# Long-range surface plasmons in dielectric-metal-dielectric structure with highly anisotropic substrates Page: 3

This
**article**
is part of the collection entitled:
UNT Scholarly Works and
was provided to Digital Library
by the UNT College of Arts and Sciences.

#### Extracted Text

The following text was automatically extracted from the image on this page using optical character recognition software:

LONG-RANGE SURFACE PLASMONS IN DIELECTRIC-...

t)p

s- l

1 + 6~(4)

C m 1m (2 - ,x6z)32(68m1 + )1/2

L(t) - 2 6

C," Em ,Z (Ea + exEz + 2Ez 1Em )(7)

at k- oc. Since (s is symmetric with respect to ex and ez, the

equivalent isotropic dielectric constant may be defined as

eis= E . The dispersion curve for the structure with

equivalent isotropic dielectrics (dotted line) lies in between

the solid and the dashed lines in Fig. 1. The dispersion

curves are plotted for silver film of thickness of d= 50 nm.

The numerical values of the principal dielectric constants are

taken to be 2 and 7.5. These are the homogenized values

obtained in the low-frequency limit for photonic crystal of Si

cylinders arranged in a square lattice with Si filling of 57%.15

The larger value 7.5 corresponds to the dielectric constant

along the cylinders. In the plane of periodicity, the photonic

crystal is isotropic with dielectric constant equals 2.

The asymmetry of the dispersion Eq. (3) with respect to

the interchange ex - Ez gives rise to different propagation

lengths for two different orientations. Since only the case of

weak dissipation is of practical interest, we consider the re-

gion of frequencies where the imaginary part of the dielectric

function of the metal film em()= E'(Wo)+ie"(wO) is small,

i.e., e" e'. For a typical metal this condition is valid in the

infrared and visible regions. In weakly dissipative medium,

the wave vector acquires small imaginary part, k=k' +ik".

Expanding the dispersion Eq. (3) over e" and k" and keeping

the linear terms, the following result for the propagation

length L(w)= 1/2k" is obtained:

L() 1 x - + d K- -MeK2

28 K2 z K1 Ex K1 Im ,

2 2 d m K Ex -1

X 1 2K2 + K2

m2c2K 4c2K2 Ex K2

(5)

Apart from the factor 1 / e", all the quantities on the right-

hand side (rhs) are calculated for a lossless metal, e"=0. The

propagation length L(w) -0 when w-+ s. As it was men-

tioned in the introduction, this effect is due to surface plas-

mon dispersion (vanishing of the group velocity) but not due

to increase in dissipation. The dispersion equation Eq. (3)

and the propagation length Eq. (5) can be simplified in the

limiting case of thick film.

The limit d--+ oc is readily obtained from Eqs. (3) and (5).

In this limit the surface plasmons propagating along two

metal-dielectric interfaces do not interact with each other,

therefore the dispersion relation is reduced to the result ob-

tained in Ref. 3 for semi-infinite metal

k- 6 6m12 ). (6)

C \mm- x6/z

Now, using Eq. (6), we obtain from Eq. (5) the following

result for the propagation length:Of course, in the case of isotropic dielectrics, ex= Ez, Eqs.

(3)-(8) are reduced to the well-known results.3,16-21

The calculation of propagation length in the limit when

d oc and in the limit when w - ws can both be considered

equivalent because at frequencies close to resonant fre-

quency os, the decay length K21 -0 (since the surface plas-

mon wave vector k- oc). For the evanescent field of surface

plasmon, this has the same effect as having a semi-infinite

metal film. Consequently, the propagation length

L(w) -- (w- )3/2 for a metal film of any given thickness

close to resonant frequency, as one obtains from Eq. (7).

In the opposite limit of thin film, d--+ 0, Eq. (5) is simpli-

fied in the long-wavelength regime, i.e., when surface plas-

mon behaves like a transverse light wave2 (c)3 E 3

L(w) - 2 3/2

S d2 Ex83/2(I m zm +(8)

In this approximation the dispersion relation w = kc/ 6 does

not contain characteristics of the metal but the propagation

length does. It follows from Eq. (8) that for fixed w, the

propagation length scales as d-2, which is a signature of the

long-range surface plasmon. Analysis of the long-wavelength

limit shows that the favorable orientation in the limit of thin

film (d 0) is not the same as the one in the case of a

semi-infinite film (d- oc). In the limit of thin film (for a

given frequency), [L(w)]-lo ex3/2, while in the case of a

semi-infinite film, [L(w)]- ex8 2. There is a certain critical

frequency Wcr (for a given thickness d of metal film) at

which the favorable orientation reverses (see Fig. 2). The

dependence of critical frequency on the thickness d of the

metal film is discussed in more detail later in this paper.

Further examination of asymptotes in the linear dispersion

regime (w= kc/ 6V) reveals some interesting details. The as-

ymptote in the limit of thin film (kd C 1) is given by Eq. (8),

and in the limit of thick film (kd > 1), we obtain from Eq. (5)(9)

L(w) ~ (m-6 kd > 1.

exmk (6mI + 2z)The linear dispersion regime in the limit of very thin metal

film spans over a broad range of frequencies, while in the

case of very thick metal film, the linear dispersion regime is

limited only to low frequencies (see Fig. 3). Although very

thin film favors a much longer propagation length (see Figs.

2 and 4), it is relatively more difficult to reach the resonance

frequency w (see Fig. 3). In addition to this, the surface

plasmon density of states dk/dw for very thin films is rela-

tively very low (due to the greater slope dOw/dk of the dis-

persion curve), leading to the decrease in probability of light

emission. We note that in the limit of very thick metal, the

form of Eq. (9) is different from Eq. (7), because, linear

dispersion does not span over a broad frequency range as

compared to linear dispersion in the limit of very thin metal.

However, at very low frequencies (in the long wavelength

regime), both Eqs. (7) and (9) are reduced to085426-3

PHYSICAL REVIEW B 81, 085426 (2010)

## Upcoming Pages

Here’s what’s next.

## Search Inside

This article can be searched. **Note: **Results may vary based on the legibility of text within the document.

## Citing and Sharing

Basic information for referencing this web page. We also provide extended guidance on usage rights, references, copying or embedding.

### Reference the current page of this Article.

Nagaraj & Krokhin, Arkadii A. Long-range surface plasmons in dielectric-metal-dielectric structure with highly anisotropic substrates, article, February 22, 2010; [College Park, Maryland]. (digital.library.unt.edu/ark:/67531/metadc103273/m1/3/: accessed January 23, 2017), University of North Texas Libraries, Digital Library, digital.library.unt.edu; crediting UNT College of Arts and Sciences.