyne detection is noted for its sensitivity but complexity. Key advantages and applications of these detection methods are discussed along with references for further exploration.

1. PRESENTED BY
VAISHALI.K
M.Tech (ECE) - Ist yr
21304023
DEPARTMENT OF ELECTRONICS & COMMUNICATION
ENGINEERING
PONDICHERRY UNIVERSITY
SUBMITTED TO
Dr.R.NAKKERAN,
Head of the department,
Dept.Of Electronics Engineering

2. AGENDA
 Introduction
 Coherent detection
 Homodyne detection
 Heterodyne detection
 Heterodyne detection principle
 Advantages
 Applications
 References
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3. INTRODUCTION
 A heterodyne is a signal frequency that is
created by combining or mixing two other
frequencies using a signal processing
technique called heterodyning.
 Heterodyning is used to shift one frequency
range into another, new frequency range, and
is also involved in the processes
of modulation and demodulation.
 The two input frequencies are combined in
a nonlinear signal-processing device such as
a vacuum tube, transistor, or diode, usually
called a mixer.
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4. INTRODUCTION
 In coherent detection the local carrier generated at the receiver is
phase locked with the carrier at the transmitter.
 Hence it is also called synchronous detection.
 In non coherent detection the local carrier generated at the
receiver not be phase locked with the carrier at the transmitter.
 Hence it is also called asynchronous detection.
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5. COHERENT DETECTION
 In optical fiber communication the term coherent refers to any
technique which employs non linear mixing between two optical
waves.
 In this technique gain is provided to the incoming optical signal
by combining or mixing it with locally generated continuous
wave (CW) optical field.
 The device used for creating the CW signal is a narrow line width
laser called a local oscillator (LO).
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6. COHERENT DETECTION
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7. MATHEMATICAL ANALYSIS OF
COHERENT DETECTION
 Let us consider the electric field of the optical signal to be plane
wave having the form
 To send information one can modulate the amplitude, frequency
or phase of the signal carrier.
 Thus one of the following three modulation techniques can be
implemented
 ASK
 FSK
 PSK
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8. MATHEMATICAL ANALYSIS OF
COHERENT DETECTION
 In direct detection system the electrical signal coming into the
transmitter amplitude modulates the optical power level of the
light source.
 Thus the optical power is proportional to the signal current level.
 At the receiver the incoming optical signal is converted directly
into demodulated electrical output.
 This directly detected current is proportional to the intensity Idd
of the optical signal
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9. MATHEMATICAL ANALYSIS OF
COHERENT DETECTION
 Because the response capability of the receiver
 If the local oscillator field is
 Now the coherent detected output at the receiver is
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10. MATHEMATICAL ANALYSIS OF
COHERENT DETECTION
 Since the optical power P(t) is proportional to the intensity at
the photodetector we have
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11. HOMODYNE DETECTION
 When the signal carrier and local oscillator frequencies are
equal, it is called a homodyne detection.
 Homodyne detection brings the signal directly to the baseband
frequency, so that no further electrical demodulation is required.
 Homodyne receivers yield the most sensitive coherent system.
 It is most difficult to build, since the local oscillator lasers to
have the same frequencies.
 In this since
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12. HETERODYNE DETECTION
 In heterodyne detection, the intermediate frequency is nonzero
and an optical phase locked loop is not needed.
 In heterodyne detection, the local-oscillator frequency (LO)
ωLO is chosen to differ from the signal-carrier frequency ω0 such
that the intermediate frequency ωIF is in the microwave region
(ωIF = 1 GHz).
 Heterodyne receivers are much easier to implement than
homodyne receivers.
 In heterodyne detection, 3dB degradation in sensitivity
compared to homodyne detection.
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13. HETERODYNE DETECTION
 Let us consider the output current at the receiver
 The receiver output current then contain a dc term given by
 The dc current is normally filtered out in the receiver, and IF
current gets amplified. One then recovers the information from
the amplified current using conventional RF demodulation
techniques.
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14. HETERODYNE DETECTION
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15. HETERODYNE DETECTION
Heterodyne detection
 Information can be transmitted through amplitude, phase, or
frequency modulation of the optical carrier wave in heterodyne
detections.
 Heterodyne detection is used for the construction of Doppler
velocimeters and laser range finders and as well as in
spectroscopy (particular LIDAR systems).
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16. DIFFERENCE B/W HOMODYNE AND
HETERODYNE
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17. ADVANTAGES OF HETERODYNE
 Direct encoding of the spectrum of the incoming signal over a
given wavelength range.
 Signals are down-converted to frequencies where low noise
electronics can be used.
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18. APPLICATIONS OF HETERODYNE
 The heterodyne detection used in radio as they boost the angular
resolution through inter-ferometry.
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19. REFERENCE
 optical-fiber-communications-by-gerd-keiser_2
 https://youtu.be/h-M270YlImk
 https://electronics-club.com/difference-between-
homodyne-and-heterodyne-detection/
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