Techno Forum on
Micro-optics and Nano-optic Technologies
송 석 호, 한양대학교 물리학과 [email protected]
1-(06/23) Introduction: Micro- and nano-optics based on diffraction effect for next generation technologies 2-(06/30) Guided-mode resonance (GMR) effect for filtering devices in LCD display panels
3-(07/07) Surface-plasmons: A basic 3-(07/07) Surface-plasmons: A basic
4-(07/14) Surface-plasmon waveguides for biosensor applications
5-(07/21) Efficient light emission from LED, OLED, and nanolasers by surface-plasmon resonance
Macros Millis Micros Nanos
λ limit
How to reach from Micros toward
How to reach from Micros toward Nanos Nanos? ?
λ limit
Plasmonics: the next chip-scale technology
Plasmonics is an exciting new device technology that has recently emerged.
A tremendous synergy can be attained by integrating plasmonic, electronic, and conventional dielectric photonic devices on the same chipand taking advantage of the strengths of each technology.
Plasmonic devices,
therefore, might interface naturally with similar speed photonic devices and similar size electronic components For these reasons plasmonics and similar size electronic components. For these reasons, plasmonics may well serve as the missing link between the two device
technologies that currently have a difficult time communicating. By increasing the synergy between these technologies, plasmonics may be able to unleash the full potential of nanoscale functionality and become the next wave of chip-scale technology.
1-(06/23) Introduction: Micro- and nano-optics based on diffraction effect for next generation technologies
We have five lectures on:
1-(06/23) Introduction: Micro- and nano-optics based on diffraction effect for next generation technologies 2-(06/30) Guided-mode resonance (GMR) effect for filtering devices in LCD display panels
3-(07/07) Surface-plasmons: A basic
4 (07/14) S f l id f bi li i
4-(07/14) Surface-plasmon waveguides for biosensor applications
5-(07/21) Efficient light emission from LED, OLED, and nanolasers by surface-plasmon resonance
R0 T0
GMR grating
Micros
Dcore
SPP mode metal strip
core cladding
metal slab
core
cladding
Micro & nano-optics based on diffraction effect for next generation technologies
RAY DESIGN WAVE DESIGN PHOTON DESIGN
d > λ d ~ λ d < λ
RAY DESIGN WAVE DESIGN PHOTON DESIGN
Optical Technologies
RAY DESIGN
( )
WAVE DESIGN
( )
PHOTON DESIGN ( d > λ ) ( d ~ λ ) ( d < λ )
Geometrical Optics Ray tracing
Wave Optics Wave propagating
Photon Optics Photon localizing Reflection/Refraction
Etendue Limit:
Α x Ω ~ 1
Diffraction/Interference
Diffraction Limit:
d / λ ~ 1
Resonance/Confinement Confinement Limit:
ΔxΔp ~ 1
W d i f t ti
< An example: LEDs >
Wave design for extraction
(guided modes, surface scattering)
LED
Ray design for projection
(propagation modes, optical aberration)
Photon design for internal QE
(evanescent modes, spontaneous emission)
Optical Technology Roadmap
매출
RAY DESIGN WAVE DESIGN PHOTON DESIGN
(100억) 60
( d >> λ ) ( d ~ λ ) ( d << λ ) Geometrical Optics EM Wave Optics Photon Optics
50
OPU
ISM
LED lighting LASER
Geometrical Optics Ray tracing
EM Wave Optics Wave propagating
Photon Optics Photon localizing
굴절 / 반사
렌즈 설계 (lens design)
회절 / 간섭
회절격자 설계 (grating design)
공명 / 구속
나노구조 설계 (resonator design) 40
LED BLU SOS O-PCB
금형 (metal mastering) 사출 (injection molding) 조립 (assembling)
기판 (wafer mastering) 전사 (UV embossing) 합체 (packaging)
입자 (self assembling) 복제 (nano imprinting) 집적 (integrating)
20
측정 (MTF monitoring) 측정 (extraction efficiency)
( 현재 보유 기술) ( 확보 시급 기술) ( 미래 요구 기술)
측정 (quantum efficiency)
2004 2006 2008 2010 2012 2014
d > λ RAY DESIGN
Far-field diffraction
Far field diffraction
Fraunhofer diffraction
http://www.anteryon.com
Integrated Lens Stacks & Camera Modules g
L A O ti l St t
Large Area Optical Structures
Single Shot Light Field Cameras Single Shot Light Field Cameras
Mask
micrOOptics in nature
??
Extraction of light
d > λ
Single-order DOE Multiple-order DOE
-1.5 -1.0 -0.5 0.0 0.5 1.0 1.5
0.0 0.2 0.4 0.6 0.8
1.0 X0
XDF0R1 XDF30R1 XDF0R0.5
FDTD BPM
http://diffractive.optics.free.fr
DECAD ( Diffractive Element Computer Assisted Design ) is a powerful and versatile software developed by Dr Olivier MAGNIN for diffractive optics design
software developed by Dr. Olivier MAGNIN for diffractive optics design.
DECAD handles all steps of diffractive optics design from optical specifications to e-beam files generation.
Controls Controls
Window IFTA Window
Laser writing system
i i l l i i l l i i l l i i l l CGH
CGH CGH
CGH Digital Hologram Digital Hologram Digital Hologram Digital Hologram DOE Lens
DOE Lens DOE Lens DOE Lens
Waveguide Waveguide Waveguide Waveguide Micro Lens
Micro Lens Micro Lens
Micro Lens Micro prism Micro prism Micro prism Micro prism
Replication onto plastics
Exposure
data Original
t master
• Lens designg
• Waveguide design
• Algorithm
• Interface Laser writing
Maste r plate Replication
plate
• Electro plating
• Evaporating
• Hot embossing
• UV embossing Plastic optics
UV embossing
• molding
d ~ λ WAVE DESIGN
Near-field diffraction Fresnel diffraction
Bragg diffraction
Beam shaping : www.doc.com
Flexible BLU : www.modilis.com
N N E X X T
?
Photon Confinement – Photonic Crystal
Mechanisms of photon confinement Mechanisms of photon confinement
- Total Internal Reflection (TIR) Photonic Band Gap (PBG) - Photonic Band Gap (PBG)
Micro-disk
Micro-pillar
Micro-sphere
Micro pillar
Micro sphere
Photonic crystal slab 3 D h t i t l
<TIR
3>
Photonic crystal slab 3-D photonic crystal
<TIR
2PBG> <TIR PBG
2> <PBG
3>
Photonic Crystal Slab Devices
Point defect : micro-cavity laser, filter
Line defect : low-loss waveguide coupler
Line defect : low-loss waveguide, coupler
Periodic structure : light-emitting diode, band edge laser
Laser cavity Waveguide LED, Laser
(a) (b)
n-GaN
Photon
Sapphire
Exciton generation Radiation p-GaN
Sili b
reflector
InGaN MQW e-h
Silicon submount
Extraction efficiency
Photonic Crystal-LEDs Photonic Crystal LEDs
Baba
Limited by surface recombination
Good scheme!!!
Limited by surface recombination
Good scheme!!!
Lumiled
100 um device size achievable.
Several layer of PC for extraction.
Good internal quantum efficiency N d d ( 90%)
100 um device size achievable.
Several layer of PC for extraction.
Good internal quantum efficiency N d d ( 90%)
Needed (>90%).
Multiple pass limits device size (~10um).
Small volume needed.
Not so good for lighting Needed (>90%).
Multiple pass limits device size (~10um).
Small volume needed.
Not so good for lighting Not so good for lighting.
Surface recombination limited
Surface recombination limited.
Not so good for lighting.
Surface recombination limited
Surface recombination limited.
Noda
Guided-mode resonance (GMR) filters
I n c i d e n t l i g h t
0
0
≥ + 1 ≤ − 1
λ-scale fabrication
λ-scale fabrication
Holographic Lithography
Aperture[variable]
Sample 부착용 Rotation stage (PRM1-z7)
Controller (TDC001)
Linear stages (NRT100) Controller
Mirror Holder[75 x 75]
Controller (BSC103)
Rotation stage (NR360S)
Linear stage (NRT150) Controller
(NR360S) Controller (BSC101) Controller
(BSC103)
NANO
NANO EGGBOX EGGBOX
d < λ PHOTON DESIGN
Evanescent waves
Localized modes
Localized modes
Light transmission through a metallic subwavelength hole
Ag film, hole diameter=250nm, groove periodicity=500nm,
Science, Vol. 297, pp. 820-822, 2 August 2002.
g p y ,
groove depth=60nm, film thickness=300nm
Size Mismatch
between Nano-scale Components and Dielectric Photonics
Photonic integrated system with subwavelength scale components subwavelength scale components
CMOS Tr
Q t d t
Quantum dots
Medium-sized molecule
dielectric waveguide
~ 10 λ
Size Mismatch Æ Metallic waveguides ( ~ 10 nm)
50nm
Plasmons at Planar Metal-Dielectric Interfaces
Harry Atwater, California Institute of Technology
surface plasmons are longitudinal
charge density fluctuations on the
8
ω =c k
charge density fluctuations on the
surface of a conductor Surface Plasmon dispersion relation for Ag in air
(Light line)
λ = 337 nm
ε : dielectric
6
x
λ =337 nm; ε
1
= -1
)
( g )
ε 1 : metal ε 2 : dielectric
4 ω (10
15s
-1)
surface plasmon dispersion relation: λ << 337 nm
1
x
0
ω 2
surface plasmon dispersion relation:
Plasmon Dispersion Relation
λ 337 nm
k = ω ε ε 1 2
0 20 40 60 80 100
0
k
x( μ m
-1)
Pl hi hl l li d t t l di l t i i t f t ti l f
1 2
k
xc ε ε
= +
Plasmons are highly localized at metal-dielectric interfaces, so potential for:
• Ultra small Optical Devices
• “2D-Optics” on metal surfaces
Size Mismatch Æ Metal nanowire ( ~ 10 nm)
Metal (surface plasmon) waveguides
dielectric
Metal t=20 nm dielectric
W=10υm
Metal (surface plasmon) waveguide sensors
D metal strip
ε
d3ε
2D
D SPP mode w
metal strip
ε
d1 coreε
d3metal slab cladding
L f l l it t i d bl l t d t t
Long-range surface plasmon polaritons on asymmetric double-electrode structures Yang Hyun Joo, Seok Ho Song, et. al. / APL 92, 161103 (2008)
350
Sensing arm
Output signal
50 100 150 200 250 300
Intensity (uW) 14.3um
2.28um
Au
SPP waveguide
1.330 1.331 1.332 1.333 1.334 1.335 1.336 0
50
Refractive index of water
Reference arm
Au
Nanocavity lasers
Nanocavity lasers
Nanocavity lasers
Optical Technologies : Macro Î Micro Î Nano
S G WAVE DESIGN PHOTON DESIGN
d > λ d ~ λ d < λ
RAY DESIGN WAVE DESIGN PHOTON DESIGN
Micro lens DOE lens
Flexible BLU
Beam shaping Enhanced lighting Nanocavity laser DOE lens
Hybrid lens BLU
LED lighting
LED lighting
Resonance grating WDM filters
DFB DBR
Nanocavity laser Nanowire waveguide Nano-photonics
Surface plasmonics
Beam shaping DFB, DBR, …
PhC device
Silicon device
Next lecture at 06/30
(06/23) Introduction: Micro- and nano-optics based on diffraction effect for next generation technologies (06/30) Guided-mode resonance (GMR) effect for filtering devices in LCD display panels
(07/07) Surface-plasmons: A basic
(07/14) Surface plasmon waveguides for biosensor applications (07/14) Surface-plasmon waveguides for biosensor applications
(07/21) Efficient light emission from LED, OLED, and nanolasers by surface-plasmon resonance
Possible to use GMR films in LCD panel???
Guided-mode resonance (GMR) filters
Diffuser
Polarized
RED GREEN BLUE RED GREEN BLUE
LCD panel
GMR grating Light
Emission
Reflector Light guide film LED
Unpolarized light beam