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Topological Description for Photonic Mirrors
Hong Chen
School of Physics, Tongji University, Shanghai , China
HKUST IAS, Jan. 11, 2016
Collaborators: Dr. Wei Tan, Dr. Yong Sun, Tongji Uni. Prof. Shun-Qing Shen , The University of Hong Kong
同舟共济
outline 1. Introduction
topological Insulators, band inversion
photonic analogs, mirrors as photonic insulators 2. Topological description: Theoretical study
mapping 1D Maxwell’s equations to Dirac equation
topological orders for photonic mirrors 3. Topological description: Experimental study
band inversion, microwave experiments
edge modes, microwave and visible light experiments 4. Summary
M. Z. Hasan et al., Rev. Mod. Phys. 82, 3045 (2010)
topological description for electronic insulators
1. Introduction
electronic medium
Metallic, unidirectional Edge state between insulators with different topological orders
Quantum Hall Effect
Chiral Edge State with H
Broken T-symmetry
Quantum Spin Hall Insulator
Edge states without H
with T-symmetry
M. Z. Hasan et al., Rev. Mod. Phys. (2010)
From ENGHETA and.ZIOLKOWSKI 2006
Materials Responds To EM Waves: Permittivity ε and Permeabilty µ
εµ±=n
double-positive (DPS)
forward-wave propagation
single-negative µ-negative
(MNG) evanescent wave
“barrier”
single-negative ε-negative
(ENG) evanescent wave
“barrier”
double-negative (DNG)
backward-wave propagation
zero-index materials
0,0 >< εµ
photonic medium: metamaterials with designed ε and μ
Materials Responds To EM Waves: Permittivity ε and Permeabilty µ
εµ±=n
Photonic Conductor Right-Handed
Photonic Insulator II MNG Mirror
Photonic Insulator I ENG Mirror
Photonic Conductor Left-Handed
Dirac-Point Related Medium Photonic Graphene?
0,0 >< εµ
analog to electrons
Q1:different topological orders between EMG and MNG mirrors ??
M. Z. Hasan et al., Rev. Mod. Phys. (2010)
semimetal for x < .07
semiconductor for .07 < x < .22
semimetal for x > .18
bands Ls;a invert at x ~ .04
Manipulating topological order: Electronic band inversion transition from normal insulator (NI) to TI [d=3]
Photonic analog
Experiments: Wang et al., Nature 461, 772 (2009).
Chirality
Nature materials 2012
Photonic analog
Mapping between electrons and photons
Schroedinger Equation :
Maxwell’s Equation :
Periodical Structures:
electronic band gaps , electron insulators
photonic band gaps (PBG) , photonic insulators
Photonic Crystals Yablonovitch and John 1987
For electronic and photonic NI, we have mapping: Schroedinger Eq. ↔ Maxwellʹs Eq. + photonic crytals
PBG as Normal Photonic Insulator
Band inversion transition in electronic systems:
theoretical description
(2013)
Dirac Equation (1928)
- Dirac matrices, for example:
d=1: d=2:
Q2: Dirac Eq. ↔ Maxwell’s Eq. + artificial structures?? we proposed: Metamaterials !
Band inversion : metematerial analogs
PBG in a 1D stack of ε-negative (ENG)/ µ-negative (MNG) pairs (Jiang et al., PRE 2004, 2006; Weng et al., PRE 2007; Jiang et al. AIP Adv. 2012, )
at sub-wavelength condition and normal incidence, a PBG structure: with the edge ωε and ω µ :
( )
( ) 0)()(
,0)()(
21
2211
21
2211
=++
=
=++
=
dddd
dddd
µµµ
εεε
ωµωµωµ
ωεωεωε
2101101 )( ,ωαµωµεε −==
2022202 ,)( µµωβεωε =−=
A structure made of opaque or "dark" metamaterials!!
ENG for ω < β1/2
MNG for ω < α1/2
Earlier studies:
2. Topological Description: theoretical study
T
ω
0,0 << µε 0,0 >> µε
0,0 <= µε 0,0 => µε
0,0 <> µε
µ-negative gap
DNG band
MNG gap
DPS band
0,0 =< µε 0,0 >= µε
0,0 >< µε
ENG gap ε-negative gap
ωε ω µ
ω µ ωε
band edges 𝝎𝜺,𝝁 inverted
Band inversion transition: metematerial analogs
tailoring ε and µ
Earlier studies:
Evidence: photonic band inversion in metamaterials
recent studies: 2013
Answers to the two questions
massive Dirac Eq.:
Maxwell’s Eq.: 0 ( )x z r yE i x Hωµ µ−∂ =
0 ( )x y r zH i x Eωε ε∂ = −
[ ] 1 1
2 2( ) ( )x x zi m x V x E
ϕ ϕϕ ϕ
− ∂ + + =
σ σ
metamaterials
1 0 zEϕ ε= 2 0 yHϕ µ=
( )( )2 r rm xc
ω ε µ= −
2 r rEc
ω ε µ= − +
( )( )2 r r r rV xc
ω ε µ ε µ = + − +
1. Mapping 1D Maxwell’s equations to 1D Dirac equation
<…..> : Average on space
2. EMG and MNG mirror as mass inversion in Dirac Eq.
For SNG mirror, if : 𝜖𝑟 ~ − 𝜇𝑟 ,𝐸 =𝜔2𝑐
𝜖𝑟 + 𝜇𝑟 ~ 0
Then at low energy 𝐸~0: the behavior of Dirac Eq. ONLY depends on the sign of the mass
𝑚 = 𝜔2𝑐
𝜖𝑟 − 𝜇𝑟 ~ 𝜔𝑐
𝜀𝑟 ~ − 𝜔𝑐𝜇𝑟
MNG mirror: 𝜀𝑟 > 0. 𝜇𝑟 < 0 positive mass: m > 0
ENG mirror: 𝜀𝑟 < 0. 𝜇𝑟 > 0 negative mass: m < 0
So, the sign of the mass is inverted from MNG to ENG :
Different topological orders for MNG and ENG: The first evidence
m > 0 m = 0 m < 0
Su-Schrieffer-Heeger Model for Polyacetylene (Rev. Mod. Phys. 1988)
Mapping the Dirac Eq. to the SSH model (S.Q Shen 2013)
Band inversion in the SSH model Mass inversion in the Dirac Eq.
Berry phase:
=�0 𝑓𝑓𝑓 ∆𝑡 > 0𝜋 𝑓𝑓𝑓 ∆𝑡 < 0
winding number:
𝜈
= �0 𝑓𝑓𝑓 Δ𝑡 > 0 𝑓𝑓 𝑚 > 0 and 𝐌𝐌𝐌 𝐦𝐦𝐦𝐦𝐦𝐦 1 𝑓𝑓𝑓 Δ𝑡 < 0 𝑓𝑓 𝑚 < 0 and 𝐄𝐌𝐌 𝐦𝐦𝐦𝐦𝐦𝐦
Therefore, MNG and ENG mirrors have Different topological orders!
Our study: Guo et al., PRE 2008; Chin. Phys. B 2008 multilayer structures or1D-PC made of dielectrics with (ε > 1, μ = 1) can act as SNG metamaterials in gap region
The gap divided into two parts: EMG and MNG
For asymmetry unit cell: mAB)(
For symmetry unit cell: mABA)(
The gap described by: EMG or MNG
Depending on symmetry of the unit cell.
Topological description: Extend to mirrors made of dielectric multilayers
Retrieval theory : Smith et al., PRB 2002 Bloch-wave-expansion theory: Kan et al., PRA 2009
Determination of effective parameters
Effective parameters in gap regime
The gap is divided into two parts: EMG and MNG
Dependence on periodic number 20,15,10:)( =mAB m
non-local effective parameters !! For asymmetry unit cell: mAB)(
MNG ENG
Effective parameters in gap regime
It can be shown: Ε and μ are independent of the periodic number
local effective parameters
10)(ABA
First gap Second gap
( )( )2 r rm x
cω ε µ= −
0 21 1 e
rs
C ip Ld
γε
ε ωω = − +
0 21 m
rs
p L iCd
γµ
µ ωω = − +
choosing different circuit parameters one gets DNG, ENG, MEG materials
1D Metamaterials Realized By Transmission Line
Eleftheriade et al., 2002; and by Itol et al., 2002
3. Topological Description: experimental study
1( ) gdkgd D
τω
π ω π= ∝DOS:
gτ : group delay D : sample length
Band Inversion in photonic chains
Simulations & Experiments
Edge modes in heterostructures made of ENG and MNG: Theory prediction
m < 0 ENG mirror m > 0 MNG mirror
dEdge mode
x 0 Edge mode:
Jackiw-Rebbi Solution (Phys. Rev. D 1976)
for
Edge mode at the interface between two photonic
mirrors with m>0 and m<0
Edge modes in heterostructures made of ENG and MNG: Microwave experiments
Edge modes in photonic chains: Microwave experiments
Poster presented by Jun Jiang
Poster presented by Kejia Zhu
Edge mode in heterostructure: (AB)6M
1D PC Metal
Incident light
A: SiO2 B: TiO2 M: Ag
nmdnmdnmd
nn
M
BA
BA
2.605.550.89
327.2443.1
===
==,
,
----- S1 , ----- S2 theoretical results
with different losses θ = 0o
….. S3 experimental results
θ = 15o
For λ = 589 nm, dM = 60.2 nm T < 1% without edge mode T = 33% with edge mode
Enhancement: 30 ∼ 40
MNG mirror m >0
Edge mode in heterostructures made of ENG and MNG: Visible-light experiments
Edge mode in sandwich structure: (AB)6M(BA)6
Metal
Incident light
(AB)5M(BA)5 S; A: SiO2 ; B: TiO2 ; M: Ag ; S: glass
nmdnmdnmd
nn
M
BA
BA
1.835.55,0.89
327.2,443.1
===
==
----- S1 , ----- S2 theoretical results
with different losses θ = 0o
….. S3 experimental results
θ = 15o
For λ = 589 nm , dM = 83.1 nm T = 0.15% without edge mode T = 38% with edge mode
Enhancement: 255
OPTICAL THICK metal film FAR FIELD excitation
MNG m >0 MNG m >0
Possible applications: plasmonics
M. Z. Hasan et al., Rev. Mod. Phys. (2010)
d < dc
NI TI
comparing to sandwich structures of electronic TI
Edge state → Resisdence 10-2 !
Extend to 2D structures
Plannar metamaterials made of transmission lines
Band gap inversion transition
0,0 <= µε
0,0 =< µε
0,0 =< µε
0,0 <= µε
m > 0 m < 0 m = 0
1 3 2 4
x- direction linearly polarized source
y- direction linearly polarized source 1
3
4
2
1
3
4
2 clockwise circularly polarized source
counterclockwise circularly polarized source 1
3
4
2
Thank You
Mapping Maxwell’s equation to Dirac Eq., it is shown 𝜖-negative and 𝜇-negative mirrors have different topological orders.
Realizing topological modes in structures made of photonic mirrors.
Proving new ways of applications based on photonic topological modes.
Financial Supports: NSFC, 973 Program of MOST
4. Summary