laser transmitter adaptive feedforward linearization

22
ASEAN IVO Forum 2015 Laser Transmitter Adaptive Feedforward Linearization System for Radio over Fiber Applications Authors: Mr. Neo Yun Sheng Prof. Dr Sevia Mahdaliza Idrus Prof. Dr Mohd Fua’ad Rahmat Dr Atsushi Kanno

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Page 1: Laser Transmitter Adaptive Feedforward Linearization

ASEAN IVO Forum 2015

Laser Transmitter Adaptive

Feedforward Linearization System for

Radio over Fiber Applications

Authors:

Mr. Neo Yun Sheng

Prof. Dr Sevia Mahdaliza Idrus

Prof. Dr Mohd Fua’ad Rahmat

Dr Atsushi Kanno

Page 2: Laser Transmitter Adaptive Feedforward Linearization

Background

Optical Feedforward Linearization System

Feedforward Loops Setup

Experimental Results

Adaptive Control System

Conclusion

Contents

2

Page 3: Laser Transmitter Adaptive Feedforward Linearization

Background Radio over Fiber Technology:

3

Smaller cell size:

- Fiber closer to users

- Less user per cell

- Better frequency

reusability

- Reduced RF power

(EMI)

Page 4: Laser Transmitter Adaptive Feedforward Linearization

4

Consolidating signal

processing functions:

- Small RAU size and

power consumptions

- Easy installations

and maintenance

- Perfect coordination

between RAUs

- Multi-service

operation

- System upgradability

and reconfigurability

Background

Page 5: Laser Transmitter Adaptive Feedforward Linearization

RoF – Basic Structure of System

Mobile

wave

Terminal

Mobile

wave

Terminal

Base

Station

RF Data

Input

Fiber

Central

Station RF Data

Output

Optical

Transceiver

RF Data

Output

Optical

Transceiver

RF Data

Input

Radio System

Fiber link

5

Background

Page 6: Laser Transmitter Adaptive Feedforward Linearization

Background Impairments in RoF Links:

Important link parameters:

– RF gain, Noise figure (S/N

ratio)

– linear dynamic range

– bandwidth (bandwidth fiber-

length product)

Key issues:

– high-speed, high-efficiency, high-

power transmitters and receivers

– devices and fibers nonlinearities

– Low/controlled chirp transmitters

(fiber dispersion)

Optical

Transmitter

Optical

Fiber Channel

Optical

Receiver

Optical

Amplifier

•ASE Noise •Attenuation

•Dispersion

•HD

•IMD

•RIN

•Shot Noise

•Thermal Noise

optical signal

RF in RF out

CNR CNR

6

Page 7: Laser Transmitter Adaptive Feedforward Linearization

Rate Equation for Laser Diode

Dynamic Nonlinear System:

Produce Harmonic Distortion

and Intermodulation Distortion

7

Background

Page 8: Laser Transmitter Adaptive Feedforward Linearization

Linearization method Operating

frequency

Correction

Bandwidth

Correction

capability (dB)

Electronic predistortion Up to 14 GHz Up to 500 MHz 10 - 25

Feedback Up to 2.5 GHz Narrow band 15 - 25

Optical injection Up to 18 GHz NA 10 - 25

Dual parallel modulation Up to 8 GHz Narrow band 20 - 30

Quasi feedforward Up to 2.1 GHz NA 17 - 35

Feedforward 50 MHz–18 GHz Up to 850 MHz Up to 38

8

Background Linearization Techniques: Quantitative Comparison

Page 9: Laser Transmitter Adaptive Feedforward Linearization

9

Background

Feedforward: Need for Adaptation

- Feedforward is a sensitive scheme, where the magnitude, phase shift

and propagation delay along the feedforward path has to be properly

tuned to optimize the distortion cancellation of the system.

- The magnitude and phase adjustments are also bound to be disrupted

by any sort of drift and process variations such as temperature effect,

laser aging, and input signal variations

- For practical implementations the feedforward system has to be real-

time adaptive in terms of its component parameters.

Page 10: Laser Transmitter Adaptive Feedforward Linearization

10

Laser Diode

1 (LD1) Photo-

detector 2 Fixed gain

amplifier 3

Electrical path

Optical path

The optical signal is converted back to RF signal by

PD2 and amplified. The output RF signal can be

visualized in an RF spectrum analyzer. Input RF

signal

For an uncompensated optical link, the input RF

signal directly modulate the primary laser diode,

and the optical output will be transmitted through

optical fiber.

Output

RF signal

Optical Feedforward

Linearization System

s

s+d

Page 11: Laser Transmitter Adaptive Feedforward Linearization

11

Power

splitter 1

Vector Modulator

1 +

Laser Diode

1 (LD1)

Electrical

Delay

Photo-detector

1 (PD1)

Power

combiner

Optical

Coupler 1

Photo-

detector 2

Fixed gain

amplifier 1

The input RF signal is split to obtain a copy of

reference signal.

An optical coupler diverted part of the optical

signal from LD1 to obtain a sample of distorted

signal, and it is converted back to RF signal by

PD1 .

The distorted signal sample is then cancelled with

the reference signal at Power combiner 2, leaving

only the distortion products of LD1.

Vector modulator 1 is used to match the magnitude and

phase of the reference signal with the distorted signal

sample, while the electrical delay is used to match the

signal delay between both path to ensure an effective

cancellation over a wide bandwidth.

This loop of cancelling the desired signal to isolate the

distortion product is called signal cancellation loop

(SCL).

Input RF

signal

Fixed gain

amplifier 3

Output

RF signal

Electrical path

Optical path

Optical Feedforward

Linearization System

s+d

s

s+d

s

d

Page 12: Laser Transmitter Adaptive Feedforward Linearization

12

Power

splitter 1

Vector Modulator

1 +

Vector Modulator

2

Laser Diode

1 (LD1)

Electrical

Delay

Photo-detector

1 (PD1)

Power

combiner

Optical

Coupler 1 Optical

Coupler 2

Laser

Diode 2

(LD2)

Photo-

detector 2

Fixed gain

amplifier 1

Fixed gain

amplifier 2

Optical

Delay

The distortion products from

Power combiner 2 are then

magnitude and phase adjusted by

Vector Modulator 2 before it

directly modulates the secondary

laser diode LD2.

The compensating optical

signal is then combined

with the delayed optical

signal of LD1 at Optical

coupler 2, hence

compensating the distortion

product from LD1.

This loop of cancelling the distortion product from the

primary laser diode output is called error cancellation

loop (ECL).

Input RF

signal

Fixed gain

amplifier 3

Output

RF signal

Electrical path

Optical path

Optical Feedforward

Linearization System

s

s+d

s+d

s

d

d

s

s+d

Page 13: Laser Transmitter Adaptive Feedforward Linearization

13

Feedforward Loops Setup Magnitude and Phase Matching:

Problem Nonideality of vector modulator (magnitude adjustment

inconsistent over different phase adjustments)

i) Adjust the reference signal magnitude close to the original signal

ii) Adjust the reference signal phase till the two signals are in anti-phase

Solution:

f1

A1 dB A2 dB + G dB

f1 f1

A1 dB

x dB

𝐺𝑖+1 𝑑𝐵 = 𝐺𝑖 𝑑𝐵 ± 20 log10(1 + 10𝑥𝑑𝐵20 )

G = vector modulator gain

Page 14: Laser Transmitter Adaptive Feedforward Linearization

14

Feedforward Loops Setup Propagation Delay Matching:

f1 f1 + ∆f

A1 dB

f1 f1 + ∆f

A1 dB

Cancellation between two identical signals separated by a propagation delay of ∆t :

f1 f1 + ∆f

A1 dB

x dB

signal 1 signal 2 ∆t

The propagation delay, ∆t can be calculated as :

∆𝑡 =1

𝜋∆𝑓∙ sin−1(±

1

2∙ 10

𝑥𝑑𝐵20 )

The path length difference,

∆L can be calculated as : ∆𝐿 = ∆𝑡 ∙ 𝑐 , where c is the speed

of light constant

Page 15: Laser Transmitter Adaptive Feedforward Linearization

15

Experimental Results

Device: EA modulator integrated DFB laser diode module λ LD1= 1547 nm , λ LD2= 1549 nm

Operating Freq: 2.3 GHz Input power: 10 dBm

Laser transmitter output before feedforward

linearization (10 MHz freq spacing) Laser transmitter output after feedforward

linearization (10 MHz freq spacing)

The IMD3 level for the uncompensated system is about -21 dBc. A reduction of 14 dB has

been achieved for both IMD3 products, equivalent to a bandwidth of 40 MHz.

Page 16: Laser Transmitter Adaptive Feedforward Linearization

16

Experimental Results

Laser transmitter output before feedforward

linearization (1 MHz freq spacing)

Laser transmitter output after feedforward

linearization (1 MHz freq spacing)

By narrowing down the freq spacing to 1 MHz, the achievable reduction for both IMD3

products has increased to 20 dB. The system is expected to achieve a larger margin of

reduction by further improving the path delay matching.

Page 17: Laser Transmitter Adaptive Feedforward Linearization

17

Adaptive Control System

Power

splitter 1

Vector Modulator

1

+

Vector Modulator

2

Laser Diode

1 (LD1)

Electrical

Delay

Photodetector

1 (PD1)

Power

combiner

2

Optical

Coupler

1 Optical

Coupler

2

Power

splitter 2

Laser

Diode 2

(LD2)

Down-convertor 2

Adaptive Controller

Downconvertor 3

Photodetector

2

Fixed gain

amplifier 1

Fixed gain

amplifier 2

Fixed gain

amplifier 3

Power

splitter 1

Down-convertor 1

Power

splitter 3

V1

V2

V3

I1 Q1

I2 Q2

Electrical path

Optical path

Control signal

Optical

Delay

Input RF

signal Output

RF

signal

Page 18: Laser Transmitter Adaptive Feedforward Linearization

18

Adaptive Control System

Least Mean Square (LMS)

Algorithm: Recursive Least Square (RLS)

Algorithm:

Adaptive Algorithms:

(1)

(2)

(3)

Stochastic Deterministic

Low computational complexity High computational complexity

Slower convergence Fast convergence

Mean square error trade-off with

convergence speed

Converge to optimal solution

Fast response to input changes Slow response to input changes

2)(1/)()( nxnnxng

2)1()( nxnn

)()()1()( * nengnwnw

)()(*)1()( * nenxnwnw

Page 19: Laser Transmitter Adaptive Feedforward Linearization

19

Adaptive Control System

LMS RLS

Performance Comparison between LMS and RLS

Signal Cancellation Loop:

The RLS algorithm is converging faster at the beginning, but the

LMS algorithm is settling down more steadily.

Page 20: Laser Transmitter Adaptive Feedforward Linearization

20

Adaptive Control System

Error Cancellation Loop:

LMS RLS

The error cancellation loop input signal is dependent on the output from

SCL, hence it is a time varying signal. It can be seen that the RLS

algorithm has poor convergence towards the steady state, while the

LMS algorithm is still showing a steady convergence.

Page 21: Laser Transmitter Adaptive Feedforward Linearization

21

Conclusion

- The optical feedforward linearization system has achieved a

suppression of 14 dB in IMD3 products over a bandwidth of 40 MHz.

Suppression by a larger margin can be achieved with better delay

matching.

- On the adaptive control part, the LMS algorithm is chosen over the RLS

algorithm in this application because it has shown more stability,

robustness, and less computation demanding.

- The outcome of this project serves as the exploration for a future proof

alternative for the widely researched predistortion technique, where

laser transmitters of even higher performance are in demand for future

wireless communication systems in the long run.

Page 22: Laser Transmitter Adaptive Feedforward Linearization

Thank You