Narrowband reflection-and-transmission filter in an annular defective photonic crystal containing an ultrathin metallic film |
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Authors: | Mei-Soong Chen Chien-Jang Wu Tzong-Jer Yang |
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Affiliation: | 1. Department of Electrical Engineering, Chung Hua University, Hsinchu 300, Taiwan;2. Institute of Electro-Optical Science and Technology, National Taiwan Normal University, Taipei 116, Taiwan;1. LPMR, Département de Physique, Faculté des Sciences, Université Mohamed Premier, 60000 Oujda, Morocco;2. Département de Physique, Faculté Pluridisciplinaire Nador, Université Mohamed Premier, 60000 Oujda, Morocco;3. IEMN, UMR CNRS 8520, Département de Physique, Université de Lille, 59655 Villeneuve d’Ascq, France;1. College of Electronic and Information Engineering, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China;2. Nanjing Artillery Academy, Nanjing 211132, China;3. State Key Laboratory of Millimeter Waves of Southeast University, Nanjing Jiangsu 210096, China;1. Department of Physics, School of Physical and Decision Sciences, Babasaheb Bhimrao Ambedkar University, Vidya Vihar, Raebareli Road, Lucknow, U.P. 226025, India;2. Department of Applied Physics, Amity Institute of Applied Sciences, Amity University, Uttar Pradesh, Noida 201303, India;3. Department of Physics, SLAS, Mody University of Science and Technology, Lakshmangarh 332311, Sikar, Rajasthan, India;4. Department of E & T, Amity School of Engineering and Technology, Amity University, Uttar Pradesh, Noida 201303, India;1. College of Arts and Sciences in Mahayel Aseer, Physics Department, King Khalid University, Abha, Saudi Arabia;2. Photovoltaic and Semiconductor Materials Laboratory, University of Tunis El-Manar-ENIT P.O. Box 37, Le Belvedere 1002-Tunis, Tunisia |
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Abstract: | The filtering properties for a narrowband reflection-and-transmission filter in an annular defective photonic crystal containing an ultrathin and strongly lossy metallic film are theoretically investigated based on the transfer matrix method for the cylindrical Bragg waves. At a certain design wavelength, simultaneous peaks in reflectance and transmittance can be found. The peak wavelength is shown to be dependent on the azimuthal mode number of the cylindrical waves. The peak heights in reflectance and transmittance can be directly varied by the stack numbers. In addition, the influence of the starting radius in reflectance and transmittance is also illustrated. |
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