A PROPOSAL FOR ANTI-UVB FILTER BASED ON ONE-DIMENSIONAL PHOTONIC CRYSTAL STRUCTURE

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Digest Journal of Nanomaterials and Biostructures Vol. 7, No. 1, January - March 2012, p. 367-371 A PROPOSAL FOR ANTI-UVB FILTER BASED ON ONE-DIMENSIONAL PHOTONIC CRYSTAL STRUCTURE HAMED ALIPOUR-BANAEI *, FARHAD MEHDIZADEH a Electrical Department, Faculty of Engineering, Tabriz Branch, Islamic Azad University, Tabriz, Iran a Electrical Department, Faculty of Engineering, Ahar Branch, Islamic Azad University, Ahar, Iran In this work we proposed an Anti-UVB filter based on 1D photonic crystal structures. The UVB radiation is very harmful for human beings and its range is between 280 nm and 320 nm of wavelengths. It can cause many skin disorders. It is harmful for eye and also affects DNA and drugs. So filtering it out of sun light is very important. In this paper we design a filter to forbidden this hazardous radiation. The proposed structure has a bandgap between 280 nm and 320 nm. Transfer Matrix Method (TMM) is used for simulation of this structure. (Recieved December 15. 2011; Accepted March 9, 2012) 1. Introduction Human beings are daily exposed to Ultra Violet (UV) radiation from the sun. UVB (280nm- 320nm) makes up 4% to 5% of UV light but is the most effective constituent of solar light. UVB causes sunburn 1000 times more than UVA [1]. UVB radiation is the main culprit of various skin anomalies like erythema and edema [2]. Phototoxic effects induced by UVB radiation involve the generation of Reactive Oxygen Species (ROS) resulting in oxidative damage [3]. These events can ultimately lead to diseases related to UV radiation, such as irritation or sunburn, photo allergy and skin cancer [4]. UVB irradiation results in DNA damage and delayed apoptosis and cell death [5]. Photo aging is also occurring mainly due to UVB radiation [6]. UVB radiation has harmful effects on eyes and also some drugs and chemically alters their functionality. Furthermore increased levels of UVB radiation during winter and spring time threatens the survival of life on the earth, also by present trend of ozone depletion it became even worse. According to above discussion filtering out the UVB radiation from the solar light is very crucial for human health. So in this work we aim to design a filter which is able to filter the UVB radiation and pass the rest of the sun light. For this purpose we suggest photonic crystals. Photonic crystals are the best candidates for designing ultra compact structures. As far as we know photonic crystals are periodic arrays of dielectric layers with alternating refractive indices. The period of these arrays is called lattice constant. According to their structure and the periodicity of the refractive index distribution they are divided into three categories: one-dimensional, two-dimensional and three-dimensional photonic crystals (1D PhC, 2D PhC and 3D PhC). One of the most important characteristics of these artificial structures is their Photonic Band Gap (PBG). Photonic band gap is a special region in the band structure of photonic crystals in which no optical wave is allowed to propagate through them. That is, any optical ray striking to these structures, if it s wavelength be in the band gap range of the photonic crystal, the ray will be reflected completely and it won t be able to penetrate into the structure [7-8]. Optical circulators [9], optical switches [10], power splitters [11], optical demultiplexers [12-13] and optical filters [14] are some reported examples of photonic crystal based devices. * Corresponding author: alipour@iaut.ac.ir

368 One-dimensional photonic crystal filters are very popular among the researchers. Defect mode properties [15], light transmission characteristics [16] and photonic band gap controlling [17] in one-dimensional photonic crystals have been investigated. There has been much kind of one-dimensional photonic crystal filters. For example a 1D Si/SiO 2 photonic crystal filter for thermo photovoltaic applications has been proposed [18] in which large oscillations around 1.45-1.75 μm in the pass band of this PhC filter would reduce the above band gap power transmitted to cells, leading to discounts of system efficiency and power density. Another example of recent works on 1D photonic crystal is a narrow pas band and narrow transmission angle filter [19]. This structure was composed of two parts: the first part was a 1D PhC with positive refractive index defect layer and the second part was a 1D PhC with negative refractive index defect layer. So it was capable of filtering the incident angle and only the waves which are normal to the structure at the specified frequency are allowed to transmit through the filter. In this work we propose a structure, a one-dimensional photonic crystal based filter whose band gap is such that it can filter the UVB radiation and so no UVB radiation is allowed to pass through this structure but other rays of the sun light can pass through it. 2. Mathematical theory In order to design our anti-uvb filter based on photonic crystals we should calculate the band structure of the photonic crystal based filter and try to locate its band gap in the desired wavelength range. Transfer Matrix Method [20] is the simplest and the most straight forward tool for analyzing 1D PhC s so we employ it to do our simulations and calculations. Firs we briefly introduce the TMM method. The schematic of our one dimensional photonic crystal is shown in Fig. 1. Fig. 1. The schematic of the proposed structure. The transmittance in the structure: (1) And the reflectance: (2) are directly determined by the transmission coefficient and the reflection coefficient respectively. According to TMM, and are expressed as follow: (3) and (4) Where M 11 and M 12 are the matrix element of total transfer matrix M for the entire structure given by (5)

369 Where N is the number of the periods and is the transfer matrix of one period given by Where is the dynamical matrix given by: (6) 1 1 (7) Where m=0, 1 and 2 that m=0 represents the free space and is the the ray angle in each layer and is the propagation matrix given by: exp 0 1,2, (8) 0 exp Where is the thickness of the dielectric layers and in which ω is the angular frequency. 3. Calculations and results Every one-dimensional photonic crystal is composed of two dielectric layers with different refractive indices which are repeated in one-direction. These refractive indices and the thickness of the layers are very important and directly control the band gap of the one-dimensional photonic crystal. The center wavelength of the photonic band gap of one-dimensional photonic crystal should satisfy the following relation: (9) Where and are the refractive indices and and are the thicknesses of the first and the second dielectric layers, respectively and is the center wavelength of photonic band gap. In order to have large band gap we use the following relation: (10) As we know the UVB radiation wavelength lays between 280 nm and 320 nm. So we have to design a one-dimensional photonic crystal based filter such that its band gap lies between 280 nm and 320 nm. So our center wavelength is 300 nm. So we should have 150 (11) And the optical thickness ( ) of our layers should be: 75 (12) By trial and error to find the most suitable band gap we choose that the refractive index of the first and the second layer to be 1.8 and 1.4 which are correspondent to Au and MgF2, respectively. From equation (12) we calculated the thicknesses of the layers that are approximately as follow: 42

370 And 53 And the number of the periods is 10 it means that totally we have 20 layers consisting of 10 Au and 10 MgF2 layers the total thickness of our filter is 1.9 m. The transmittance and reflectance spectrum of our filter is demonstrated in Fig. 2. As we can see from Fig.2 the band gap is in our desired range and all the UVB radiation will be reflected from it. (a) (b) Fig. 2 (a) reflectance and (b) transmittance spectrum of the proposed filter. As shown in reflectance characteristic of the structure, PBG is between 280 nm and 320 nm and we conclude that the proposed structure is useful for anti-uvb filtering. 4. Conclusion In this paper we proposed a new one-dimensional photonic crystal based filter for filtering out the UVB radiation of sun light. Our filter is composed of 10 periodic bilayers of Au and MgF2.

The photonic band gap of our photonic crystal based filter is approximately between 275 nm and 325 nm which is suitable for filtering the UVB radiation. 371 References [1] Matsumura, Y., Ananthaswamy, H.N., Toxic evects of ultraviolet radiation on the skin. Toxicology and Applied Pharmacology 195, 298 308 (2004). [2] de Gruijl, F.R., Longstreth, J., Norval, M., Cullen, A.P., Slaper, H.,Kripke, M.L., Takizawa, Y., Van der Leun, J.C., Health effect from stratospheric ozone depletion and interaction with climate change. Photochemistry Photobiology Science 2(1), 16 28 (2003). [3] Bayerl, C., Taake, S., Moll, I., Jung, E.G., Characterization of sunburn cells after exposure to ultraviolet light. Photo dermatol. Photo immunol. Photomed. 11, 149 154 (1995). [4] Black, H.S., De Gruijl, F.R., Forbes, P.D., Cleaver, J.E., Anathaswamy,H.N., de Fabo, E.C., Ulrich, S.E., Tyrrell, R.M., Photocarcinogenesis:an overview. J. Photochem. Photobiol. B 40, 29 (1997). [5] Godar, D.E., Miller, S.A., Thomas, D.P., Immediate and delayed apoptotic cell death mechanisms: UVA versus UVB and UVC radiation Cell Death Differ. 1, 59 66 (1994). [6] Longstreth, J., de Gruiji, F.R., Kripke, M.L., Abseck, S., Arnold, F.,Slaper, H.I., Velders, G., Takizawa Vanderleun, Y., Healthrisks. Journal of Photochemistry and Photobiology B 46, 20 (1998). [7] Sakoda K, Optical Properties Of Photonic Crystals. Springer-Verlag, Berlin (2001). [8] Joannopoulos J D, Meade R D and Winn J N, Photonic Crystals: Molding the Flow of Light, Princeton. University Press, Princeton, NJ, USA (1995). [9] Wang Z and Fan S, Optical circulators in two dimensional magneto-optical photonic crystals Optics Lett. 30, 1989-1991 (2005). [10] Cuesta-Soto F. et al. All optical switching structure based on a photonic crystal directional coupler Optics Express 12, 161-167 (2004). [11] Bayindir M et al. Photonic crystal based beam splitter Appl. Phys. Lett. 77, 3902-3904 (2000). [12] Rostami A et al, An ultra compact photonic crystal wavelength division demultiplexer using resonance cavities in a modified Y-branch structure Optik 122, 1481-1485 (2011). [13] Rostami A et al, A novel proposal for DWDM demultiplexer design using modified-t photonic crystal structure Photonic and Nanostructures Fundamentals and Applications 8, 14-22 (2010). [14] Qiu M and Jaskorzynska B, Design of channel drop filter in a two dimensional triangular photonic crystal Appl. Phys. Lett 83, 1074-1076 (2003). [15] Aly A H, defect mode properties in a one-dimensional photonic crystal Physica B doi: 10.1016/j.physb.20011.09.137 (2011). [16] Lin Y and Xu H, Research in light transmission characteristics of 1-dimensional photonic crystal Optik int. Light Electron Opt.doi: 10.1016/j.ijleo.2011.02.027 (2011). [17] Q. Zhu, et al. Control of photonic band gaps in one-dimensional photonic crystals Optik 122, 330-332 (2011). [18] Mao L. and Ye H, New development of one-dimensional Si/SiO 2 photonic crystals filter for thermo photo volataic applications Renewable Energy 35, 249-256 (2010). [19] Lin M and Xu J, Narrow pass-band and narrow transmission-angle filter by photonic heterostructures containing negative index materials IEEE ICMMT Proceedings 1662-1664 (2010). [20] Yeh P, Optical Waves in Layered Media Wiley New York Chap. 6 (1998).