generalized snell’s laws - rqc.ru · optical camouflage: projecting background image onto masked...

60
And The Exciting Science of Light with Metamaterials Vladimir M. Shalaev Birck Nanotechnology Center

Upload: lekiet

Post on 22-Jul-2018

218 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

And

The Exciting Science of Light with Metamaterials

Vladimir M. Shalaev

Birck Nanotechnology Center

Page 2: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Outline

• Intro to metamaterials

• Nanophotonics enabled by Plasmonics and Metamaterials

• Toward Better Materials for MM and TO applications

• Negative-index metamaterials

• Transformation optics and cloaking

• Engineering PDOS & Sub-wavelength light confinement with Hyperbolic MMs

• Flat photonics with Metasurfaces: Generalized Snell’s Law, negative refraction, meta-lens, meta-hologram….

Page 3: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

3

Natural Optical Materials

S

S

k

E

H

k

E

H

Negative Index

Materials

Common

Transparent

Dielectrics

Electrical Plasma(Metals at optical

wavelengths)

Magnetic Plasma(Not naturally occurring at

optical wavelengths)

Evanescent waves

Evanescent waves

k

k

1

1

Semiconductors

Crystals

Water

metals

Air E,H ~exp[in(ω/c)z] n = ±√(εμ)

Page 4: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

4

What is a metamaterial?

+-

-

Metamaterial is an arrangement of artificial structural elements, designed to achieve

advantageous and unusual electromagnetic properties.

ta = meta = beyond (Greek)

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

+-

-+

-

-+

-

-+

-

-+

-

-+

-

-

A natural material with its atoms A metamaterial with artificially structured

“atoms”

Page 5: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

5

Photonic crystals vs. Optical metamaterials: connections and differences

0 1 aa<<.

Effective medium

description using

Maxwell equations with

, , n, Z

a~

Structure dominates.

Properties determined

by diffraction and

interference

a>>

Properties described

using geometrical optics

and ray tracing

Example:

Optical crystals

Metamaterials

Example:

Photonics crystals

Phased array radar

X-ray diffraction optics

Example:

Lens system

Shadows

Page 6: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

6

Photonic crystals

... have lattice constants comparable to light

wavelengths: a ~

… can be artificial or natural

… have properties governed by the diffraction of

the periodic structures

… may exhibit a bandgap for photons

… typically are not well described using effective

parameters , , n, Z

… often behave like but they are not true

metamaterials

Page 7: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Electrical Metamaterials (Plasmonics): Route to Nanophotonics

Page 8: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Why Plasmonics/Electric MMs?

M. Brongersma, V. Shalaev, Science (2010)

Plasmonics will enable an improved synergy between electronic and photonic devices ̶ Plasmonics naturally interfaces with similar size electronic components ̶ Plasmonics naturally interfaces with similar operating speed photonic networks

Critical dimension active devices (nm)

Op

erat

ing

spee

d THz

GHz

MHz

kHz

10nm 100nm 1m 10m 1mm 100m

Semiconductor Electronics

Metallic Nanoplasmonics

Dielectric Photonics

The past

PHz

Page 9: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Silicon Integrated Nanophotonics

Page 10: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

IBM Silicon Integrated NP Technology

IBM chip: BLUE optical waveguides and YELLOW copper wires

IBM 90nm Silicon Integrated Nanophotonics: Integrated photodetector (red feature) Modulator (blue feature) Silicon transistors (red sparks)

“After More Than a Decade of Research, Silicon Nanophotonics is Ready for Development of Commercial Applications.”

IBM Press release, December 10, 2012

Page 11: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

ELECTRONIC-PHOTONIC INTEGRATION:

SUMMARY

Photonic circuit + High speed + High bandwidth - Component size is limited (>~ 100nm - 1 µm)

Modern communication systems Huge amount of data Ever increasing speed

Electronic circuit + Very compact (~ 10nm) - Operational speed is limited (RC-delay)

Electronic + Photonic circuit: NEED FOR NEW TECHNOLOGIES

Si NANOPHONICS (near-term)+ PLASMONICS/METAMATERIALS (~5 years)

Optical mode in waveguide > 0/2nCORE

Diffraction limit

www.mayang.com/textures/

Page 12: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

[ Bow-tie antennas ]

Other Applications: Sensors

from LC-contour to nanophotonic circuits (Engheta – ‘metatronics’)

OE (2009); NJP (2008); Metamaterials (2008); APL (2008)

OPTICAL NANOANTENNAE

Page 13: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Optical Nanolaser Enabled by SPASER

Related prior theory: Stockman (SPASER)

Zhang group: Plasmon Laser (Nature,2009) Room-T Plasmon Laser (Nat. Mat, 2010) “Spasing Laser” – Zheludev, Stockman M. T. Hill, et al; C. Z. Ning, et al (electr. pump) Spotlight on Plasmon Lasers (Perspective, Science, 2011)- X. Zhang, et al

Optical MOSFET (Stockman)

Noginov, Shalaev, Wiesner groups, Nature (2009)

Page 14: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Toward Better Materials for Plasmonic and MM Applications

(Boltasseva group, Purdue)

Page 15: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

METALS TO LESS-METALS:

Doped semiconductors + Intermetallics (nitrides, borides, silicides, …)

New Plasmonic Materials

A. Boltasseva and H.A. Atwater, Science 331 (2011)

Page 16: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Alternative Plasmonic Materials

P. West, et al, Lasers & Photon. Rev. (2010) (Boltasseva group)

(see also work by the Noginov group)

Transparent Conductive Oxides

ε΄ becomes negative below 2μm

Page 17: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Metallic: Golden luster

Titanium Nitride

G.V. Naik et al., Optical Materials Express 2 p. 478 (2012)

http://www.mini-lathe.com/Feat_Mach/Turbocam

OSA press release March 27, 2012

‘Researchers Discover a New Path for Light Through Metal: Novel Plasmonic Material May Merge Photonic and Electronic Technologies’

Hard & tough: high speed drill-bits

Well-established processing

Page 18: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

New Plasmonic Materials for HMMs

Performance of HMM devices: (A. Hoffman, Nature Materials 6(2007) 946–950)

FOM=Re{k}/Im{k}

Phys. Status Solidi RRL 4, 295 (2010) G..V. Naik and A. Boltasseva, Metamaterials 5(2011) 1-7

Page 19: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Negative Refraction in all-Semiconductor based HMM

G. Naik, et al, PNAS (2012)

Page 20: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Negative refraction in semiconductor-based metamaterials

• Semiconductors exhibit metallic

properties when heavily doped

• Aluminum doped zinc oxide (AZO)

exhibits metallic property in the

near-infrared

• Conventional metals replaced by

semiconductor-based ones such as

AZO can produce high

performance metamaterials

• The figure-of-merit of AZO/ZnO

metamaterial is 11: three orders

higher than metal-based designs

G. Naik, et al. PNAS (2012) (Boltasseva /Shalaev groups)

Page 21: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

21

Page 22: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Sir Arthur Schuster Sir Horace Lamb

L. I. Mandel’stam

V. G. Veselago

Sir John Pendry

… energy can be carried forward at the group velocity

but in a direction that is anti-parallel to the phase

velocity…

Schuster, 1904

Negative refraction and backward propagation of

waves

Mandel’stam, 1945

Left-handed materials: the electrodynamics of substances

with simultaneously negative values of and

Veselago, 1968

Pendry, the one who whipped up the recent boom

of NIM researches

Perfect lens (2000)

EM cloaking (2006) Others: Sivukhin. Agranovich,…

22

Page 23: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

if ,0n

• Refraction:

• Figure of merit: θ1

θ2

θ1 θ2

"/|'| nnF

εμn

εμn

2

0 ||' ||'

23

Page 24: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

E

H

k

Dielectric

Metal

Nanostrip pair (TM)

< 0 (resonant)

Nanostrip pair (TE)

< 0 (non-resonant)

Fishnet

and < 0

S. Zhang, et al., PRL (2005)

24

Page 25: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

O. Hess, Nature 455, 299 (2008)

Negative Refraction Effects

Page 26: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

http://io9.com/5036183/secrets-of-the-metamaterials-that-will-make-you-invisible

Negative Refraction Effects

Page 27: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

V. M. Shalaev, Transforming Light, Science, Oct. 17, 2008

27

Page 28: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Spatial profile of & tensors determines the distortion of coordinates

Seeking for profile of & to make light avoid particular region in space — optical cloaking

Fermat:

δ∫ndl = 0

n = √ε(r)μ(r)

“curving”

optical space

Distorted field line in distorted coordinate

Straight field line in Cartesian coordinate

Pendry et al., Science, 2006

Leonhard, Science, 2006

Greenleaf et al (2003)

L. S. Dolin, Izv. VUZ, 19614

28

Page 29: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Form-invariance of Maxwell’s equations

Coordinate transformation from x to coordinate x is described using the

Jacobian matrix G: ij i jg x x

( )

( ) 0

E

H

HEt

EH Jt

Maxwell’s equation in x

1 1

;

( ) ; ( )

;

T T

T T

G G G G

G G

E G E H G H

GJJ

G G

Transformation of variables

Ward and Pendry, J. Mod.Opt. 43, 777 (1996)

Page 30: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Pendry et al., 2006

The bending of light due to the gradient in refractive index in a desert mirage

Page 31: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

31

Kildishev, VMS (OL, 2008); Shalaev, Science 322, 384 (2008)

Optical Black Hole (Zhang group; Narimanov,Kildishev)

(b)

Fermat: δ∫ndl = 0 n = √ε(r)μ(r)

curving optical space

Planar hyperlens (Kildishev and VMS) (Schurig et al; Zhang group)

Light concentrator (also, Schurig et al)

Page 32: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Narimanov, Kildishev

32

Page 33: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Invisibility in Nature, Physics and Technology

• Natural camouflage

• Black hole

• …

Current technologies to achieve invisibility:

Stealth technique: Radar cross-section reductions by absorbing paint / non-metallic frame / shape effect…

F-117 “Nighthawk” Stealth Fighter

Optical camouflage: Projecting background image onto masked object.

Optical Camouflage, Tachi Lab, U. of Tokyo, Japan

Page 34: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

The Invisible Man by H. G. Wells (1897)

“The invisible woman” in The Fantastic 4 by Lee & Kirby (1961)

Examples with scientific elements:

"... it was an idea ... to lower the refractive

index of a substance, solid or liquid, to

that of air — so far as all practical

purposes are concerned.” -- Chapter 19

"Certain First Principles"

"... she achieves these feats by bending all

wavelengths of light in the vicinity around

herself ... without causing any visible

distortion.” -- Introduction from Wikipedia

Pendry et al.; Leonhard, Science, 2006 (Earlier work: cloak of thermal conductivity by Greenleaf et al., 2003)

34

Page 35: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Nature Photonics (to be published)

Optical Cloaking with Metamaterials: Can Objects be Invisible in the Visible?

Cover article of Nature Photonics (April, 2007)

Page 36: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

metal needles embedded in dielectric host

Unit cell:

Flexible control of r ;

Negligible perturbation in

Cai, et al., Nature Photonics, 1, 224 (2007)

Page 37: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Cloaking performance: Field mapping movies

Example: cloak @ 632.8nm with silver wires in silica

Cloak ON Cloak OFF

Page 38: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

J. Li and J. B. Pendry , Phys. Rev. Lett., 2008

picture from discovery.com

Page 39: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Progress Towards True Invisibility on May.17, 2009, under Science www.codingfuture.com

Theory: J. Li, J. Pendry

GHz: Smith et al (Duke)

Optical: Zhang et al (Berkeley)

Lipson et al (Cornel)

39

Page 40: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Signal

Signal

Signal

Signal

Control C

Wave guide

Wave guide

Wave guide

Wave guide

(a)

(b)

(c)

(d)

Control C

Control C

Control C

Control A

Control A

Control A

Control A

Turn on Control A

Turn of fControl C

A B C

A B C

A B C

A B C

M. W. McCall and et al., Journal of Optics, 2011 Gaeta eta al, experiment

Star Trek transporter

Page 41: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Modern cosmology describes Universe as collection of spaces connected by black holes and wormholes. These spaces may have different topology and different number of dimensions.

Using transformation optics we can create “optical spaces” having non-trivial topology, which cannot normally fit into Euclidean 3D space:

Even metric signature of the “optical space” may differ from the (+ - - - ) signature of the Minkowski space. In hyperbolic materials (Smolyaninov, Narimanov – PRL, 2010):

2

2

2

2

2

2

1

2

22

2 1

yxztc

01 02

02

4

2

2

3

2

2

2

2

2

1

2

xxxx Flashes of light are observed during metric signature transitions : toy Big Bang physics

2T K-G

41

Page 42: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Hyperbolic Metamaterials: Engineering Photonic Density of States

& Subwavelength Light Confinement

S. Ishii, et al, Laser Photonics Rev., 1–7 (2013)

DOI 10.1002/lpor.201200095

Page 43: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Cover article

Page 44: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Hyperbolic Metamaterials (HMMs)

A metamaterial has hyperbolic dispersion relation

22 2 2x y z

k k k

c

hyperbolic dispersion

Jacob, et al., Opt. Express, 2006

22 2 2x y z

k k k

c

x

y

z

22 2 2

x y zk k k

c

normal dispersion

Transverse Negative (TN) Transverse Positive (TP)

x

y z

Page 45: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

PHOTONIC DENSITY OF STATES (PDOS)

Iso-frequency surface at ω

Iso-frequency surface at ω+δω

Page 46: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

QED IN THE ’HYPERSPACE’

• Rate of SE, can be understood as property of atom-environment system

• Environment (cavity, PhC, nanowire) enhances density of states

(Dipole matrix element)2

Environment strongly alters the rate of SE through the available PDOS!

Fermi’s Golden Rule:

Available density of states for emitted light

Coupling of emitter to field (depends on the mode volume)

Page 47: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

: Ford and Weber (1984)

QED: Hughes group (2009)

Calculation Methods:

EMISSION POWER SPECTRUM

Page 48: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Diffraction from double slits

– FWHM = 45 nm at = 465 nm

Diffraction inside Hyperbolic Media

• Hyperbolic metamaterial (HMM) – Ag/SiO2 lamellar HMM

– High-k waves are supported

– Propagation of high-k waves is confined

eff

x

eff

z

2.78 0.22

6.31 0.15

i

i

S

=465 nm

=465 nm

(15 nm Ag/15 nm SiO2)3

S. Thongrattanasiri and V. A. Podolskiy, Opt. Lett. (2009) Satoshi Ishii et al, in preparation

Page 49: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Subwavelength Interference (Experiment)

Ag/SiO2 HMM sample SiO2 sample

• For Ag/SiO2 HMM sample: FWHM = 83 nm (< ) • For SiO2 sample: FWHM = 542 nm (~ )

1. Sample fabrication

Deposition and FIB

2. Photolithography

Photoresist exposure, develop

3. AFM scan

=465 nm

Page 50: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Flat Photonics with Metasurfaces: Generalized Snell’s Law,

Negative Refraction, and much more....

Birck Nanotechnology Center

Page 51: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Principle of Least Action

Maupertuis felt that “Nature is thrifty in all its actions”, and applied the principle broadly

Pierre Louis Maupertuis (1698-1759)

Leonhard Euler (1707-1783)

Louis de Broglie (1892-1987)

Page 52: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Principle of least action → The momenta difference between blue and red path is zero

Generalized Snell’s Law (Capasso Group)

For refraction

For reflection

see also S. Larouche and D.R. Smith, OL v. 37, 2391 (2012)

A

B

ni

Ф Ф+dФdr

θt

θr

nt

In essence, momentum conservation!

Page 53: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Generalized Snell’s Law

N. Yu, et al. Science, 2011 (Capasso Group)

Demonstrated at 8 µm wavelength

Page 54: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Broadband light bending with plasmonic nanoantennas

ΛΛ/8

xyz

200

1920

240

1760

220

1600

200

1440

180

unit: nm

X. Ni, et al. Science-Express, Dec. 22, 2011 (Shalaev & Boltasseva groups) Science v. 335, 427 (2012)

Page 55: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Incident Angle Sweep – Refraction

λ = 1500 nm

Page 56: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

λ = 1500 nm

Incident Angle Sweep – Reflection

Page 57: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

θi = 30⁰

Broadband!

Broadband Negative Refraction

Page 58: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Ultra-thin planar meta-lenses: design

• Au film (30 nm) by electron beam evaporation

• Babinet antennas fabrication by focused ion beam (FIB)

r

X. Ni etal (2012)

Page 59: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Ultra-thin planar meta-lenses: experiment

sample

x-polarizer

y-polarizer

Ar/Kr laser (676 nm / 530 nm / 476 nm)

Z = 0 μm

Z = 7 μm

Z = 10 μm

Focal length: 2.5 μm Focal length: 4 μm Focal length: 7 μm

wavelength 676 nm

Page 60: Generalized Snell’s Laws - rqc.ru · Optical camouflage: Projecting background image onto masked object. Optical Camouflage, Tachi Lab, U. of Tokyo, Japan The Invisible Man by H

Take home messages

• Nanophotonics enabled by Plasmonics and Metamaterials

• Toward Better Materials for MM and TO applications

• Negative-index metamaterials

• Transformation optics and cloaking

• Engineering PDOS & Sub-wavelength light confinement with Hyperbolic MMs

• Flat photonics with Metasurfaces: Generalized Snell’s Law, negative refraction, meta-lens, meta-hologram….