7. Guided-wave optics
Optical waveguides
slab strip fiber
strip embedded strip rib or ridge strip loaded
Symmetric & Asymmetric waveguides
Cladding (or, cover) : nc
Core (or, film) : nf
Cladding (or, substrate) : ns x
y
Guided waves
A waveguide
Electromagnetic modes of waveguides
A mode of a waveguide is a stable, propagating pattern of electric and magnetic fields that is periodic along the axis of the waveguide, apart from attenuation
7.1 Planar perfect-mirror waveguides
Waveguide modes
Condition of self-consistency
2 2
cos 2 (1 2 sin ) - 2 sin 2 sin AB AC AC AC AB AC d
Bounce angles
(Transverse Component)
: The ray-optics picture of light guidance by multiple reflections
2d k ym 2
mPropagation constants
Bounce angle Propagation constant
z
2 2 2 2 2
( / )
m kzm k kym k m d
k nk
0k
ymm d
msin m m 2 d
0 sin
ym m
k nk
2 2 2
( / )
m k m d
Field distributions : TE modes
The complex amplitude of the total field in the waveguide is the superposition of the two bouncing TEM plane waves :
upward wave + downward wave
= +
: symmetric modes, odd modes
: antisymmetric modes, even modes
are normalized
are orthogonal in [-d/2. d/2] interval
Assume that the bouncing TEM plane wave is polarized in the x direction,
the guided wave is a transverse-electric (TE) wave.
TE mode
(
x, 0, 0); (0,
y,
z)
E E H H H H
Each mode can be view as a standing waves in the y direction, traveling in the z direction.
Modes of large m vary in the transverse plane at a greater rate ky, and travel with a smaller propagation constant .
The field vanishes at y = +d/2 for all modes, so that the boundary conditions at the surface of the mirrors are always satisfied.
[ TE guided waves ]
Number of modes
( d < /2 )
( /2 < d < ) single-mode waveguide
Group velocities
Group velocity of mode m :
More oblique modes travel with a smaller group velocity
since they are delayed by the longer path of the zigzaging process.
Geometrically,
Field distributions : TM modes
upward wave + downward wave Magnetic field is in the x direction,
the guided wave is a transverse-magnetic (TM) wave.
Since the z component of the electric field is parallel to the mirror, it must behave like the x component of the TE mode :
y components of the electric field:
m Ez
Ey E
z components of the electric field:
E
(0,
y,
z); (
x0, 0) E E E H H H
TM mode
Multimode fields
( m = 1 )
( m = 2 )
( m = 1 & 2 )
7.2 Planar dielectric waveguides
Cladding (or, cover) : nc
Core (or, film) : nf
Cladding (or, substrate) : ns x
y
n
1Let’s first consider a symmetric waveguide.
Transverse Component of the wavevector
: The ray-optics picture of light guidance by multiple reflections
Self-consistency condition
2 2 sind 2m
(Perfect mirror)
2d k ym 2m (Perfect mirror)
Self-consistency condition : TE modes
Self-consistency condition (TE mode)
From the TIR of TE modes,
Self-consistency condition : TE modes
(open circles)
0,1, 2,
m
Number of modes : TE modes
Single-mode waveguide (TE mode) In a dielectric waveguide, there is at least one TE mode, since the fundamental mode m = 0 is always allowed.
No cutt-off frequency
Propagation constants : TE modes
: propagation constant ( the z-component of wavevector)
n
11 2 M
Field distributions : TE modes
: Extinction coefficient
Confinement factor
the ratio of power in the slab to the total power
Dispersion relation
2 2 2 2
1 2 1 2
2 2
2 2
1 1
2 tan
c
n n n n
m n n
n n
0 0
/
N c Nk
/ 2
0/(2 )
c
c d NA
(N : effective index)
Single-mode waveguide (TE mode)
Nk
0
3 modes
1 mode
2 modes
c2
c1
Group velocities
The group velocities lie between c
1and c
2(the phase velocities in the slab and substrate).
At a given ,
the lowest-order mode (the least oblique mode, m = 0) travels with a group velocity closest to c
1.
The most oblique mode (m = M) has a group velocity ~ c
2.
The higher mode is faster than the lower!
Group velocities
1 GH cos
c
z
More oblique modes travel this lateral distance at a fast speed than less oblique modes
증명 !!!
The higher mode is faster than the lower!
Lateral shift
Time delay
Goose-Hanchen shift
Goose-Hanchen effect Evanescent field
Now, consider asymmetric waveguides.
( Slab )
For TE modes :
Guided TE modes :
Evanescent waves (x > d, x < 0)
Penetration distances
Guided waves ( d > x > 0)
Transverse wavevector ( d > x > 0)
Effective thickness of the waveguide
Dispersion relation for TE modes in a planar dielectric waveguide
Dispersion relation & Effective thickness
Normalized frequency : V
Dispersion relation for TE modes in terms of V , b and a:
Dispersion relation for TM modes in terms of V , b and a:
(TE)
(TE)
Summary of planar dielectric waveguides
TE :
TM :
has two modes .
7.3 Two-dimensional waveguides
Comparison : the number of modes
0
M 2d NA l
æ ö÷
ç ÷
» çççè ø÷÷÷
0 0
2 / 2
d d
M = l = l
2 2
0 0
2 1
4 4 / 2
d d
M p
l p l
æ ö÷ æ ö÷
ç ÷ ç ÷
» çççè ÷÷÷ø = çççè ÷÷÷ø
2 2
0
2 4
M p d NA l
æ ö÷
ç ÷
» çççè ø÷÷÷
1-d Mirror Guide
1-d Dielectric Guide
2-d Mirror Guide
2-d Dielectric Guide
(
0)
0
2 d
V p NA k d NA
= l =
For the mirror guide the number of modes is just the number of ½ wavelengths that can fit.
For dielectric guides
it is the number that can fit but now limited by the angular cutoff characterized by the NA of the guide
7.4 Optical coupling in waveguides
A. Mode excitation
Input couplers
Coupling by focusing beam
End butt Coupling
Prism coupling
B. Coupling between waveguides
In the n1 slab waveguide, In the n2 slab waveguide, When a is very large (no-coupling)
Derivation of coupled wave equations
n1 n2
: coupling coefficient.
Coupled wave equations
Coupling coefficients
Phase mismatch per unit length
Exchange of power
Exchange of power when the guides are identical (phase-matched)
: transfer distance
: 3-dB coupling
Power transfer ratio in a small phase mismatched case
EO, TO, MO waveguide switches