Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation
Autor(a) principal: | |
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Data de Publicação: | 2019 |
Outros Autores: | , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Journal of Microwaves. Optoelectronics and Electromagnetic Applications |
Texto Completo: | http://old.scielo.br/scielo.php?script=sci_arttext&pid=S2179-10742019000100080 |
Resumo: | Abstract Photonic crystal fiber (PCF) structures with do-octagonal geometry have been studied. These do-octagonal PCF structure have smaller circular holes arranged in rhombic fashion at its centre. Moreover, these small holes are doped with materials like butanol, ethanol, methanol and propanol. Do-octagonal PCF structures doped with methanol and air filled structure report very high birefringence. Ultra flattened zero dispersion has been achieved by all the simulated structures. Besides, low confinement loss and large nonlinearity have also been reported. Numerical simulation for supercontinuum generation has been performed. Supercontinuum spectra obtained for peak power 1 kW, 2 kW, 5 kW and 10 kW are 650 nm, 950 nm, 1450 nm and 2050 nm respectively. |
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Journal of Microwaves. Optoelectronics and Electromagnetic Applications |
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Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generationPhotonic crystal fibersbirefringencesupercontinuum generationdispersionconfinement lossnonlinearityAbstract Photonic crystal fiber (PCF) structures with do-octagonal geometry have been studied. These do-octagonal PCF structure have smaller circular holes arranged in rhombic fashion at its centre. Moreover, these small holes are doped with materials like butanol, ethanol, methanol and propanol. Do-octagonal PCF structures doped with methanol and air filled structure report very high birefringence. Ultra flattened zero dispersion has been achieved by all the simulated structures. Besides, low confinement loss and large nonlinearity have also been reported. Numerical simulation for supercontinuum generation has been performed. Supercontinuum spectra obtained for peak power 1 kW, 2 kW, 5 kW and 10 kW are 650 nm, 950 nm, 1450 nm and 2050 nm respectively.Sociedade Brasileira de Microondas e Optoeletrônica e Sociedade Brasileira de Eletromagnetismo2019-03-01info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersiontext/htmlhttp://old.scielo.br/scielo.php?script=sci_arttext&pid=S2179-10742019000100080Journal of Microwaves, Optoelectronics and Electromagnetic Applications v.18 n.1 2019reponame:Journal of Microwaves. Optoelectronics and Electromagnetic Applicationsinstname:Sociedade Brasileira de Microondas e Optoeletrônica (SBMO)instacron:SBMO10.1590/2179-10742019v18i11454info:eu-repo/semantics/openAccessKumar,PranawFiaboe,Kokou FirminRoy,Jibendu Sekhareng2019-03-19T00:00:00Zoai:scielo:S2179-10742019000100080Revistahttp://www.jmoe.org/index.php/jmoe/indexONGhttps://old.scielo.br/oai/scielo-oai.php||editor_jmoe@sbmo.org.br2179-10742179-1074opendoar:2019-03-19T00:00Journal of Microwaves. Optoelectronics and Electromagnetic Applications - Sociedade Brasileira de Microondas e Optoeletrônica (SBMO)false |
dc.title.none.fl_str_mv |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation |
title |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation |
spellingShingle |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation Kumar,Pranaw Photonic crystal fibers birefringence supercontinuum generation dispersion confinement loss nonlinearity |
title_short |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation |
title_full |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation |
title_fullStr |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation |
title_full_unstemmed |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation |
title_sort |
Highly birefringent do-octagonal photonic crystal fibers with ultra flattened zero dispersion for supercontinuum generation |
author |
Kumar,Pranaw |
author_facet |
Kumar,Pranaw Fiaboe,Kokou Firmin Roy,Jibendu Sekhar |
author_role |
author |
author2 |
Fiaboe,Kokou Firmin Roy,Jibendu Sekhar |
author2_role |
author author |
dc.contributor.author.fl_str_mv |
Kumar,Pranaw Fiaboe,Kokou Firmin Roy,Jibendu Sekhar |
dc.subject.por.fl_str_mv |
Photonic crystal fibers birefringence supercontinuum generation dispersion confinement loss nonlinearity |
topic |
Photonic crystal fibers birefringence supercontinuum generation dispersion confinement loss nonlinearity |
description |
Abstract Photonic crystal fiber (PCF) structures with do-octagonal geometry have been studied. These do-octagonal PCF structure have smaller circular holes arranged in rhombic fashion at its centre. Moreover, these small holes are doped with materials like butanol, ethanol, methanol and propanol. Do-octagonal PCF structures doped with methanol and air filled structure report very high birefringence. Ultra flattened zero dispersion has been achieved by all the simulated structures. Besides, low confinement loss and large nonlinearity have also been reported. Numerical simulation for supercontinuum generation has been performed. Supercontinuum spectra obtained for peak power 1 kW, 2 kW, 5 kW and 10 kW are 650 nm, 950 nm, 1450 nm and 2050 nm respectively. |
publishDate |
2019 |
dc.date.none.fl_str_mv |
2019-03-01 |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://old.scielo.br/scielo.php?script=sci_arttext&pid=S2179-10742019000100080 |
url |
http://old.scielo.br/scielo.php?script=sci_arttext&pid=S2179-10742019000100080 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
10.1590/2179-10742019v18i11454 |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
dc.format.none.fl_str_mv |
text/html |
dc.publisher.none.fl_str_mv |
Sociedade Brasileira de Microondas e Optoeletrônica e Sociedade Brasileira de Eletromagnetismo |
publisher.none.fl_str_mv |
Sociedade Brasileira de Microondas e Optoeletrônica e Sociedade Brasileira de Eletromagnetismo |
dc.source.none.fl_str_mv |
Journal of Microwaves, Optoelectronics and Electromagnetic Applications v.18 n.1 2019 reponame:Journal of Microwaves. Optoelectronics and Electromagnetic Applications instname:Sociedade Brasileira de Microondas e Optoeletrônica (SBMO) instacron:SBMO |
instname_str |
Sociedade Brasileira de Microondas e Optoeletrônica (SBMO) |
instacron_str |
SBMO |
institution |
SBMO |
reponame_str |
Journal of Microwaves. Optoelectronics and Electromagnetic Applications |
collection |
Journal of Microwaves. Optoelectronics and Electromagnetic Applications |
repository.name.fl_str_mv |
Journal of Microwaves. Optoelectronics and Electromagnetic Applications - Sociedade Brasileira de Microondas e Optoeletrônica (SBMO) |
repository.mail.fl_str_mv |
||editor_jmoe@sbmo.org.br |
_version_ |
1752122126606794752 |