Philosophical Transactions A

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Philosophical Transactions A Design, fabrication and characterization of indefinite metamaterials of nanowires by Jie Yao, Yuan Wang, Kun-Tong Tsai, Zhaowei Liu, Xiaobo Yin, Guy Bartal, Angelica M. Stacy, Yuh-Lin Wang, and Xiang Zhang Philosophical Transactions A Volume 369(1950):3434-3446 September 13, 2011 ©2011 by The Royal Society

(a) Hyperbolic iso-frequency contour for an anisotropic indefinite medium when εv>0 and εp<0, and circular iso-frequency contour for an isotropic medium such as air. (a) Hyperbolic iso-frequency contour for an anisotropic indefinite medium when εv>0 and εp<0, and circular iso-frequency contour for an isotropic medium such as air. For an oblique incidence from air, the Poynting vector is negatively refracted inside the medium, although the wave vector undergoes positive refraction. (b) A typical realization of an indefinite metamaterial composed of an array of parallel metallic nanowires embedded in a dielectric matrix. (c,d) εp and εv values (real parts) as functions of wavelength in a vacuum with two different filling ratios of 0.1 (dashed line) and 0.2 (solid line). Alumina permittivity ε=2.4 was used [20], and the data for permittivity of silver were obtained from literature [21]. (Online version in colour.)‏ Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

(a) Schematic of the vertical cross section of the porous alumina membrane formed on top of an aluminium substrate. (a) Schematic of the vertical cross section of the porous alumina membrane formed on top of an aluminium substrate. The curved layer at the bottom of each pore is the barrier layer. (b) Scanning electron microscope (SEM) image of the porous alumina template (top view). (Online version in colour.)‏ Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

Cross-sectional view of an AAO template after the growth of a silver nanowire using the electrochemical plating method. Cross-sectional view of an AAO template after the growth of a silver nanowire using the electrochemical plating method. (a) The centre part of the sample. (b) Close to the edge of the same sample in (a), the boundary between the nanowire filled and empty parts can be seen. The nanowires grow faster at the edge than at the centre part, and overgrown silver forms a block on top of the sample. Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

Atomic force microscope images of the template bottom surface morphology after removal of the barrier layers. Atomic force microscope images of the template bottom surface morphology after removal of the barrier layers. The two samples are fabricated using the two-step anodization approach. First anodization time is (a) 5 and (b) 24 h, respectively. (Online version in colour.)‏ Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

A three-dimensional simulation of light transmission through the anisotropic sample. A three-dimensional simulation of light transmission through the anisotropic sample. The sample is a slab made of nanowire/AAO composite. The nanowires are along the vertical direction. Incident light with 660 nm wavelength is illuminated on the sample through a 600 nm slit cut in the silver layer covering the bottom surface of the slab. (a) Nanowire array without any missing nanowires and (b,c) a nanowire array with one missing nanowire, whose position is shown by an arrow. (Online version in colour.)‏ Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

SEM images of two nanowire samples with different uniformity. SEM images of two nanowire samples with different uniformity. It is clear that the pores in (a) are much less ordered than those in (b) [4], and therefore more defects can be found in it. Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

SEM images of FIB pre-patterned samples. SEM images of FIB pre-patterned samples. (a) Pre-patterned Al film, (b) a nanopore array guided by the surface texture and (c) a silver nanowire array embedded in an AAO template fabricated by FIB pre-patterning. Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

Schematic setup for negative refraction in silver nanowire metamaterials (BS, beam splitter; L, tube lens; M, mirror; O, objective; P, polarizer; xyz-PZT, piezo-scanner tunable in xyz directions; AFM, atomic force microscope; PMT, photomultiplier tube). Schematic setup for negative refraction in silver nanowire metamaterials (BS, beam splitter; L, tube lens; M, mirror; O, objective; P, polarizer; xyz-PZT, piezo-scanner tunable in xyz directions; AFM, atomic force microscope; PMT, photomultiplier tube). The incident angle 1 is tuned by adjusting the position of the laser diode (D) with a one-dimensional stage (S). The inset illustrates a cross-sectional review of the light propagation of the TE mode (beam no. 2) and the TM mode (beam no. 3) inside the metamaterial. (Online version in colour.)‏ Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society

(a) Schematic picture of the light being negatively refracted at the air/metamaterial interface. (a) Schematic picture of the light being negatively refracted at the air/metamaterial interface. The light beam is narrowed by a slit cut through the silver seed layer. (b) Experimental results of NSOM detected output light beam location as the incident angle varies. Upper half, TM-polarized light; lower half, TE-polarized light. (Online version in colour.)‏ Jie Yao et al. Phil. Trans. R. Soc. A 2011;369:3434-3446 ©2011 by The Royal Society