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Hollow core planar waveguides and multilayers

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Simplest mirrors present thin layers of metals such as aluminum deposited ... a p-polarised light reflectivity goes through zero at a so called Brewster angle. ... – PowerPoint PPT presentation

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Title: Hollow core planar waveguides and multilayers


1
Hollow core planar waveguides and multilayers
  • Prof. M. Skorobogatiy, review for the course
  • Introduction to Photonic Crystals
  • École Polytechnique de Montréal
  • Montréal, QC, Canada

2
Hollow core planar waveguide, scaling relations
T
T
ql/D
R3
R
D
R2
R4
D2/l
I1
REFLECTOR
T
T
TIR silica fiber D10mm l1.55mm,
loss0.2dB/km T10-6-10-5
3
Metallic reflectors
q
Metallic Reflector Omnidirectional reflection,
high material loss in the IR
  • Simplest mirrors present thin layers of metals
    such as aluminum deposited on glass substrates.
    Choice of metals will determine reflection
    characteristics of a mirror.
  • Aluminum is the cheapest and least expensive
    material with a coefficient of reflection of
    88-92 in the visible.
  • More expensive is silver with reflectivity of
    95-99 even in the IR, while less than 90 in
    the blue and UV.
  • Most expensive is gold with an excellent
    reflectivity of 98-99 in the IR, while poor
    reflectivity below 550 nm.

4
Losses of hollow metallic waveguides
D100mm l1-10mm T10-2 Losses1-10 dB/m
5
Dielectric reflectors
Reflectance
1
Contraste dindice saugmente
s-pol
p-pol
SiO2-air 0.04 AsSe-air 0.22
Conventional Dielectric Mirrors Very low material
absorption loss, strong dependence of reflection
characteristics on the light polarization
Contraste dindice saugmente
q1
tan-1(nh/nl)
90o
0
  • Dielectric mirrors are characterised by very low
    absorption losses, but their reflection
    characteristics are strongly dependent of the
    angle of radiation incidence and polarization.
    For the s-polarized light reflectivity increases
    monotonically with an increase of an angle of
    incidence. However, for a p-polarised light
    reflectivity goes through zero at a so called
    Brewster angle.

6
Losses of hollow dielectric waveguides
T
D100mm l1-10mm nc1 nr1.5 LossesTE0.04-4
dB/cm
ql/D
R
D
I1
REFLECTOR
7
ARROW waveguides
l1.55mm LossesTE0.2 dB/cm
8
ARROW multilayer waveguides
9
Planar antiresonant reflecting optical (ARROW)
waveguides, SiN/SiO2 (2.1/1.46)
dc3.7mm
12mm
Capillary
1 layer
Sensor applications - putting the light where the
analyte (gas) is
2 layers
3 layers
D. Yin et al. 14 June 2004 / Vol. 12, No. 12 /
OPTICS EXPRESS 2710
10
Omnidirectional reflectorsORhigh index contrast
multilayers
11
Multilayer dielectric reflectors
Omnidirectional Dielectric Mirrors Reflection for
all angles of incidence and polarizations
normal q0o
Ep
Es
q
q90o
  • Omnidirectional reflection - for any incoming
    polarization and any angle of incidence radiation
    is completely reflected in a certain frequency
    band.

12
Omnidirectional dielectric reflectors
13
Omnidirectional dielectric reflectors
14
Omnidirectional dielectric reflectors
When cladding index nc is increased beyond a
critical value, omnidirectional reflectivity is
lost.
15
Omnidirectional reflectorsSURPRIZE !!!low index
contrast multilayers
16
All-polymer multilayers
17
Giant birefringence polymer multilayers
18
Giant birefringence polymer guides
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