journal article·2017-10-01Open access

Interactions between the first mode and the second Bragg gap in a cylindrical waveguide with undulated walls

Jiu-Ling Xue, Huan Liu, Ting Liu, Fu-Hou Zheng, Ya-Xian Fan, Zhi-Yong Tao

AIP Advances· Volume 7· Issue 10

Abstract

Bragg resonances caused by the same transverse modes can always play a major role in periodic waveguides when the period is larger than the average radius. Because of higher-order mode cutoffs, the related Bragg gaps can be identified as interactions between different spatial harmonics of the fundamental mode, and the first Bragg gaps are more intensive than the higher ones. When we alter the parameters of the periodic waveguide, especially, decrease the period, the first transverse mode can be involved in Bragg gaps. Here, we demonstrate a direct mode-stopband interaction between the first mode and the second Bragg gap, that an extraordinary passband arises in the original second Bragg gap and splits the bandgap into two. Furthermore, the extraordinary passband is mainly composed of a pure first mode, which effectively suppresses the transmission of the fundamental one. We have also investigated the influence of wall profiles on the transmission and mode purity, and have found that the defined shape factor of wall profiles is proportionally related to the width of both pass and stop bands. The results could benefit not only the understanding of wave phenomena but also the applications in mode generators, filters, and so on.
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Research context

OpenAlex topics: Photonic Crystals and Applications · Photonic and Optical Devices · Microwave Engineering and Waveguides

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Key Lab of In-fiber Integrated Optics, Ministry Education of China, Harbin Engineering University 1 , Harbin 150001, People’s Republic of China

Physics Research Center, College of Science, Harbin Engineering University 2 , Harbin 150001, People’s Republic of China

Funding

National Natural Science Foundation of China

References (27)

Show source-provided references
1. J. Appl. Phys. · 2005 · 97 · 11490710.1063/1.1922068 ↗
2. J. Appl. Phys. · 2011 · 110 · 01490410.1063/1.3599886 ↗
3. Philos. Mag. XXIV · 1887 · 14510.1080/14786448708628074 ↗
4. Phys. Scripta · 1996 · T66 · 14610.1088/0031-8949/1996/t66/025 ↗
5. Phys. Rev. Lett. · 2008 · 101 · 13450110.1103/physrevlett.101.134501 ↗
6. Phys. Rev. Lett. · 2006 · 96 · 01430110.1103/physrevlett.96.014301 ↗
7. Appl. Phys. Lett. · 2004 · 85 · 34110.1063/1.1772854 ↗
8. Phys. Rev. Lett. · 2005 · 94 · 11550110.1103/physrevlett.94.115501 ↗
9. J. Acoust. Soc. Am. · 1974 · 56 · 76810.1121/1.1903324 ↗
10. J. Acoust. Soc. Am. · 1994 · 96 · 184410.1121/1.410196 ↗
11. Math. Probl. Eng. · 2013 · 26729110.1155/2013/267291 ↗
12. Math. Probl. Eng. · 2015 · 51698210.1155/2015/516982 ↗
13. Phys. Rev. E · 1998 · 58 · R526110.1103/physreve.58.r5261 ↗
14. J. Acoust. Soc. Am. · 2002 · 112 · 135310.1121/1.1497625 ↗
15. Opt. Commun. · 2004 · 232 · 20110.1016/j.optcom.2003.12.067 ↗
16. Appl. Phys. Lett. · 2005 · 86 · 15111510.1063/1.1905804 ↗
17. Appl. Phys. Lett. · 2008 · 92 · 12192010.1063/1.2897296 ↗
18. Phys. Rev. E · 2008 · 78 · 01631110.1103/physreve.78.016311 ↗
19. J. Sound. Vib. · 2013 · 332 · 654110.1016/j.jsv.2013.07.027 ↗
20. J. Sound. Vib. · 2015 · 349 · 34810.1016/j.jsv.2015.03.047 ↗
21. J. Appl. Phys. · 2014 · 115 · 13350110.1063/1.4870137 ↗
22. J. Sound. Vib. · 2015 · 353 · 13510.1016/j.jsv.2015.05.013 ↗
23. J. Acoust. Soc. Am. · 2016 · 139 · 189810.1121/1.4945988 ↗
24. J. Appl. Phys. · 2009 · 105 · 12351510.1063/1.3152996 ↗
25. 2000 · 383
26. J. Sound. Vib. · 2008 · 313 · 83010.1016/j.jsv.2007.11.055 ↗
27. IEEE Trans. Plasma Sci. · 2003 · 31 · 75210.1109/tps.2003.815482 ↗