Bandwidth control of forbidden transmission gaps in compound structures with subwavelength slits

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Phase resonances in transmission compound structures with subwavelength slits produce sharp dips in the transmission response. For all equal slits, the wavelengths of these sharp transmission minima can be varied by changing the width or the length of all the slits. In this paper we show that the wi...

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Autor principal: Skigin, D.C
Otros Autores: Loui, H., Popovic, Z., Kuester, E.F
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2007
Acceso en línea:Registro en Scopus
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100 1 |a Skigin, D.C. 
245 1 0 |a Bandwidth control of forbidden transmission gaps in compound structures with subwavelength slits 
260 |c 2007 
270 1 0 |m Skigin, D.C.; Grupo de Electromagnetismo Aplicado, Departamento de Física, Ciudad Universitaria, Pabellón I, C1428EHA Buenos Aires, Argentina; email: dcs@df.uba.ar 
506 |2 openaire  |e Política editorial 
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504 |a Loui, H., Kuester, E.F., Skigin, D.C., Popovic, Z., ; Loui, H., (2006), Ph.D. dissertation, University of Colorado, Boulder; Lewin, L., Chang, D.C., Kuester, E.F., (1977) Electromagnetic Waves and Curved Structures, 2. , Series IEE Electromagnetic Waves (Peter Peregrinus, Stevenage, England 
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520 3 |a Phase resonances in transmission compound structures with subwavelength slits produce sharp dips in the transmission response. For all equal slits, the wavelengths of these sharp transmission minima can be varied by changing the width or the length of all the slits. In this paper we show that the width of the dip, i.e., the frequency range of minimum transmittance, can be controlled by making at least one slit different from the rest within a compound unit cell. In particular, we investigate the effect that a change in the dielectric filling, or in the length of a single slit, produces in the transmission response. We also analyze the scan angle behavior of these structures by means of band diagrams and compare them with previous results for all-equal slit structures. © 2007 The American Physical Society.  |l eng 
593 |a Grupo de Electromagnetismo Aplicado, Departamento de Física, Ciudad Universitaria, Pabellón I, C1428EHA Buenos Aires, Argentina 
593 |a Sandia National Laboratories, P.O. Box 5800, Albuquerque, NM 87185-1330, United States 
593 |a Department of Electrical and Computer Engineering, University of Colorado, Boulder, CO 80309-0425, United States 
593 |a Consejo Nacional de Investigaciones Científicas y T́cnicas (CONICET), Av. Rivadavia 1917, C1033AAJ, Buenos Aires, Argentina 
690 1 0 |a BAND STRUCTURE 
690 1 0 |a BANDWIDTH 
690 1 0 |a DIELECTRIC MATERIALS 
690 1 0 |a OPTIMIZATION 
690 1 0 |a WAVELENGTH 
690 1 0 |a BANDWIDTH CONTROL 
690 1 0 |a COMPOUND STRUCTURES 
690 1 0 |a TRANSMISSION GAPS 
690 1 0 |a TRANSMISSION MINIMA 
690 1 0 |a MOLECULAR STRUCTURE 
700 1 |a Loui, H. 
700 1 |a Popovic, Z. 
700 1 |a Kuester, E.F. 
773 0 |d 2007  |g v. 76  |k n. 1  |p Phys. Rev. E Stat. Nonlinear Soft Matter Phys.  |x 15393755  |t Physical Review E - Statistical, Nonlinear, and Soft Matter Physics 
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856 4 0 |u https://doi.org/10.1103/PhysRevE.76.016604  |y DOI 
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