http://photonics.intec.UGent.bePhotonics Research Group
Silicon Photonics
Roel BaetsGhent University – IMEC
ESA February 9 2006
Photonics Research Group© intec 2005
AcknowledgementsThe Photonic Research Group at Ghent University – IMECThe European Union
IST-PICCO IST-PICMOSIST-ePIXnet
The European Space AgencyThe Belgian IAP-PHOTON networkThe Flemish Institute for the industrial advancement of Scientific and Technological Research (IWT)The Flemish Fund for Scientific Research (FWO-Vlaanderen)The Silicon Process division at IMECThe P-line at IMEC
Photonics Research Group© intec 2005
Outline
Silicon Photonics: why and how?
Passive wavelength routers in Silicon
Active photonic functions in Silicon
Silicon photonics: what for?
Photonics Research Group© intec 2005
Silicon Photonics: why and how?Why?• Functionality + performance• Technology• CostHow?• Wafer-level fabrication• Packaging
Photonics Research Group© intec 2005
Silicon photonicsFunctionality and performance: spectacular breakthroughs in last 2 years• low loss waveguides (IMEC, NTT, IBM…)• compact wavelength routers (IMEC…)• ultra-compact microcavities (U. Kyoto…)• >>10 Gb/s receivers (LETI…)• 10 Gb/s modulators (INTEL, LUxtera…)• Raman Silicon laser (INTEL…)• (velocity tunable) slow light (IBM…)• all-optical switching + λ-conversion (NICT+IMEC…)• integration with CMOS (Luxtera…)
Photonics Research Group© intec 2005
DARPA: EPICObjectives
Si nanophotonics with CMOS processesApplication-specific EPICNew photonic devices in Si (lasers, wavelength converters, amplifiers, ...)
PartnersMITLuxteraSunFreescale
Budget: 12M$ www.darpa.mil/mto/epic
Photonics Research Group© intec 2005
Nanophotonic waveguidesSilicon on Insulator
Transparent at telecom wavelengths (1.55µm and 1.3µm)
High refractive index contrastin-plane: 3.45(Si) to 1.0 (air)out-of-plane: 3.45 (Si) to 1.45 (SiO2)
Typical dimensions:Thickness: 200 nm Width: 500 nmRequired accuracy: 1-10 nm
Compatible with CMOS processes
Si substrate
silica
Photonics Research Group© intec 2005
SOI-nanophotonic wires
EBeamyes1110.0 600260Oct. 03ColumbiaEBeamyes119.0300300Oct. ‘04NEC
5.0 500200DUVyes115.0 300300Apr. '05LETI / LPMG-lineyes132.0 500200Dec. '01MITEBeamno1105.0 400320Dec. '02Yokohama
EBeamyes37.82.8
300400
300200
Feb. '05NTTEBeamno35.0 470270Aug. '03CornellEBeamno23.6 445220Apr. '04IBMDUVno12.4 500220Apr. '04IMECFab.
top clad
BOX [um]
loss [dB/cm]
w [nm]
h [nm]DateGroup
Photonics Research Group© intec 2005
Waveguide bendsSpirals
Long waveguides (up to 50mm)
Many bends (up to 560)
(b)
Transmission [dB]600
500
400
300
200
100
00 20 40 60
Total length [mm]
# 90
°be
nds
-2
-4
-6
-8
-12
-10
-14
R = 5µm
Exc
ess
bend
loss
[dB
/90°
]
0.08
0.06
0.04
0.02
01 2 3 4 5
0.004dB/900.01dB/90°
0.027dB/90°
0.09dB/90°
Photonics Research Group© intec 2005
Bends
4040
0.150.05
2.05.0
500220LETI/LPM
2 bends1.3resonant 400340Columbia
poly-Si0.3resonant 12 bends0.51.0 500200MIT
31.0 400320Yokohama0.173.0
24 bends0.462.0 300300NTT0.0045.0 0.0272.0
> 500 bends0.091.0 500220IMEC05.0
0.0132.0 20 bends0.0861.0 445220IBMNote
Loss [dB/90]
Radius [um]
w [nm]
h [nm]Group
(Table partly from Vlasov, McNab, Opt. Expr. ’04, pp1630)
Photonics Research Group© intec 2005
Nano ?Feature size: a few 100nmRequired accuracy of features: < 10nmFor wavelength-dependent structures:
Fabrication ?Classical optical lithography too low resolutionE-beam lithography, focused ion beam too slowDeep UV lithography (used for CMOS)
248nm, 193nmFabrication in IMEC CMOS-pilot line 200mm wafers
nm-scale wavelength accuracy : O(1nm) dimensional accuracy !
⎟⎟⎠
⎞⎜⎜⎝
⎛⋅
δλδλ
cladcorennf
dd~
Photonics Research Group© intec 2005
Low cost• Wafer-scale fabrication on large wafers with high yield• Wafer-scale testing• Low cost packaging
Photonics Research Group© intec 2005
Coupling into SOI nanophotonics
Single-mode fiber
1µm
SOI wire
Important:Low loss
Large bandwidth
Coupling tolerance
FabricationLimited extra processingTolerant to fabrication
Polarization
Photonics Research Group© intec 2005
Coupling to fiber – Inverse taper
0.4µm
80nm
0.2µm
200 µm
polished facet
< 2dB3x1.3Polymer175.0175.0 500200IMEC(DUV)3x3
?x?2x2
Cladding Size
0.8Polymer/Si3N460.0200.0 300300NTT (ebeam)
< 4dBSiO2100.040.0 470270Cornell (e-b)< 1dBPolymer75.0150.0 445220IBM (e-beam)
LossCladding Material
tip width [nm]
L [um]w [nm]
h [nm]
Group
Photonics Research Group© intec 2005
Coupling to fiber – Grating couplerAlternative: Grating couplers
Waferscale testing
Waferscale low cost packaging
High alignment tolerance
deep trench
shallow fibre coupler
Towards optical circuit
Single modefiber core
From Fibre
-40
-35
-30
-25
-20
-15
-10
-51500 1520 1540 1560 1580 1600
Tran
smis
sion
[dB
]
Wavelength [nm]
∆λ1dB = 35nm
33% efficiencymeasured
Photonics Research Group© intec 2005
Alignment tolerancesgood alignment tolerances
measurement of P/Pmax versus fiber position
Z
X
Taillaert et al, JQE 38(7), p. 949 (2002)
Photonics Research Group© intec 2005
Coupling to fiber – Grating couplerImproved design
Apodise grating efficiency 63%
Add bottom reflector efficiency over 90%
Photonics Research Group© intec 2005
Theoretical coupling efficiency 78%
Bonded SOI-coupler with gold bottom mirror
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
1500 1520 1540 1560 1580 1600
wavelength
coup
ling
effic
ienc
y
s1_golds2_no_golds1_gold_fits2_no_gold_fit
Si
Au
Measured coupling efficiency:69% (1.5 dB loss)
air
BCB-buffer
SiO2 box layer
Pyrex-substrate
BCB
Grating coupler
waveguide
Photonics Research Group© intec 2005
Polarisation problemProblem: nanophotonic circuits are highly polarisation dependentOur solution:
2D grating
Couples each fiber polarisationin its own waveguide
In the waveguides the polarisation is the same (TE)
Allows for polarisationdiversity approach
Single modefiber core
Taillaert et al. PTL 15(9) p. 1249 (2003)
Photonics Research Group© intec 2005
Polarisation Diversity Circuit
2-D grating
y-polarization
split polarisations
light in
identicalcircuits
x-polarization
x
yz
xy
light out
single-modefiber
2-D grating
combine polarisations
Photonics Research Group© intec 2005
Polarisation Diversity Circuit
2-D grating
y-polarization
split polarisations
light in
identicalcircuits
x-polarization
x
yz
xy
light out
single-modefiber
2-D grating
combine polarisations
Results 2D-coupler:• 20 % efficiency • 1dB bandwidth ~ 35 nm• Extinction ratio > 18dB
Photonics Research Group© intec 2005
Outline
Silicon Photonics: why and how?
Passive wavelength routers in Silicon
Active photonic functions in Silicon
Silicon photonics: what for?
Photonics Research Group© intec 2005
WDM switched optical backplanerouting functionality (w/o switches): passive λ-based routing using tunable lasers
Switching speed determined by tuning speed and by burst-mode receivers
passive
WDM-router
2 single fibers or MT fiber ribbon
Tx/Rx..
.
...
.
.Tx/Rx
Tx/Rx
Tx/Rx
Tx/Rx
Tx/Rx
Photonics Research Group© intec 2005
connectorchip
SOI wavelength router4 x 4 wavelength router
Commercial connector with8 fibers
Vertical fiber couplers
4 x 4 AWG
200 GHz channel spacing
Photonics Research Group© intec 2005
SOI wavelength router
in
reference waveguides
4 x 4 wavelength routerFour input and four output fibers
250 GHz channel spacing
shallow star couplers, 3µm radius bends
3.5dB device insertion loss (waveguides and star coupler), -12 to -14 dB sidelobes
connectorchip
Photonics Research Group© intec 2005
AWG16-channel AWG, 200GHz 200µm x 500µm area
-3dB insertion loss
-15dB to -20dB crosstalk
-40
-35
-30
-25
-20
-15
-10
-5
0
1520 1525 1530 1535 1540 1545 1550 1555 1560 1565 1570
wavelength [nm]
Tran
smis
sion
[dB
]
12345678910111213141516
100µm
Photonics Research Group© intec 2005
Outline
Silicon Photonics: why and how?
Passive wavelength routers in Silicon
Active photonic functions in Silicon
Silicon photonics: what for?
Photonics Research Group© intec 2005
Active photonic functionsThe options for modulation, switching, tuning at high speed:• all Silicon approach
carrier density based optical effects + electric field induced carrier sweep away
All-optical approach using two-photon absorption
• Silicon + III-V-membrane integrationUsing ultra-fast carrier lifetime in III-V
Also allowing light emission, gain, detection
Photonics Research Group© intec 2005
Heterogeneous integrationSilicon waveguide structure
Passive only
Heterogeneous circuit
Active + passive
Silicon substrate
InP thin film
Polymer bonding layer (BCB)
2um
SiliconSilicon
InP
InP
InP
InP
Photonics Research Group© intec 2005
Die-to-wafer bondingMolecular bonding
InP on SOI-waveguides on CMOS demonstrated (LETI, TRACIT)
Polymer bondingPlanarization and bonding in single step (IMEC)
Ultra-thin bonding layers (sub 200nm demonstrated)
InP-layer
Si-wire
Photonics Research Group© intec 2005
Die to wafer bonding technology
Processed SOI substrate
InP/InGaAsPthin film
Good chemical resistance
Photonics Research Group© intec 2005
InGaAs Detectors on SOI
Measured response of 4 detectors
To detectors
Photonics Research Group© intec 2005
InP tunable ring resonators
0.00
0.20
0.40
0.60
0.80
1.00
1.20
1530 1535 1540 1545 1550 1555 1560
Golflengte (nm)
Tra
nsm
issie
(a.u
.)
Photonics Research Group© intec 2005
InP Fabry-Perot lasersGood functionality
Damp-heat testing as proof of reliability of the BCB bonding process
Component 11
0
0.02
0.04
0.06
0.08
0.1
0.12
0 100 200 300 400 500I [mA]
P [m
W]
ref48u100u250u500u
damp heat testing (85°C, 85% RH) for 48, 100, 250 and 500 hours
Photonics Research Group© intec 2005
InP DFB laser diode coupled to SOI
Low k
BCB
SOI/CMOS wafergrat
ing
coup
ler
Photonics Research Group© intec 2005
Outline
Silicon Photonics: why and how?
Passive wavelength routers in Silicon
Active photonic functions in Silicon
Silicon photonics: what for?
Photonics Research Group© intec 2005
Silicon photonics: what for?
• WDM components • switches for high speed backplanes• single chip high speed low power transceivers• on-chip optical interconnect• sensors• labs on a chip
Siliconphotonics
With CMOS
With InP