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Perfect lens makes a perfect trap

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Abstract

In this work, we present for the first time a new and realistic application of the “perfect lens”, namely, electromagnetic traps (or tweezers). We combined two recently developed techniques, 3D negative refraction flat lenses (3DNRFLs) and optical tweezers, and experimentally demonstrated the very unique advantages of using 3DNRFLs for electromagnetic traps. Super-resolution and short focal distance of the flat lens result in a highly focused and strongly convergent beam, which is a key requirement for a stable and accurate electromagnetic trap. The translation symmetry of 3DNRFL provides translation-invariance for imaging, which allows an electromagnetic trap to be translated without moving the lens, and permits a trap array by using multiple sources with a single lens. Electromagnetic trapping was demonstrated using polystyrene particles in suspension, and subsequent to being trapped to a single point, they were then accurately manipulated over a large distance by simple movement of a 3DNRFL-imaged microwave monopole source.

©2006 Optical Society of America

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Supplementary Material (4)

Media 1: MPG (8945 KB)     
Media 2: MPG (7211 KB)     
Media 3: MPG (6157 KB)     
Media 4: MPG (7139 KB)     

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Figures (5)

Fig. 1.
Fig. 1. (a) Three-dimensional PhC fabricated layer by layer (20 layers in total). The inset shows a conventional cubic unit cell of the bcc structure. (b) Band structure of the bcc lattice PhC.
Fig. 2.
Fig. 2. Image of the optimized monopole source achieved through the 3D PhC flat lens at 39mm away from the source (the lens is 25mm thick). The outlined region shows the area of the image where the intensity was>0.5 max.
Fig. 3.
Fig. 3. The schematic of the basic apparatus used for the microwave tweezers. The inset shows the polarization of the electric field with regard to the PhC.
Fig. 4.
Fig. 4. (a,b) Microwave electromagnetic trapping of neutral particles through a negative-refraction flat lens [Media 1]. (c, d) Microwave electromagnetic dragging of neutral particles along the vertical axis [Media 2]. Based on the result shown in Fig. 4(a,b), the monopole source has moved 10mm along the vertical axis. (e,f) Microwave electromagnetic dragging of neutral particles along the horizontal axis. Based on the result shown in Fig. 4(c,d), the monopole source has moved 6mm along the horizontal axis [Media 3].
Fig. 5.
Fig. 5. Microwave electromagnetic trapping of neutral particles with different sizes. The average diameter of the large particles and that of the small particles are 100μm and 600μm, respectively. Two circles are used to track the motion of particles. [Media 4]
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