R e a l i z a t i o n o f P l a s m o n i c D e v i c e s
Kristján Leósson/Science Institute/University of Iceland ADVANCES ON NANOPHOTONICS IV – Erice Sicily 2012
BIO
1994 B.Sc. Engineering Physics, Canada
1996 M.Sc. Physics, Iceland/France/Germany 2002 Ph.D. Electrical Engineering, Denmark
2001 Co-founded MMP A/S
2004 Co-founded Lumiscence A/S 2005- Senior Research Scientist
University of Iceland
1990 1995 2000 2005 2010 0
1000 2000 3000 4000 5000
ISI Web of Knowledge Topic: Surface plasmon*
Annual # of publications
Year
1990 1995 2000 2005 2010 0
2 4 6 8 10 12 14 16
Surface plasmon papers
% o f p u b lic a tio n s
Year
1990 1995 2000 2005 2010 0
2 4 6 8 10 12 14 16
Surface plasmon papers Papers by Smith
% o f p u b lic a tio n s
Year
1990 1995 2000 2005 2010 0
2 4 6 8 10 12 14 16
Surface plasmon papers Papers by Smith
Papers by Yang
% o f p u b lic a tio n s
Year
1990 1995 2000 2005 2010 0
2 4 6 8 10 12 14 16
Surface plasmon papers Papers by Smith
Papers by Yang Graphene papers
% of publications
Year
http://www.youtube.com/watch?v=9tkDK2mZlOo
1. Brief plasmonics background 2. SPP waveguide devices
3. Biophotonics 4. Prospects
o u t l i n e
o u t l i n e 1. Brief plasmonics background
2. SPP waveguide devices 3. Biophotonics
4. Prospects
Re(εr2)<0 Im(εr2)>0 Re(εr1)>0
s u r f a c e p l a s m o n p o l a r i t o n s
D r u d e m o d e l
g o l d
Maier
d i s p e r s i o n , D r u d e v s . g o l d
520 nm
Maier
d i s p e r s i o n , s i l v e r
Maier
f i e l d c o n f i n e m e n t
520 nm
d i f f r a c t i o n l i m i t
f i e l d c o n f i n e m e n t ( S i / S i O
2)
Biberman et al.
OPTICS EXPRESS 18, 15544 (2010)
λ0=1550 nm
m o r e c o m p l e x g e o m e t r i e s
Maier
Slots Ridges V-grooves Wedges
Particle chains DLSPPWGs
LRDLSPPWGs
Other hybrids
...etc.
Optical Loss
Mode Size
o v e r a l l p i c t u r e
o u t l i n e 1. Brief plasmonics background
2. SPP waveguide devices 3. Biophotonics
4. Prospects
θ = θsp Au
BiaCore
S P R d e v i c e
m e t a l r i d g e w a v e g u i d e s
Weeber, Lacroute, Dereux, Optical near-field distributions of surface plasmon waveguide modes, PRB 68, 115401 (2003)
S P P B G w a v e g u i d e s
Bozhevolnyi, Erland, Leosson, Skovgaard, Hvam Waveguiding in surface plasmon polariton band bap structures, PRL 86, 3008 (2001)
Bozhevolnyi, Volkov, Leosson: Localization and waveguiding of surface plasmon polaritons in random nanostructures, PRL 89, 186801 (2002)
S P P B G w a v e g u i d e s
300 250 200 00 150 100 50 00
Image size: 3232m2, wavelength 737 nm
min max
300 250 200 00 150 100 50 00
Image size: 3232m2, wavelength 737 nm
min max
Image size: 3221m2, wavelength 737 nm A
B
Image size: 3221m2, wavelength 737 nm A
B
S P P B G c o m p o n e n t s SPPBG circuits
- High propagation loss >1dB/component - Coupling issues
- Single-polarization
L R - S P P B G c o m p o n e n t s LR-SPPBG circuits
+ Lower propagation loss + End-fire coupling
- Single-polarization
t h i n m e t a l f i l m s
1 2 3
d
T h i n m e t a l f i l m s
1 2 1
l o n g / s h o r t - r a n g e S P P s
Gold film thickness (nm)
L R - S P P s Substrate
Dielectric d
Comprehensive review:
Berini, Long Range Surface Plasmon Polaritons, Advances in Optics and Photonics 1, 484 (2009).
J. J. Burke, et. al., Phys. Rev. B 33, 5186 (1986) R. Charbonneau, et. al., Optics Letters 25, 844 (2000) T. Nikolajsen, et.al. Appl. Phys. Lett. 82, 668 (2003) P.G. Hermannsson, et al., Proc. SPIE 6988-0A (2008)
-15 -10 -5 0 5 10 15
0,0 0,2 0,4 0,6 0,8
1,0 t = 10 nm t = 20 nm t = 40 nm
Intensity (arb. untis)
Vertical coordinate (µm)
To SMF28
Boltasseva, et al. Propagation of long-range surface plasmon polaritons in photonic band gap structures, JOSA B 22, 2027 (2005)
Boltasseva, et al. Compact Bragg gratings for long-range surface plasmon polaritons, JLT 24, 912 (2006)
Boltasseva, et al. Compact Z-add-drop wavelength filters for long-range surface plasmon polaritons, Opt. Express 13, 4237 (2005)
Boltasseva, et al. Integrated Optical
Components Utilizing Long-Range Surface Plasmon Polaritons, JLT 23, 413 (2005)
Boltasseva, et al. Integrated Optical
Components Utilizing Long-Range Surface Plasmon Polaritons, JLT 23, 413 (2005)
Nikolajsen, et al: In-line extinction modulator based on long-range surface plasmon polaritons Optics Communications 244, 455 (2005)
0 1 2 3 4 5 6
-30 -25 -20 -15 -10 -5 0
Relative transmission (dB)
Voltage (V) Attenuation: 0-30 dB (continuous)
Drive power @ 30 dB: 50 mW Response time: 0.5 ms
Insertion loss: 1.5 dB Footprint: 1.5 x 1 mm2
Bozhevolnyi, Nikolajsen, Leosson: Integrated power monitor for long-range surface plasmon polaritons, Optics Communications 255, 51 (2005)
0 1 2 3 4 5
3.5 3.6 3.7 3.8 3.9 4.0 4.1
4.2 Bias voltage 2V
Responsivity 150mV/W
@1550nm
Monitor output [mV]
Optical input power [mW]
VOA MON
VVOA GND + VMON -
GND VBIAS
VOA Chip Schematic
w h y L R S P P w a v e g u i d e s ?
LRSPP waveguides are compatible with standard fiber-optics
Efficient thermo-optic devices; heat delivered directly to waveguide core
Properties of two closely spaced waveguides can be controlled independently Only one dielectric material is needed, no refractive index engineering
Simple fabrication, accurate patterning, low-temperature processing
L R S P P d e v i c e s
Already demonstrated:
Waveguides, bends, splitters
Directional couplers (passive/active)
Multimode interferometers (passive/active) Mach-Zehnder interferometers
Bragg gratings (passive/tunable) Wavelength add-drop filters
In-line power monitors
In-line extinction modulators
BUT ... all have high insertion loss (several dB) and 100% PDL
p o l a r i z a t i o n d e p e n d e n c e
Jung, Søndergaard, Bozhevolnyi PRB 76, 035434 (2007)
n a n o w i r e w a v e g u i d e s
P. Berini, US Patent 6,741,782 (2004)
K. Leosson, et al., Opt. Express 14, 314 (2006)
n a n o w i r e V O A
K. Leosson, T. Rosenzveig, A. Boltasseva Optics Express 16, 15546 (2008)
>30 dB extinction ratio
PDL < ± 2.5 dB across attenuation range Off-state insertion loss 5-15 dB
Very strict fabrication tolerance (<5nm)
n a n o w i r e o p t i m i z a t i o n
Rosenzveig, Hermansson, Leosson,
Modelling of Polarization-Dependent Loss in Plasmonic Nanowire Waveguides, Plasmonics 5, 75 (2010)
t r a n s i e n t r e s p o n s e
FE simulation Experiment
Dielectric Dielectric
Gain material Metal layer
MDMO-PPV
l o s s c o m p e n s a t i o n
Gather, Meerholz, Danz, Leosson,
Net optical gain in a plasmonic waveguide embedded in a fluorescent polymer,
Nature Photonics, 4, 457 (2010)
Dielectric Dielectric
Gain material Metal layer
l o s s c o m p e n s a t i o n
Non-matched
Index-matched No gain
layer
Theory
ground state
E
excited state
I
Energy
• Localization of exciton allows for strong coupling with phonons
• Vibronic relaxation <1ps
=> all emission from lowest vibronic state
• Excited state conformation is distorted =>
probability of transitions changes (Franck- Condon Principle)
spatial coordinate
1-10 ns
00 01
02
ground state
E
I
Energy
Example:
• Pump 01
• Vibronic relaxation 10
• Radiative relaxation 01
• Ground state relaxation 10
spatial coordinate
excited state
pump lasing
1-10 ns
• Is the optical energy excited in the conjugated polymer layer transferred to an LRSPP mode?
• Where should the gain material be located?
Ormoclear
Ormoclear
Gain material Metal layer
Excited Dipole
S i m u l a t i o n
Measured net gain of g = 8 ± 2 cm
-1(12.5 mJ/cm
2/pulse, 4-5 nm gold film) Room temperature, 600nm wavelength
) 1
(
Pe
glg
I AE
L R S P P g a i n
For highly confined SPPs, losses are generally too high to allow for full loss compensation with currently available gain materials and reasonable pump power
see K.Leosson, Optical amplification of surface plasmon
polaritons: a review, J. Nanophotonics (in press)
1. Brief plasmonics background 2. SPP waveguide devices
3. Biophotonics 4. Prospects
o u t l i n e
Light is coupled from an optical fiber to an embedded waveguide
Light is distributed to the sensing areas
Light couples to the surface plasmon waveguide
Fluorescence emission is collected
50-300nm high index contrast polymer waveguides
n=1.34
n1 n2
θ > θc
Nikon
© Nikon
T I R F m i c r o s c o p e
d i e l e c t r i c - p l a s m o n c o u p l i n g
Water
Gold Cytop
Cytop PMMA
0 500 1000 1500
1.36 1.38 1.40
1.42 =633 nm
Effective refractive index
Spacer layer thickness (nm)
5-layer structure (cf. directional coupler)
Fluorescent beads in solution
Penetration depth into liquid approximately 1.5µm
x20 NA 0.4 0.5mm
Scattered light
FDTD
d i e l e c t r i c - p l a s m o n c o u p l i n g
Metal, Au Dielectric, n = 1.55
Dielectric, n = 1.55
800 nm
25 nm d
Symmetric / long-range
Anti-symmetric / short-range
E
= 610nm
S P P m o d e s , t h i n f i l m
Im(n) = 10
-4 a = 10 cm
-1 L = 1 mm
f a b r i c a t i o n
CCD EM-CCD
Sía
e x p e r i m e n t a l s e t - u p
z
|E|
2(a) (b) (c) (d)
n=1.33
n=1.34
100 µm
c o l l o i d a l g o l d s o l u t i o n
b u r i e d c h a n n e l w a v e g u i d e s
b e n d l o s s
f i l t e r s
Q≈1000
10 µm
Blood diagnostics platform (Lumiscence/IMI Inc.)
x z
y
p-polarized (TM) s-polarized (TE)
yz plane xz plane
1. Brief plasmonics background 2. SPP waveguide devices
3. Biophotonics 4. Prospects
o u t l i n e
S P R d e v i c e
BiaCore
p l a s m o n - a s s i s t e d m a g n e t i c r e c o r d i n g
Mike Seigler Seagate
S E R S , p a r t i c l e g r o w t h
Virginia Joseph: Nanopartikel auf Oberflächen – Charakterisierung und Anwendung in der
oberflächenverstärkten Raman-Streuung, PhD Thesis, Humboldt Universität Berlin (2012)
S h e e t r e s i s t a n c e
S P P q u a n t u m o p t i c s
EOS2012
Benisty, H., et al., Implementation of PT symmetric devices using plasmonics: principle and applications.
Optics Express, 2011. 19(19): p. 18004-18019.
a p p l i c a t i o n s o f S P P w a v e g u i d e s
Babicheva, V.E., et al., Plasmonic modulator based on gain-assisted metal-semiconductor-metal waveguide.
arXiv:1203.3374v1, 2012.
a p p l i c a t i o n s o f S P P w a v e g u i d e s
Ranjbaran, M. and X. Li, Optimized Dipole-Surface Plasmon Waveguide Coupling for Enhancement of SLD Performance.
IEEE Photonics Journal, 2010. 2(5): p. 848 - 857
a p p l i c a t i o n s o f S P P w a v e g u i d e s