Ultralow refractive index substrates-a base for photonic crystal slab waveguides
Out of plane radiation losses in two-dimensional ( 2 D ) photonic crystal ( PC ) waveguides occur due to a lack of total internal reflection at the core-substrate∕superstrate boundaries. In order to minimize these losses, either a high vertical refractive index contrast or deep etching into the subs...
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creator | Schmidt, M. Boettger, G. Eich, M. Morgenroth, W. Huebner, U. Boucher, R. Meyer, H. G. Konjhodzic, D. Bretinger, H. Marlow, F. |
description | Out of plane radiation losses in two-dimensional
(
2
D
)
photonic crystal
(
PC
)
waveguides occur due to a lack of total internal reflection at the core-substrate∕superstrate boundaries. In order to minimize these losses, either a high vertical refractive index contrast or deep etching into the substrate is required [
G. Boettger
,
C. Liguda
,
M. Schmidt
, and
M. Eich
,
Appl. Phys. Lett.
81
,
2517
(
2002
)
]. The maximum vertical contrast is achieved in air bridge type
PC
waveguides, which are inherently fragile. In this article, we introduce a concept which combines the advantages of a high vertical index contrast of an air bridge with those of a solid substrate. This approach consists of mesoporous silica as substrate material with an ultralow refractive index (
n
=
1.14
at
1.3
μ
m
), close to that of air. Finite
2
D
PC
line defect resonators consisting of an optical polymer as core and mesoporous silica as substrate were fabricated. Compared to ordinary substrates with higher refractive indices like silica or amorphous Teflon [
C. Liguda
,
G. Boettger
,
A. Kuligk
,
M. Eich
,
H. Roth
,
J. Kunert
,
W. Morgenroth
,
H. Elsner
, and
H. G. Meyer
,
Appl. Phy. Lett.
78
,
2434
(
2001
)
], measurements show significantly increased transmission at the resonance wavelength and virtually no losses on the sensitive air band side. |
doi_str_mv | 10.1063/1.1767962 |
format | Article |
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(
2
D
)
photonic crystal
(
PC
)
waveguides occur due to a lack of total internal reflection at the core-substrate∕superstrate boundaries. In order to minimize these losses, either a high vertical refractive index contrast or deep etching into the substrate is required [
G. Boettger
,
C. Liguda
,
M. Schmidt
, and
M. Eich
,
Appl. Phys. Lett.
81
,
2517
(
2002
)
]. The maximum vertical contrast is achieved in air bridge type
PC
waveguides, which are inherently fragile. In this article, we introduce a concept which combines the advantages of a high vertical index contrast of an air bridge with those of a solid substrate. This approach consists of mesoporous silica as substrate material with an ultralow refractive index (
n
=
1.14
at
1.3
μ
m
), close to that of air. Finite
2
D
PC
line defect resonators consisting of an optical polymer as core and mesoporous silica as substrate were fabricated. Compared to ordinary substrates with higher refractive indices like silica or amorphous Teflon [
C. Liguda
,
G. Boettger
,
A. Kuligk
,
M. Eich
,
H. Roth
,
J. Kunert
,
W. Morgenroth
,
H. Elsner
, and
H. G. Meyer
,
Appl. Phy. Lett.
78
,
2434
(
2001
)
], measurements show significantly increased transmission at the resonance wavelength and virtually no losses on the sensitive air band side.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.1767962</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>American Institute of Physics</publisher><ispartof>Applied physics letters, 2004-07, Vol.85 (1), p.16-18</ispartof><rights>2004 American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c347t-7774d526af76d5e3cad764eb44390c4892dcf5857c1199b95fd50b66cf1b1f93</citedby><cites>FETCH-LOGICAL-c347t-7774d526af76d5e3cad764eb44390c4892dcf5857c1199b95fd50b66cf1b1f93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Schmidt, M.</creatorcontrib><creatorcontrib>Boettger, G.</creatorcontrib><creatorcontrib>Eich, M.</creatorcontrib><creatorcontrib>Morgenroth, W.</creatorcontrib><creatorcontrib>Huebner, U.</creatorcontrib><creatorcontrib>Boucher, R.</creatorcontrib><creatorcontrib>Meyer, H. G.</creatorcontrib><creatorcontrib>Konjhodzic, D.</creatorcontrib><creatorcontrib>Bretinger, H.</creatorcontrib><creatorcontrib>Marlow, F.</creatorcontrib><title>Ultralow refractive index substrates-a base for photonic crystal slab waveguides</title><title>Applied physics letters</title><description>Out of plane radiation losses in two-dimensional
(
2
D
)
photonic crystal
(
PC
)
waveguides occur due to a lack of total internal reflection at the core-substrate∕superstrate boundaries. In order to minimize these losses, either a high vertical refractive index contrast or deep etching into the substrate is required [
G. Boettger
,
C. Liguda
,
M. Schmidt
, and
M. Eich
,
Appl. Phys. Lett.
81
,
2517
(
2002
)
]. The maximum vertical contrast is achieved in air bridge type
PC
waveguides, which are inherently fragile. In this article, we introduce a concept which combines the advantages of a high vertical index contrast of an air bridge with those of a solid substrate. This approach consists of mesoporous silica as substrate material with an ultralow refractive index (
n
=
1.14
at
1.3
μ
m
), close to that of air. Finite
2
D
PC
line defect resonators consisting of an optical polymer as core and mesoporous silica as substrate were fabricated. Compared to ordinary substrates with higher refractive indices like silica or amorphous Teflon [
C. Liguda
,
G. Boettger
,
A. Kuligk
,
M. Eich
,
H. Roth
,
J. Kunert
,
W. Morgenroth
,
H. Elsner
, and
H. G. Meyer
,
Appl. Phy. Lett.
78
,
2434
(
2001
)
], measurements show significantly increased transmission at the resonance wavelength and virtually no losses on the sensitive air band side.</description><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNp1kEtLAzEUhYMoWKsL_0G2LqbmTiZJs3AhxRcUdFHXQ54aGTslN23tv3ekFVeuLof7cTh8hFwCmwCT_BomoKTSsj4iI2BKVRxgekxGjDFeSS3glJwhfgxR1JyPyMtrV7Lp-i3NIWbjStoEmpY-fFFcWxx-JWBlqDUYaOwzXb33pV8mR13eYTEdxc5YujWb8LZOPuA5OYmmw3BxuGOyuL9bzB6r-fPD0-x2XjneqFIppRovammikl4E7oxXsgm2abhmrpnq2rsopkI5AK2tFtELZqV0ESxEzcfkal_rco84bG9XOX2avGuBtT8mWmgPJgb2Zs-iS8WU1C__h391tH86-Df9eGbg</recordid><startdate>20040705</startdate><enddate>20040705</enddate><creator>Schmidt, M.</creator><creator>Boettger, G.</creator><creator>Eich, M.</creator><creator>Morgenroth, W.</creator><creator>Huebner, U.</creator><creator>Boucher, R.</creator><creator>Meyer, H. G.</creator><creator>Konjhodzic, D.</creator><creator>Bretinger, H.</creator><creator>Marlow, F.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20040705</creationdate><title>Ultralow refractive index substrates-a base for photonic crystal slab waveguides</title><author>Schmidt, M. ; Boettger, G. ; Eich, M. ; Morgenroth, W. ; Huebner, U. ; Boucher, R. ; Meyer, H. G. ; Konjhodzic, D. ; Bretinger, H. ; Marlow, F.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c347t-7774d526af76d5e3cad764eb44390c4892dcf5857c1199b95fd50b66cf1b1f93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schmidt, M.</creatorcontrib><creatorcontrib>Boettger, G.</creatorcontrib><creatorcontrib>Eich, M.</creatorcontrib><creatorcontrib>Morgenroth, W.</creatorcontrib><creatorcontrib>Huebner, U.</creatorcontrib><creatorcontrib>Boucher, R.</creatorcontrib><creatorcontrib>Meyer, H. G.</creatorcontrib><creatorcontrib>Konjhodzic, D.</creatorcontrib><creatorcontrib>Bretinger, H.</creatorcontrib><creatorcontrib>Marlow, F.</creatorcontrib><collection>CrossRef</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schmidt, M.</au><au>Boettger, G.</au><au>Eich, M.</au><au>Morgenroth, W.</au><au>Huebner, U.</au><au>Boucher, R.</au><au>Meyer, H. G.</au><au>Konjhodzic, D.</au><au>Bretinger, H.</au><au>Marlow, F.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Ultralow refractive index substrates-a base for photonic crystal slab waveguides</atitle><jtitle>Applied physics letters</jtitle><date>2004-07-05</date><risdate>2004</risdate><volume>85</volume><issue>1</issue><spage>16</spage><epage>18</epage><pages>16-18</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>Out of plane radiation losses in two-dimensional
(
2
D
)
photonic crystal
(
PC
)
waveguides occur due to a lack of total internal reflection at the core-substrate∕superstrate boundaries. In order to minimize these losses, either a high vertical refractive index contrast or deep etching into the substrate is required [
G. Boettger
,
C. Liguda
,
M. Schmidt
, and
M. Eich
,
Appl. Phys. Lett.
81
,
2517
(
2002
)
]. The maximum vertical contrast is achieved in air bridge type
PC
waveguides, which are inherently fragile. In this article, we introduce a concept which combines the advantages of a high vertical index contrast of an air bridge with those of a solid substrate. This approach consists of mesoporous silica as substrate material with an ultralow refractive index (
n
=
1.14
at
1.3
μ
m
), close to that of air. Finite
2
D
PC
line defect resonators consisting of an optical polymer as core and mesoporous silica as substrate were fabricated. Compared to ordinary substrates with higher refractive indices like silica or amorphous Teflon [
C. Liguda
,
G. Boettger
,
A. Kuligk
,
M. Eich
,
H. Roth
,
J. Kunert
,
W. Morgenroth
,
H. Elsner
, and
H. G. Meyer
,
Appl. Phy. Lett.
78
,
2434
(
2001
)
], measurements show significantly increased transmission at the resonance wavelength and virtually no losses on the sensitive air band side.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.1767962</doi><tpages>3</tpages></addata></record> |
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language | eng |
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source | AIP Journals Complete; AIP Digital Archive |
title | Ultralow refractive index substrates-a base for photonic crystal slab waveguides |
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