Optimizing the superlens: Manipulating geometry to enhance the resolution
Appl. Phys. Lett. 87, 231113 (2005); doi:10.1063/1.2139620
Published 30 November 2005
You are not logged in to this journal. Log in
We analyze the performance of a planar lens based on realistic negative index material in a generalized geometry. We demonstrate that the conventional superlens design (where the lens is centered between the object and the image) is not optimal from the resolution point of view, develop an analytical expression for the resolution limit of a generalized lens, use it to find the optimum lens configuration, and calculate the maximum absorption practical nearfield superlenses may have. We demonstrate that in contrast to the conventional superlens picture, planar imaging is typically accompanied by excitation of surface waves at both interfaces of the lens.
©2005 American Institute of Physics
| History: | Received 8 September 2005; accepted 31 October 2005; published 30 November 2005 |
| Permalink: |
http://link.aip.org/link/?APPLAB/87/231113/1 |
KEYWORDS and PACS
RELATED DATABASES
PUBLICATION DATA
0003-6951 (print)
1077-3118 (online)
REFERENCES (25)
For access to fully linked references, you need to log in.
For access to fully linked references, you need to Log in.
- V. G. Veselago,
Sov. Phys. Usp. 10, 509 (1968) . - J. B. Pendry, Phys. Rev. Lett. 85, 3966 (2000).
- P. V. Parimi, W. T. Lu, P. Vodo, and S. Sridhar,
Nature (London) 426, 404 (2003) . - A. Grbic and G. V. Eleftheriades, Phys. Rev. Lett. 92, 117403 (2004).
- V. A. Podolskiy and E. E. Narimanov, Phys. Rev. B 71, 201101(R) (2005);
- N. Fang, H. Lee, C. Sun, and X. Zhang,
Science 308, 534 (2005) . - W. Park and J.-B. Lee, Appl. Phys. Lett. 85, 4845 (2004).
- N. Garcia and M. Nieto-Vesperinas, Phys. Rev. Lett. 88, 207403 (2002).
- J. Pendry, Phys. Rev. Lett. 91, 099701 (2003).
- M. Nieto-Vesperinas and N. Garcia, Phys. Rev. Lett. 91, 099702 (2003).
- D. R. Smith, D. Schurig, M. Rosenbluth, S. Schultz, S. A. Ramakrishna, and J. B. Pendry, Appl. Phys. Lett. 82, 1506 (2003).
- R. Merlin, Appl. Phys. Lett. 84, 1290 (2004).
- K. J. Webb, M. Yang, D. W. Ward, and K. A. Nelson, Phys. Rev. B 70, 035602(R) (2004);
- I. A. Larkin and M. I. Stockman,
Nano Lett. 5, 339 (2005) . - V. A. Podolskiy and E. E. Narimanov,
Opt. Lett. 30, 75 (2005) . - G. Shvets,
Proc. SPIE 5221, 124 (2003) ;
G. Shvets and Y. A. Urzhumov, Phys. Rev. Lett. 93, 243902 (2004); - E. Cubukcu, K. Aydin, E. Ozbay, S. Foteinopolou, and C. M. Soukoulis, Phys. Rev. Lett. 91, 207401 (2003).
- A. L. Pokrovsky and A. L. Efros,
Appl. Opt. 42, 5701 (2003) . - G. Milton, N.-A. Nicorovici, R. McPhedran, and V. Podolskiy,
Proc. R. Soc. London, Ser. A 461, 3999 (2005) ;
N.-A. Nicorovici, R. McPhedran, and G. Milton, Phys. Rev. B 49, 8479 (1994). - N. Kuhta, G. Milton, and V. Podolskiy (unpublished).
- J.W. Goodman, Introduction to Fourier Optics (Roberts & Company, Greenwood Village, CO, 2004);
- Note that for all practical applications

,µ![[double-prime]](http://scitation.aip.org/stockgif3/Prime-script.gif)
106 this condition is achievable only in near-field a,b<
. - Some applications may require a nonzero distance between the back surface lens and the image plane. In these systems, the a=b configuration is unachievable and the optimal configuration that minimizes b will need to be selected accordingly.
- V. A. Podolskiy, A. K. Sarychev, and V. M. Shalaev,
Opt. Express 11, 735 (2003) . - S. Linden, C. Enkrich, M. Wegener, J. Zhou, T. Koschny, and C. M. Soukoulis,
Science 306, 1351 (2004) .
G. Shvets and Y. A. Urzhumov,







