digital optical systems based on coherent and …ocw.umh.es/ingenieria-y-arquitectura/optical...0,...

12
Lecture 2: Digital Optical Systems Optical Communication Systems and Networks 1/ 2. Digital Optical Systems based on Coherent and Direct Detection Optical Communication Systems and Networks

Upload: lamkhue

Post on 21-May-2018

217 views

Category:

Documents


2 download

TRANSCRIPT

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

1/

2. Digital Optical Systems based on Coherent and Direct Detection

Optical Communication Systems

and Networks

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

2/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

2/

Fiber-Optic Communications Systems Govind P. Agrawal, Chapter 10, pp. 478-512, John Wiley & Sons, 2002, Third Edition.

Optical Fiber Communications. Principles and Practice

John M. Senior. Chapter 12, pp.700-767, Ed. Prentice Hall, 1992, Second Edition,

BIBLIOGRAPHY

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

3/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

3/

Modulation formats

• Amplitude modulation A0: ASK, Amplitude-shift keying

• Phase modulation 0: PSK, Phase-shift keying

• Frequency modulation 0: FSK, Frequency-shift keying

• Polarization modulation ê: PoSK, information coded by polarization state (not allowed in optical systems based on fiber)

Most commercial systems are based on ASK (These systems are also known as on–off keying, OOK) IM/DD (intensity modulation and Direct Detection)

First Differential PSK (DPSK) are being deployed recently

Optical carrier: E(t) = A0 cos(0t − 0) ê “1” “0” “1” “0” “1” “0”

Electric signal (Bit sequence)

ASK

PSK

FSK

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

4/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

4/

Direct Detection

E(t)=f(t)cos(t)

i(t)=CE(t) f(t)

Electrical receiver

Amplifiers (& filter/s)

Antenna

ELECTRICAL RECEPTION

weak electric signal

OPTICAL RECEPTION

Optical receiver

Amplifier (& filter/s)

weak electric signal

Lens (Focusing /collimation) i(t)=C|E(t)|2 =CP(t) f2(t)

E(t)=f(t)cos(t)

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

5/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

5/

Photodetectors

Thermal

Variation of radiation makes a change of temperature T (bolometers). They are slow for communication applications

Vacuum devices As the photomultiplier tubes, which have high sensitivity but require high voltages, are expensive, slow and large. They also have difficulty operating at > 1 m

Semiconductors

Photoconductors

Incident radiation causes variation of carriers, which in turn causes the modification of the conductivity of the material. They have low sensitivity

fotodiodes

Direct Detection: Detectors

Best option in Optical Communications

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

6/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

6/

ADVANTAGES:

Coherent detection can provide a potential improvement up to 20 dB in the receiver sensivity unlike direct-detection-based systems

For a given power budget, this would allow to increase the total length of an optical link (or spacing between repeaters/aplifiers)

Higher transmisssion rates over existing optical links without reducing repeater spacing is achieved

Efficent use of the available bandwidth • 6

Allows to transmit simultaneously several carriers (frequency multiplexing)

Channel spacing can be reduced to 1 - 10 GHz.

In IM/DD systems, 100 GHz – channel spacing has been proposed. Latest recomendations (G.694.1) include 50, 25 and 12.5 GHz versions

DISADVANTAGES:

• Receivers become more complex

• Sensitivity to the optical carrier’s phase and frequency degradation in reception

Coherent Systems

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

7/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

7/

Detector

Electronic driver

Local oscillator

Beam combiner

Electrical bit secuence

Received optical signal (modulated)

Diagram of a Coherent Detection System

CW

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

8/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

8/

• The optical carrier carries modulated/coded information (phase and/or frequency)

• At receiver: coherent mixing between the incoming signal and optical wave generated by a stable and reduced spectral width local oscillator.

Incoming signal:

Local oscillator:

• Assuming perfect optical mixing, and recalling than optical power is proportional to the square of the electrical field strength, we have :

– if IF = 0, coherent system with homodyne detection

– if IF 0, coherent system with heterodyne detection

)(exp 0 sss tjAE

)(exp LOLOLOOL tjAE

),cos(2)( LOsIFLOsLOs tPPPPtP

LOIFLOLOss KAPKAP 0

22

Coherent Systems

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

9/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

9/

• When the local oscillator frequency equals to optical carrier frequency: wFI = ws - wOL = 0

• The photocurrent generated by the optical detector is proportional to the optical power (or optical intensity) :

(PLO >> Ps PLO + Ps PLO , where DC can be eliminated)

Assuming: s=LO , there is an improvement of SNR:

Main disadvantage: Very sensitive to phase variations

• Accurate control of LO and s could be a solution unless both do not fluctuate

• Solution: Phase control so that the difference between OL y s remains constant (by using phase locked-loops)

)cos(2)()( LOsLOsLOs PPPPtI

)cos(2)( LOsLOsPPtI

142

22

DetectDirect

DetectHomodyne

s

LO

s

LOs

P

P

P

PP

I

I

This information can not be detected in direct detection systems

Coherent Systems. Homodyne detection

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

10/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

10/

Typically, the local oscillator frequency is chosen so that intermediate frequency values range from 0,1 to 5 GHz.

(following the same considerations we made in homodyne detection)

A SNR improvement is obtained with regard to IM/DD systems. However, this improvement (3dB) is lower compared to the one obtained in homodyne detection

Adventage: Simpler optical receivers

Suitable for optical communications systems

Unable to demodulate directly optical signal to baseband (it is required a previous demodulation from intermediate frequency to baseband in the electrical domain)

)cos(2)()( LOsIFLOsLOs twPPPPtI

)cos(2)( LOsIFLOs twPPtI

Coherent Systems. Heterodyne detection

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

11/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

11/

• Typically, the local oscillator frequency is chosen so that intermediate frequency values range from 0,1 to 5 GHz.

(following the same considerations we made in homodyne detection)

A SNR improvement is obtained with regard to IM/DD systems. However, this improvement (3dB) is lower compared to the one obtained in homodyne detection

)cos(2)()( LOsIFLOsLOs twPPPPtI

)cos(2)( LOsIFLOs twPPtI

Coherent Systems. Heterodyne detection

I Photocurrent which depends on the detection

process (homodyne or heterodyne)

The homodyne case (OL = s) produces an increase of 3dB with regard to the heterodyne case

If the power level PLO dominates and can be controlled:

12

Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

12/ Lecture 2: Digital Optical Systems

Optical Communication Systems and Networks

12/

Diagram of a coherent system based on heterodyne detection

Local Oscillator

Beam combiner

Data out

Incoming optical signal

(modulated)

CW

Bandpass filter

Photodetector

Lowpass filter

subcarrier recovery (IF)

Coherent Systems. Heterodyne detection

12