Low-pass rugate spatial lters for beam smoothing Zhaoming Luo a,b , Shuangchun Wen a, , Zhixiang Tang a , Hailu Luo a , Yuanjiang Xiang a , Dongmo Song a a Key Laboratory for Micro/Nano Optoelectronic Devices of Ministry of Education, School of Computer and Communication, Hunan University, Changsha 410082, China b College of Information and Telecommunications Engineering, Hunan Institute of Science and Technology, Yueyang 414004, China abstract article info Article history: Received 18 September 2009 Received in revised form 24 January 2010 Accepted 22 February 2010 Keywords: Rugate structure Spatial lter Beam smoothing A new application of rugate structures is proposed as low-pass spatial lters for beam smoothing. By using the transfer matrix method to analyze the spatial properties of the bandgap of rugate structures, the low- pass rugate spatial lters with both an almost ideal at bandpass and a rather steep switching between pass- and stop-bands are designed. The angle-domain bandwidth of the spatial lters can be adjusted by changing the parameters of rugate structures for a given light frequency. The near-eld simulations carried out by using the nite-difference time-domain technique conrm the possibility of an efcient light smoothing. © 2010 Elsevier B.V. All rights reserved. 1. Introduction Many applications in optics require the use of beams of a good spatial quality characterized by a smooth envelope and, respectively, a narrow spatial spectrum. The cleanbeams diverge less in propaga- tion, and they can be focused more tightly and robust against nonlinear lamentation than the dirtyones. In laser science, the beam smoothing is usually achieved by using low-pass spatial lters. A simple and conventional low-pass spatial lter is implemented by the use of a telescope consisting of two focusing lenses in a confocal arrangement and an appropriate pinhole in the focus plane [13]. The pinhole lets the passing of the low angle-domain components and the blocking of the undesired high ones (related to the noisypart of the beam); therefore the beam after passing through the low-pass spatial lter is smoothed. The system, although widely used, has several deciencies as a relatively large size (at least four focal lengths long), high sensitivity to alignment (since the focused beam must past exactly through the middle of the pinhole) or the absence of efcient focusing lenses in infrared and in ultraviolet frequencies [3,4]. The spatial lters may also be applied to image enhancement and information processing in several regions of the electromagnetic spectrum, such as spatial spectrum analysis, matched ltering, radar data processing, aerial imaging industrial quality control, and biomedical applications. Currently, some slab spatial lters are performed for the purpose of overcoming the disadvantages of conventional spatial lters [312]. The possibilities for the realization of the low-pass, high-pass, and bandpass spatial lters have been demonstrated, whereas the slab lters based on the resonant grating systems [5,6], multilayer stacks combined with a prism [7] and two-dimensional photonic crystals [4,810] are only used as one-dimensional spatial lters. However, beam smoothing in fact demands two-dimensional spatial ltering. The spatial lters including metamaterials [3,11,12] can realize two- dimensional spatial ltering, but the fabrication of metamaterials is more difcult than that of multilayer stacks or photonic crystals since the structure unit of metamaterials is much less than the wavelength of light transmitting inside them. As a result, the way to realize two- dimensional spatial ltering for beam smoothing by using metama- terials is limited in practice. Thus it is necessary to do further work on the easily realizable spatial lters for beam smoothing. Rugate structures are optical thin lm with graded refractive- index proles. Compared with conventional multilayer stacks, they have some advantages including low internal stress, suppression of sidelobes, and continuous index matching for broadband antireec- tion coatings [1319]. Hence the performance of some devices such as frequency lters can be greatly improved, and spatial and spatial frequency ltering using one-dimensional graded-index lattices with defects is proposed [20]. In this paper, we utilize the the spatial properties of the bandgap of rugate structures to design the low-pass spatial lters with both an almost ideal at bandpass and a rather steep switching between pass- and stop-bands. The effects caused by the spatial lters on two-dimensional beam smoothing are demon- strated by using the nite-difference time-domain simulations. 2. Structure model and numerical simulation In order to obtain a strongly pronounced frequency property of very smooth high transmittance regions on both sides of the stop- band, we consider the 51-layer Gaussian half-apodized rugate Optics Communications 283 (2010) 26652668 Corresponding author. Fax: + 86 731 8823474. E-mail address: scwen@vip.sina.com (S. Wen). 0030-4018/$ see front matter © 2010 Elsevier B.V. All rights reserved. doi:10.1016/j.optcom.2010.02.047 Contents lists available at ScienceDirect Optics Communications journal homepage: www.elsevier.com/locate/optcom