thomas f krauss university of st. andrews, supa, school of ... · “room-temperature emission at...
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TF Krauss, Pavia March 2012 No.1/60
Thomas F Krauss
University of St. Andrews, SUPA, School of Physics and Astronomy, St Andrews, UK
Integrated Nanophotonics: Issues and opportunities
Key collaborators: Pavia & Catania, Italy
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TF Krauss, Pavia March 2012 No.2/60
St Andrews
Scotland’s First University
Thomas F Krauss
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TF Krauss, Pavia March 2012 No.3/60
! Scotland, UK ! 18,000 people (1/3 students) ! 80km from Edinburgh ! 600 km from London
Glasgow Edinburgh
St Andrews Dundee
Aberdeen
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TF Krauss, Pavia March 2012 No.4/60
St Andrews. The home of golf
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TF Krauss, Pavia March 2012 No.5/60
LEO 1530 SEM/ Raith Elphy Plus!
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TF Krauss, Pavia March 2012 No.6/60 CAIBE machine!
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TF Krauss, Pavia March 2012 No.7/60
Photonic crystal waveguides
220 nm Si waveguide, airbridge or oxide clad epixnet nanostructuring platform: www.nanophotonics.eu
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Silicon Photonics
What’s the problem silicon photonics is trying to solve ?
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55 W-hour battery stores the energy of
1/2 a stick of dynamite.
If battery short-circuits, catastrophe is possible ...
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fJ fJ pJ
Optical interconnects save energy
fJ fJ fJ ?
Optical Interconnect
Electrical Interconnect
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On-chip Optical Interconnects
Use the photonics layer to shift data in a multicore architecture
Peter Kogge, DARPA study on Exascale Computing
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Peter Kogge, DARPA study on Exascale Computing
Possible monolithic realisation
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TF Krauss, Pavia March 2012 No.14/60
Optical interconnects
INTEL IBM
The idea is to use optical signals to distribute information on-chip, between processors.
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fJ fJ pJ
fJ fJ fJ
Optical interconnects save energy
Optical Interconnect
Electrical Interconnect
External lightsource + modulator
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External Lightsource + Modulator
!"
Requirements: Fast (ideally ps) => Carrier modulation =>Typical #n!10-4
=>Typical length ! cm
!" = !
k0!nL = ! # L = "2!n
$ 104"
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Intel
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Solution: Resonant enhancement. Effective optical path maintained. Electrical path reduced.
++ +
+
+ - - - - -
Volume of active carriers reduced.
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Solution: Resonant enhancement. Effective optical path maintained. Electrical path reduced.
++
- -
Volume of active carriers reduced
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Kotura ring: 30"m dia. = 100"m circumf. 50 fJ/bit 10 GHz bandwidth Tuning energy: > 100 fJ/bit Tolerances ?
OpEx 17, 22484 (2009)
State-of-the-Art
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TF Krauss, Pavia March 2012 No.21/60
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TF Krauss, Pavia March 2012 No.22/60
fJ fJ pJ
fJ fJ fJ
Optical interconnects save energy
Optical
Electrical
+ #$"
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TF Krauss, Pavia March 2012 No.23/60
Photonic crystal waveguides
220 nm Si waveguide, airbridge or oxide clad
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Slow Light Mechanism!
a!
In the slow light regime, one can imagine the mode taking a longer route - that’s why it takes more time, and why there is more light inside the structure.!
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PhC MZI modulator
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Thermally activated Mach-Zehnder
80 "m long PhC
L. O'Faolain et al., IEEE Photonics Journal 2, 404 (2010)
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Dispersion curve
Switching performance
PhC – MZI Performance
L. O'Faolain et al., IEEE Photonics Journal 2, 404 (2010)
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n i p
Electrical operation. Work in progress…..
Electrical operation
William Whelan-Curtin Kapil Debnath
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Conclusion modulator
The slow light concept allows us to make small footprint, low driving power modulators with high bandwidth. They are of similar size, and therefore capacitance, as State-of-the-Art microring resonators, but offer far more bandwidth and do not need to be tuned.
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fJ fJ pJ
fJ fJ fJ
2. Solution: Internal lightsource
Optical Interconnect
Electrical Interconnect
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TF Krauss, Pavia March 2012 No.31/60
Defect luminescence
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PL from SOITEC wafer
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PL from SOITEC wafer + PhC Cavity
“Room-temperature emission at telecom wavelengths from silicon photonic crystal nanocavities”, R. Lo Savio et al., Appl. Phys. Lett. 2011
300x
300x enhancement !! Why 300x ? a) Purcell effect b) Extraction
efficiency
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Nature News & Views, 1997
FP =3!3
4" 2QV
!rad =" nonrad
" radFP
+" nonrad
E. M. Purcell, Phys. Rev. 69, 37 (1946).
Purcell effect
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TF Krauss, Pavia March 2012 No.35/60
Ti! f =2!h
f |H ' | i2"
Fermi’s Golden Rule
Matrix element Density of states
The Purcell factor relates to Fermi’s Golden Rule The transition between two quantum mechanical states is given by the product of the matrix element (derived from the Hamiltonian) and the density of final states. This transition probability is also called decay probability and is related to mean lifetime.
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%,!"FP =
3!3
4" 2QV
Ti! f =2!h
f |H ' | i2"
%,!"
i
f
To enhance the interaction between a cavity and an emitter, they need to agree in emission wavelength and be in the same space -> Q/V
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Fp =!
"cavity
"membrane
!cavity = 0.9
!membrane = 0.036
! = 300
Fp =12, !ext = 25
Extraction efficiency
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The Purcell-factor makes defect emission “Room-temperatureable”
!rad =" nonrad
" radFP
+" nonrad
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TF Krauss, Pavia March 2012 No.39/60
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TF Krauss, Pavia March 2012 No.40/60
Using hydrogen treatment and well-designed designed photonic crystal cavities, we can achieve significant light emission directly from silicon. This is not yet sufficient for optical interconnects, but further improvements are possible. The output power is competitive with comparable III-V devices,. although not with III-V materials as such.
Conclusion light sources
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2. Silicon Nanophotonics for Biosensors
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The Lab on a chip (LoC) concept aims to realise biochemical analysis/synthesis in a miniaturised format.
Lab on a chip (LoC)
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TF Krauss, Pavia March 2012 No.43/60
Surface Plasmon sensor!
Very high sensitivity -> Biacore Broad resonance
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TF Krauss, Pavia March 2012 No.44/60
Silicon ring resonator as biodetector!
K. deVos, R. Baets et al., OPTICS EXPRESS 15, pp. 7610-7615 (2007).!
Lower sensitivity Narrow resonance -> Genalyte
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#$"%&"
High sensitivity Narrow resonance -> ???
Di Falco, Krauss et al., APL 2009
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Genalyte
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TF Krauss, Pavia March 2012 No.47/60
Light source Spectrum Analyser
Chip in a lab
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TF Krauss, Pavia March 2012 No.48/60
The possible integration of silicon light sources would lead to miniaturisation, large scale integration and simplicity.
Source
Transducer
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TF Krauss, Pavia March 2012 No.49/60
Light source Spectrum Analyser
Lab on a chip
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TF Krauss, Pavia March 2012 No.50/60
Autonomous sensors
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2nd problem: Diffusion time
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TF Krauss, Pavia March 2012 No.52/60
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TF Krauss, Pavia March 2012 No.53/60
H Schmidt & AR Hawkins, Nature Photonics August 2011
Optofluidic laser
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H Schmidt & AR Hawkins, Microfluidics & Nanofluidics (2008)
Fluorescence correlation spectroscopy (FCS), FRET,… Measure changes caused by molecular binding, not using the surface.
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TF Krauss, Pavia March 2012 No.55/60
As it does not have volume, only surface, its entire structure is exposed to its environment and responds to any molecule that touches it. This makes it a good material for super-sensors capable of detecting single molecules of toxic gases.
Graphene
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TF Krauss, Pavia March 2012 No.56/60
Key issues Biology 1. Lab on a chip – chip on a lab: Integration.
2. Move away from surface affinity biosensor. Novel integrated sensor architectures.