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Page 1: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Large-Signal Modeling on Device Level:

Intermodulation Distortion andEye-Diagrams of SemiconductorLasers

S. Odermatt, B. Witzigmann, B. Schmithuesen

ETH Zürich

Page 2: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

© 2006 Synopsys, Inc. (2)

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Large-Signal Characteristics

Digital Applications:

- Resonance Overshoot

- Eye-Diagram

Vez, Proc. SPIE 4942, pp.29-42, 2003

Analog Applications:

- Intermodulation Distortion

- Spurious Free Dynamic Range

Carlson, IEEE JTL, 20 (9), 1740, 2002

Large-Signal Modeling:

- So far, theoretical description on 0-dimensional rate-equation-models, “device-level” link missing

- This work: Larg-Signal modeling on device level using harmonic balance method

Page 3: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Content

• Introduction Optoelectronics and Multi-dimensional VCSEL Simulation

• Multi-Tone Harmonic Balance Method Introduction

Single vs Multi-Tone

Performance: transient vs. HB

• Application Examples Analog: Intermodulation distortion

Digital: Eye Diagram

• Conclusion

Page 4: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

© 2006 Synopsys, Inc. (4)

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Synopsys Sentaurus Device:Optoelectronic Applications

CIS & CCD

solar cell

Laser

Photo diode

(O)LED

Page 5: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

© 2006 Synopsys, Inc. (5)

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VCSEL Simulation

Gain Mode Stability SS Dynamics

Optics Electro-Thermal Transient Heating

Page 6: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

© 2006 Synopsys, Inc. (6)

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Harmonic Balance Method

Note: The system to solve is O(H^2) bigger than the DC system memory consumption!!

Expand the source w(t) and solution x(t) into Fourier series

Assume a system of nonlin. Equations in the following form

And solve the system in the frequency domain for the Fouriercoefficients Xh of the solution vector

Page 7: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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HB for Electro-Thermal Laser Model

• Poisson:

• El./Hole DD:

• Heat Diff.:

• Phot. Rate:

• Phot. Phase:

Page 8: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Single-Tone vs. Multi-Tone HB

Input Current:

Optical Power:

!

I(t) = I0 + I1 sin("t)

...)3sin()2sin()sin()( 3210 ++++= tPtPtPPtP !!!

Input Current:

Optical Power:

....)sin()sin()( 21110 +++= tItIItI !!

...)2sin(

)]2sin([)]2sin([

)sin()sin()(

120

21)1(21212

22110

++

!+!+

++=

!!

tP

tPtP

tPtPPtP

"

""""

""

Multi-Tone

Single-Tone

Presented at NUSOD 2006

NEW in Synopsys SentaurusDevice 2007.03

Page 9: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Transient vs. Harmonic Balance

very high**lowPerformance/runtime efficiency

very high**mediumDigital modulation performance

very high**very low*Analog modulation performance

highmediumMemory consumption

difficultsimpleImplementation aspects

HBtransientFeature

* 2-tone example with f1=1GHz and ∆f=1KHz requires >>f1/ ∆f=1e6 time steps for a singlepoint.** HB schemes allow to “ramp/sweep” modulation signal parameters such as frequencies oramplitudes.

Page 10: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Application Example

• VCSEL GaAs/AlGaAs

2-D simulation domain

Electro-opto-thermal

Many-body Gain Model

• Analog Modulation: Intermodulation Distortion

• Digital Modulation: Eye-Diagram

Page 11: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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MQW AlGaAs VCSEL

anode

cathode

oxideMQWactive

Ith ~ 2.0 mAλ ~ 850 nm

Iop = 6 mA (T=300 K)

Pop = 2.5 mW

Pow

er [

mW

]

Current [mA] 2.0 4.0 6.0

2.0

1.0

0.0V

olta

ge [V

]

3.0

2.0

1.0

Page 12: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Analog: Intermodulation Distortion

Input Current: ....)sin()sin()( 21110 +++= tItIItI !!

Optical Power:

...)2sin(

)]2sin([)]2sin([

)sin()sin()(

120

21)1(21212

22110

++

!+!+

++=

!!

tP

tPtP

tPtPPtP

"

""""

""

Analog Modulation schemes have closelyspaced channels (∆f ~ kHz)

Non-linearities introduce cross-talk(IMD3,IMD5)

IMD3 and IMD5 should be as low aspossible

Page 13: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Analog: Intermodulation Distortion

MQW AlGaAs VCSELIop = 6 mA

∆f = 2 kHz

Two cases:

f1=5.0 GHz,

f1=1.0 GHz

For the higher modulationfrequency, the power inthe higher harmonics isstrongly enhanced.

(reason: resonance effects,fr~6 GHz at I=6mA)

P1

P3

P5

Page 14: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Digital Modulation: Eye-DiagramThe eye-diagram is the most

important laser characteristicin digital modulationapplications.

Vez, Proc. SPIE 4942, pp.29-42, 2003

In order to obtain a “open eyes”,the input signal may bedesigned using advancedcurrent-peaking schemes, inaddition to device design.

In this work, we chose a simplerectangular input signal andapproximate it with a finiteFourier series using 20coefficients.

Note that the Harmonic Balance method iseven better suited to support currentpeaking schemes do to it’s periodicnature.

Current-peakingscheme

Christen, Micr. And Opt. Tech. Letters, 38 (4), 304, 2003.

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Eye-Diagram (without jitter and noise)

Modulation with 1 GBit/s

f < fres

Strong overshoots

“Open Eye”

Modulation with 10 GBit/s

f > fres

Closed eye

Large phase delay(~175º)

Fourier coefficients forinternal densities,potentials etc. can beanalyzed!

(schematic)

~175º

~20º

Page 16: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Summary

• Harmonic Balance Method for simulation of Large-Signal characteristics

• Consistent link between “System Specs” and microscopic description ondevice level using Synopsys Sentaurus Device framework

• Investigation of Analog and Digital modulation schemes possible

• VCSEL Application examples Analog Modulation: Intermodulation distortion

Digital Modulation: Eye-Diagrams

Outlook:Systematic investigation of eye-diagrams on device level including noise and jitter,physics of Fourier coefficients of microscopic quantities

Page 17: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

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Backup

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Figure of Merit of Non-Linearities:Intercept Points


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