{"id":2788,"date":"2011-07-19T15:06:26","date_gmt":"2011-07-19T15:06:26","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2011\/?p=2788"},"modified":"2011-07-19T15:06:26","modified_gmt":"2011-07-19T15:06:26","slug":"nanostructured-gradient-index-antireflection-diffractive-optics","status":"publish","type":"post","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2011\/nanostructured-gradient-index-antireflection-diffractive-optics\/","title":{"rendered":"Nanostructured Gradient-Index Antireflection Diffractive Optics"},"content":{"rendered":"

In recent years there has been significant interest in broadband, omnidirectional antireflection (AR) nanostructures that minimize Fresnel reflection due to index (impedance) mismatch at an optical interface [1<\/a>] <\/sup> [2<\/a>] <\/sup>.\u00a0 The reflection can be suppressed by using adiabatic impedance matching implemented as an intermediate material with gradually varying index in the direction of surface normal. Subwavelength patterning is an effective method to implement such a gradient index (GRIN) surface.\u00a0 However, these recent studies have been mostly restricted to planar surfaces.\u00a0 Diffractive optical elements such as diffraction gratings, Fresnel zone plates, and holographic optics also suffer from Fresnel reflection losses evidenced as undesirable reflection orders.\u00a0 Recently, we proposed a new class of GRIN diffractive optics that is capable of suppressing such reflection losses [3<\/a>] <\/sup>.\u00a0 Using the same GRIN principles, we can demonstrate diffractive elements where the reflected energy can be suppressed.<\/p>\n

The proposed concept of the nanostructured GRIN grating is illustrated in Figure 1, where subwavelength tapered nanostructures with period p<\/em> are integrated on both the ridge and groove of the grating. \u00a0Top-view and cross-section micrographs of the fabricated GRIN grating in silicon substrate are depicted in Figure 2. The grating has a period \u039b of 5 mm, and the subwavelength cone-shaped pillars have nominal base diameter of 150 nm. The fabricated structure resembles a grating with nano-engineered surfaces. A cross-sectional micrograph is shown in Figure 2(b), where the cone heights on the ridge and groove are 650 and 600 nm, respectively. Some point defects characteristic of nanosphere self-assembly used in the fabrication process can be observed.\u00a0 Broadband characterization of the fabricated structure indicated suppression by at least two orders of magnitude in the reflected orders of the GRIN grating over a large range of incident angles up to 60\u00ba.<\/p>\n\n\t\t