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<ArticleSet>
<Article>
<Journal>
<PublisherName>OICC Press</PublisherName>
<JournalTitle>Majlesi Journal of Electrical Engineering</JournalTitle>
<Issn>2345-3796</Issn>
<Volume>16</Volume>
<Issue>3</Issue>
<PubDate PubStatus="epublish">
<Year>2022</Year>
<Month>09</Month>
<Day>15</Day>
</PubDate>
</Journal>
<ArticleTitle>Comparison of Chromatic Dispersion of Circular and Hexagonal Photonic Crystal Fibers with Chloroform-Core</ArticleTitle>
<VernacularTitle></VernacularTitle>
<FirstPage></FirstPage>
<LastPage></LastPage>
<ELocationID EIdType="doi">10.30486/mjee.2022.696507</ELocationID>
<Language>EN</Language>
<AuthorList>
<Author>
<FirstName>Ban Tran</FirstName>
<LastName>Le Tran</LastName>
<Affiliation>Department of Physics, Vinh University, Vinh, Vietnam</Affiliation>
<Identifier Source="ORCID">0000-0001-9097-9782</Identifier>
</Author>
<Author>
<FirstName>Thuy</FirstName>
<LastName>Nguyen Thi</LastName>
<Affiliation>University of Education, Hue University, Hue, Vietnam</Affiliation>
<Identifier Source="ORCID">0000-0001-7738-6720</Identifier>
</Author>
<Author>
<FirstName>Lanh</FirstName>
<LastName>Chu Van</LastName>
<Affiliation>Department of Physics, Vinh University, Vinh, Vietnam</Affiliation>
<Identifier Source="ORCID">0000-0001-7738-6720</Identifier>
</Author>
</AuthorList>
<PublicationType>Journal Article</PublicationType>
<History>
<PubDate PubStatus="received">
<Year>2022</Year>
<Month>09</Month>
<Day>15</Day>
</PubDate>
</History>
<Abstract>In this paper, we compare dispersion characteristics of chloroform-core photonic crystal fibers (PCFs) with circular lattice and hexagonal lattice in the case of different air hole diameters. By varying lattice constant É and filling factor in the first ring d1/É, we can easily control chromatic dispersion and achieve three optimal structures for the circular lattice of fibers #CF1 (É = 1.0 µm, d1/É = 0.65), #CF2 (É = 1.0 µm, d1/É = 0.7), and #CF3 (É = 2.0 µm, d1/É = 0.3) and two optimal structures for the hexagonal lattice of fibers #HF1 (É = 1.0 µm, d1/É = 0.5), #HF2 (É = 2.0 µm, d1/É = 0.3). At the same structural parameter (É = 2.0 µm, d1/É = 0.3) and the corresponding pumping wavelength, the circular structure has a dispersion smaller by 5.598 ps/mn/km than the hexagonal lattice. #CF1 has all-normal dispersion with the peak of the dispersion curve asymptote to the zero-dispersion curve which is very suitable for coherent supercontinuum generation (SCG). The #HF1 structure has a near-zero flat anomalous dispersion in the wide wavelength range from 1.1 µm to 1.4 µm. Our results will be an important premise in choosing a PCF structure to study SCG.</Abstract>
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<Object Type="keyword">
<Param Name="value">Chloroform</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Circular lattice</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Dispersion Characteristic</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Hexagonal lattice.</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Photonic crystal fibers</Param>
</Object>
</ObjectList>
</Article>
</ArticleSet>