InP-Based Photonic Integrated Circuits
CLEO’08 Tutorial CTuBB1
Larry A. Coldren ECE and Materials Departments University of California, Santa Barbara, CA 93106 coldren@ece.ucsb.edu
Acknowledgements: Chris Doerr, Alcatel-Lucent; Chuck Joyner, Infinera; UCSB colleagues
Coldren CLEO Tutorial 050608
Outline/Contents • Integration Platforms/Technology • Transmitters • Receivers • Transceivers/Wavelength Converters • Conclusions
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Indium phosphide
III-V material
Zincblende structure
(two intersecting FCC lattices, one for In and one for P)
Lattice constant = 5.87 A at 300K
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InGaAsP/InP lattice-matched alloys
InGaAsP lattice-matched to InP
1.31 1.55
λg(µm) = 1.24/ Eg(eV)
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Lateral waveguides/couplers
Waveguide cross sections
InP InGaAsP
Deeply-etched Ridge Buried channel Surface ridge Buried rib
Higher index contrast MMI coupler
WMMI Pin LTUNE
WWG Pout
LMMI
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Modulators
Electro-absorption modulator (EAM)
~ 100 µm Can use quantum-confined Stark effect for large ∆α Data Electro-absorption modulator (EAM)
Mach-Zehnder modulator (MZM) lumped
~ 500 µm Can use quantum-confined Stark effect with larger ∆λ
Data
Traveling-wave linear phase modulator
~4 mm
Data
RF and optical velocities difficult to match
(Can get away with lumped phase modulator up to ~10 GHz) (Also, current injection for < 1 GHz)
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Active-Passive (axial) Integration
Desire lossless, reflectionless transitions between sections
Vertical Twin-Guide Twin-
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Partially transmissive mirrors
• Coupling mirrors between integrated active and passive sections
Etched grooves
Tunable single frequency Laser-modulator Laser-detector
First integrated InP (laser – X) devices
L.A. Coldren, B.I. Miller, K. Iga, and J.A. Rentschler, “Monolithic two-section GaInAsP/InP active-optical-resonator devices formed by RIE,” Appl. Phys. Letts., 38 (5) 315-7 (March, 1981).
DBR gratings and vertical couplers
Tunable single frequency Combined integration technologies
Y. Tohmori, Y. Suematsu, Y. Tushima, and S. Arai, “Wavelength tuning of GaInAsP/InP integrated laser with butt-jointed built-in DBR,” Electron. Lett., 19 (17) 656-7 (1983). Coldren CLEO Tutorial 050608
QWI For Multiple-Band Edges/Single Growth
•
Simple/robust QWI process
– Ability to achieve multiple band edges with a single implant
E. Skogen et al, “Post-Growth Control of the Quantum-Well Band Edge for the Monolithic Integration of Widely-Tunable Lasers and Electroabsorption Modulators,” IEEE Coldren CLEO Tutorial 050608 J. Sel. Topics Quantum Electron.
PIC Transmitters
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Early PIC transmitter: EML
EML = electroabsorption-modulated laser
DFB laser
EAM
M. Suzuki, et al., J. Lightwave Technol., LT-5, pp. 1277-1285, 1987. Coldren CLEO Tutorial 050608
Early PIC with wavelength-selectable laser and EAM
M. G. Young, et al., Electron. Lett., 31, pp. 1835-1836, 1995. Coldren CLEO Tutorial 050608
Early PIC with widely-tunable laser and EA or MZ-modulator
SGDBR+X: (UCSB’91-’08 Agility’99-’05
SG-DBR Laser Rear Mirror
-140 -150 -160 SMSR (dB) 55 50 45
JDSU’05 )
SGDBR/SOA (no mod.)
∆ν (MHz) 3 2 1
• Vernier sampled DBRs and phase set wavelength • External SOA controls amplitude
MZ Modulator Amplifier Front Mirror
Gain Phase
RIN (dB/Hz)
MQW active regions
Sampled gratings
19dBm 16dBm 13dBm 192
FIBER POWER
193 194 195 Channel Frequency (THz)
196
10 Gb/s Optical Duobinary Transmission
0 km
200 km
Courtesy of JDSU + UCSB
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L.A. Johansson, L.A. Coldren, P.C. Koh, Y.A. Akulova, and G.A. Fish, "Transmission of 10 Gbps Duobinary Signals Using an Integrated Laser-Mach Zehnder Modulator" Optical Fiber Communication (OFC), paper no. OThC4, San Diego, CA, MARCH, 2008
SGDBR- Mach-Zehnder transmitter stage of wavelength converter
Series-push-pull SGDBR-MZ transmitter
• • • • Integrated load R and bypass C 30 GHz Bandwidth 40 Gb/s error free operation Low/negative chirp
Transmitter
DQW
Receiver
MZ small-signal bandwidth
40 Gb/s eyes
Negative chirp result
10 Gb/s Eyes 0 km 25 km 50 km
(km)
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A. Tauke-Pedretti, M.N. Sysak, J.S. Barton, L.A. Johansson, J.W.Raring, and L.A. Coldren, “40 Gbps series-push-pull Mach-Zehnder Transmitter on a dual-QW integration platform,” Photon. Tech. Lett., 18 (18) 1922-4 (2006).
40 Gb/s SGDBR/TW-EAM
40 Gb/s NRZ 1533 nm
1543 nm
1559 nm
• Integration of traveling-wave EAM designs with SG-DBR laser • Modulation efficiency 15 – 20 dB/V over the tuning range • Open eyes at 40 Gb/s for all wavelengths
– 6 – 10 dB extinction with 2.1V
M. M. Dummer, J.Klamkin, E. J. Norberg, J. W. Raring, A. Tauke-Pedretti, and L A. Coldren, “ Periodic Loading and Selective Undercut Etching for High-Impedance Traveling-Wave Electroabsorption Modulators”, OFC’08, March, 2008. Coldren CLEO Tutorial 050608
Recent multi-channel transmitter PIC
10 x 10 Gb/s Electrical Input AWG Multiplexer CH1
Optical Output l1... l10 10 x 10 Gb/s
DC Electrical Bias and Control
CH10
ra EA y M Ar Tu ra y na ble D A FB OP rray M Ar ray Ar VO A
R. Nagarajan, et al., Sel. Top. Quant. Electron., 11, pp. 50-65, 2005. Coldren CLEO Tutorial 050608
Slide courtesy of C. Joyner
Multi-channel transmitter results
10
Optical Power Monitor Photocurrent (arbitrary units)
2
C hannels 1-10
10 2 3
Normalized Power (dB) -10 -20 -30 -40 -50 -60 -70 -80 1526
DFB Voltage (V)
4 5
6
7 8 9 10
1.5 1 0.5 0
Large-Scale Photonic Integrated C ircuit 10-C hannel D W D M T ransm itter D C (20°C )
0 50 100 150 200 250 300
-0.5 -1 -1.5
D FB Forw ard C urrent (m A )
1530
1534 1538 Wavelength (nm)
1542
Normalized Transfer Function (dB)
Normalized Electrical Response Normalized Electrical Response (dB) (dB)
3 0
LS-PIC DWDM Transmitter EAM Frequency Response (-3V)
0 -4 -8 -12 -16 -20 0 1 2 Negative Bias (V) 3 4
EAM transfer function
-3 -6 -9
Channels 1-10
0 5 10 Frequency (GHz) 15 20
-12
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Slide courtesy of C. Joyner
Traveling-wave MZM DQPSK PIC
Sub-MZMs
I I
π/2 phase shifters
50-Ω termination Modulated signal
CW light
Q
Q
50-Ω termination
DC bias
Wavelength range: L-band (λPL = 1.47 µm) RF input: Differential EO interaction length: 3 mm (Sub-MZMs), 1.5 mm (π/2-phase shifter) Chip size: 7.5 mm x 1.3 mm
Courtesy of N. Kikuchi
N. Kikuchi, ECOC, 10.3.1, 2007. Coldren CLEO Tutorial 050608
Uses novel n-p-i-n structure
TW-MZM DQPSK Results
Driving voltage: 3 Vpp (Vπ ) for each
40 Gbit/s
data data
Received eye patterns
80 Gbit/s
LD
λ = 1580 nm data data
+/-π/4
(+π/4)
MZDI
Fiber output power (dBm)
-10 -20 -30 -40 -50 -60 -70 -80 189.5 189.6
Balanced receiver
40 Gbit/s
(-π/4)
(10 ps/div)
189.7
189.8
Frequency (THz)
Slide courtesy of N. Kikuchi
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Recent InP DQPSK modulator PIC
1.7 mm
Star coupler 37%
Ground pad EAM #1 0° 225°
EAM pad
DC bias pad Au p+ InGaAs 2.2 µm p InP i InP
26%
Inlet width ratio chosen to achieve desired splitting ratio
BCB
8 QWs n InP
37% EAM #2
+90°
Set to 90° bias by design (using extra path length in one arm)
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C. R. Doerr, et al., OFC, PDP33, 2007.
DQPSK modulator results
-2
Quad #1 Quad #2
10 ps
Log (bit error rate)
-3 -4 -5 -6 -7
215-1 PRBS -30
Power (dBm)
-40 -50 -60 1554.4 1554.6 1554.8 1555 1555.2
-8 79.6 Gb/s (OC-1536) -9 15 20 25 OSNR (dB)
Wavelength (nm)
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C. R. Doerr, et al., OFC, PDP33, 2007.
Receivers
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Early PIC multi-wavelength receiver
8 × 2 nm
J. B. D. Soole, et. al., Electron. Lett., pp. 1289-1290, 1995. Coldren CLEO Tutorial 050608
Recent multi-channel receiver PIC
CH1 AWG De-Multiplexer
Optical Input l1... l10 10 x 10Gb/s
10 x 10Gb/s Electrical Output
PIN Photodiode Array
CH10
Slide courtesy of C. Joyner
R. Nagarajan, et al., Sel. Top. Quant. Electron., 11, pp. 50-65, 2005. Coldren CLEO Tutorial 050608
Multi-channel receiver results
Normalized Photoresponse (dB)
5 -5 -10 -15 -20 -25 -30 -35 1528
1533 1538 1543 Wavelength (nm) 1548
Polarization Dependent Loss (dB)
0
1.0 0.8 0.6 0.4 0.2 0.0 0 1 2 3 4 5 6 7 8 Channel Number 9 10
Slide courtesy of C. Joyner
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Early heterodyne receiver PIC
Heterodyne receiver for coherent
LO laser
T. L. Koch, et al., Electron. Lett., 25, pp. 1621-1622, 1989. Also, H. Takeuchi, et al., IEEE Photon. Tech. Lett., 1, pp. 398-400, 1989. Coldren CLEO Tutorial 050608
Balanced receiver for phase modulated signals with feedback
is ~ sin(ϕsignal - ϕLO) Photocurrent
1
Large-signal modulation •Open loop •Closed loop
Transmission
0 .5
0
M Z p h ase (r Signal – LO phasea d ) difference
0
π
2π
• Signal mixed with local oscillator to demodulate optical phase
– Detected differential photocurrent represents signal-LO phase difference – Response of interferometer based demodulator is sinusoidal
• With feedback the differential photocurrent is reduced by the loop gain: 1/(1+T)
– Hybrid integrated EIC* provides transconductance amplification – Closely track received optical phase to operate within linear regime
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L.A. Johansson, H.F. Chou, A. Ramaswamy, L. A. Coldren, and J.E. Bowers, “Coherent optical receiver for linear optical phase demodulation,” Proc. MTT-S Microwave Sym., Tu3D-01 (June, 2007).
Balanced PD implementation
Adjacent UTC-PDs electrically isolated with high energy Helium implantation
– – Rshn Rshp = 5.28 MΩ/sq = 2.46 MΩ/sq PD 1 Interconnect
Plan view SEM of BPD
PD 2
PDs connected in series with a monolithic metal interconnect
Cross-sectional schematic of series-connected PDs
IV curves of PDs
Ti/Pt/Au P-metal and interconnects
Ni/AuGe/Ni/Au N-metal
Helium implantation to substrate for isolation
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UTC-PD design
p+ InGaAs Absorber n-InP Collector InGaAsP MQW and Waveguide BPM simulation illustrating absorption profile
2D overlap of mode with absorber: 2.8%
1D mode profile
QW 4 µm wide 9 µm wide
Absorber
Barrier
Long absorption profile and wide input reduce front end saturation
J. Klamkin, A. Ramaswamy, L. A. Johansson, H-F Chou, M.N. Sysak, J. W. Raring, N. Parthasarathy, S.P. DenBaars, J.E. Bowers, and L. A. Coldren, “High-output-saturation and high-linearity uni-traveling-carrier waveguide photodiodes,” Photonics Tech. Letts. 19 (3) 149-151 (Feb. 2007).
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Saturation characteristics
UTC CC-UTC
f = 1 GHz
f = 1 GHz
Isat = 65 mA • •
Isat = 63 mA Appears less linear More bias dependent
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J. Klamkin, Y-C Chang, A. Ramaswamy, L. A. Johansson, J.E. Bowers, S.P. DenBaars, and L. A. Coldren, “Output saturation and linearity of waveguide uni-traveling-carrier photodiodes,” J. Quantum Electron,. 44 (4) 354-359 (Apr., 2008).
Phase modulator design
15 QW - Γ2D = 20.7 %
Push-pull modulation
QW
Barrier
VπDC = 2.1 V•mm
• •
∆φ
Linear term doubled, even order terms cancelled Third order distortion suppressed with bias optimization
∆φ
Linearized output characteristic [∆φ(∆V) – ∆φ(-∆V)]
∆V V0
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∆V V V0 V
MMI coupler design-surface ridge
Surface ridge BPM simulation
Integrated pad for current injection tuning
WMMI Pin LTUNE WWG Pout
LMMI
WMMI 8 µm
WWG 2.5 µm
LTUNE 100-300 µm
LMMI 345 µm
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Deep-etched 2x2 MMI coupler
Deep ridge
Shorter MMI coupler Shorter bends and tapers
Deep Etched Ridge Surface Ridge WMMI WWG
WMMI
WMOD LMM
I
WWG 1.8 µm
LMMI 130 µm
WDET
9 µm
DR MMI coupler
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DR to SR transition
PIC receiver/QWI process flow
MQW ERM (as grown) Low loss passive waveguide Offset ternary detector
InP
n- - InGaAsP WG n+ - InP n++- InGaAs or InGaAsP contact
n+ - InP Semi-Insulating InP substrate
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PIC receiver/QWI process flow
MQW ERM (as grown) Low loss passive waveguide Offset ternary detector
InP
n- - InGaAsP WG n+ - InP n++- InGaAs or InGaAsP contact
n+ - InP Semi-Insulating InP substrate
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PIC receiver/QWI process flow
MQW ERM (as grown) Low loss passive waveguide Offset ternary detector
n- - InGaAsP WG n+ - InP n++- InGaAs or InGaAsP contact
n+ - InP Semi-Insulating InP substrate
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PIC receiver/QWI process flow
MQW ERM (as grown) Low loss passive waveguide Offset ternary detector
p+ - InP p++ - InGaAs absorber InP collector n- - InGaAsP WG n+ - InP n++- InGaAs or InGaAsP contact
n+ - InP Semi-Insulating InP substrate
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PIC receiver/QWI process flow
MQW ERM (as grown) Low loss passive waveguide Offset ternary detector
p+ - InP p++ - InGaAs absorber InP collector n- - InGaAsP WG n+ - InP n++- InGaAs or InGaAsP contact
n+ - InP Semi-Insulating InP substrate
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PIC receiver/QWI process flow
p++ - InGaAs contact p+ - InP p+ - InP p++ - InGaAs absorber InP collector n- - InGaAsP WG n+ - InP n++- InGaAs or InGaAsP contact
n+ - InP Semi-Insulating InP substrate
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PIC receiver/QWI process flow
p++ - InGaAs contact p+ - InP p+ - InP p++ - InGaAs absorber InP collector n- - InGaAsP WG n+ - InP n++- InGaAs or InGaAsP contact
n+ - InP Semi-Insulating InP substrate
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SOA-PIN “all-photonic” receiver for transceiver/wavelength-converter PIC
• Semiconductor Optical Amplifiers (SOAs)
– High gain
• Low input powers - increases conversion efficiency
– High saturation power
• Prevents pattern dependence • Aids in conversion efficiency
• Photodetectors
– – High bandwidth Large absorption coefficient
• Smaller devices
Transceiver PIC
A. Tauke-Pedretti, M.M. Dummer, M.N. Sysak, J.S. Barton, J.W. Raring, J. Klamkin, and L.A. Coldren, “Monolithic 40 Gbps Separate Absorption and Modulation Mach-Zehnder Wavelength Converter,” Proc. OFC, paper no. PDP36, Anaheim, CA (March 25-29, 2007)
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Simple offset QW integration platform
Use simplest integration platform to do the job
Active
InGaAs p-contact p-InP 7 – Quantum Wells 1.4 Q InGaAsP WG
Passive
Offset well
Gain for SGDBR and SOA λPL = 1550 nm
Semi-insulating substrate
Reduces capacitance Isolates absorber and modulator grounds
n-InP InGaAs n-contact n-InP Fe doped InP substrate
Single blanket regrowth
InP cladding InGaAs contact layer
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Offset QW receiver design
• Receiver SOA
– Offset quantum wells provide gain – Linearly flared waveguide
• Quantum-well PIN detector
– Reverse biased laser QW provide high absorption coefficient – Wide front end prevents saturation – Tapering reduces capacitance
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SOA gain and linearity
• High-gain pre-amps improve conversion efficiency
– 23 dB of gain was achieved
• High saturation power preserves signal quality / reduces pattern dependence
– 16 dBm of unsaturated output power with a 12 µm width – 13 dBm (20mW) 1 V rms (2.8 Vpp) over 50 Ω
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Tranceivers/wavelength converters
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Wavelength converter/SOA-PIN receiver & SGDBR-Mach Zehnder transmitter
• • • • • • Photocurrent driven 35 µm QW absorption region in receiver
– Tapered for reduced capacitance
300 µm traveling-wave Mach-Zehnder modulation region
– Series-push-pull design to maximize bandwidth
Data format and rate transparent No optical filter required Integrated termination resistor and bypass Capacitor
– No external bias tees used
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Mach-Zehnder Wavelength Converter
Current from absorber drives MZM
WC Performance
• • 40 Gb/s NRZ operation <2.5 power penalty for varying input and output wavelengths DQW
Constant input to varying output
Varying input to constant output
1529 nm
1545 nm
1561 nm
Back to back
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A. Tauke-Pedretti, M.M. Dummer, M.N. Sysak, J.S. Barton, J. Klamkin, J.W. Raring and L.A. Coldren, “Separate Absorption and Modulation Mach-Zender Wavelength Converter,” J. Lightwave Tech., 26, (1), 91-98 (Jan. 2008)
QWI+ widely-tunable transceiver/ SOA-PIN & SGDBR-EAM
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J.W. Raring, and L.A. Coldren, “40-Gb/s Widely Tunable Transceivers,” IEEE J. Sel. Topics Quantum Electron., 13, (1), pp. 3-14, (January/February 2007)
Transceiver chip architecture
• Low confinement SOAs, UTC photodiodes, and QW EAMS integrated with SG-DBR lasers Widely-tunablemodulator 175µM QW EA Psat SOA • High photodiode UTC gain/high SGDBR laser
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Tranceiver 40Gb/s receiver performance
• Chip-Coupled Receiver Sensitivity at 40 Gb/s
– 250µm/1650µm error-free (1E-9) at -16.8dBm – 400µm/1500µm error-free (1E-9) at -20.3dBm
• 40 Gb/s eye diagams
– 25Ω effective load
– ~-19.8 dBm sensitivity @ 40Gb/s – 500mV amplitude – Integrated with 40Gb/s transmitter
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QWI+ tranceiver 40 Gb/s transmit and receive functionality
• Transceiver #1
– Transmitter: 75µm EAM DC = 3.5-4.75V: VPtoP = 2.5 – Receiver: SOA design #1 with 30µm UTC
• Transceiver #2
– Transmitter: 175µm EAM DC = 2.5-4.5V: VPtoP = 2.5 – Receiver: SOA design #2 with 40µm UTC
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SOA-PIN & SGDBR-TW/EAM wavelength converter
• Data format and rate transparent 5-40Gb/s • No filters required (same λ in and out possible) • On-chip signal monitor • Two-stage SOA pre-amp for high sensitivity, efficiency and linearity • Traveling-wave EAM with on chip loads • Only DC biases applied to chip • 40 nm wavelength tuning range
M. Dummer et al. OFC 2008 OThC6 (2008) Coldren CLEO Tutorial 050608
LASOR 40 Gb/s Packet Forwarding Chip – OQW & Butt-joint regrowth
• • • • Fast Tunable SGDBR Laser Differential Mach-Zehnder Interferometer SOA Wavelength Converter (‘all-optical’) Preamplifier SOAs Integrated delay
Output 1550nm
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V. Lal, M. L. Masanovic, J. A. Summers, G. Fish, and D. J. Blumenthal, "Monolithic Wavelength Converters for High-Speed Packet-Switched Optical Networks," JSTQE, 13, pp. 49-57, 2007.
Tunable wavelength converter using AWG-laser + SOA + filter
lsig
• Fast-tunable 40G wavelength converter
– 8-channel multi-frequency laser (MFL) – λ-conversion via nonlinear SOA and delay filter
WC
WC-SOA
MZI
lsig & lj
lj j = 1..8
MFL
SOA
InP
SOA Array
Converted optical eye diagram at 40 Gb/s
W C
Laser
6.5 mm
P. Bernasconi, et al., PDP16, OFC 2005. Coldren CLEO Tutorial 050608
Slide courtesy of P. Bernasconi Alcatel-Lucent—IRIS Project
4.0 mm
Conclusions
• Multi-functionality InP-based Photonic ICs can now be made with state-of-the-art performance and reductions in power dissipation, size, and perhaps cost in sufficient numbers. • Multi-channel WDM transmitters, receivers, and wavelength converters demonstrated • Many future PICs now on the ‘drawing board’
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