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负折射率的最大优点在于超透镜效应,可以很好的解决成像分辨率以及信息传输的精度。![]()
提供你一些参考文献:
•1. V.G. Veselago, Soviet Physics USPEKHI, 10, 509 (1968).
•2. J.B. Pendry, A.J. Holden, D.J. Robbins, and W.J. Stewart,IEEE transactions on microwave theory and techniques, 47,2075 (1999).
•3. R.A. Shelby, D.R. Smith, S.C. Nemat-Nasser and S. Schultz, Appl. Phys. Lett., 78, 4 (2001).
•4. R.A. Shelby, D.R. Smith, and S. Schultz, Science 292, 77 (2001).
•5. Kolinko, P., and Smith, D.R., 2003, Optics Express, 11, 640 (2001).
•6. A.A. Houck, J.B. Brock, and I.L. Chuang, Phys. Rev. Lett., 90, 137401 (2003).
•7. C.G. Parazzoli, R.B. Greegor, K. Li, B.E.C. Koltenbah, and M. Tanielian, Phys. Rev Lett., 90 107401-1 (2003).
•9. C. Luo, S.G. Johnson, J.D. Joannopoulos, and J.B. Pendry, Opt. Express, 11, 746 (2003).
•10. E. Cubukcu, K. Aydin, E. Ozbay, S. Foteinopoulou, C. M.Soukoulis, “Electromagnetic waves: Negative refraction by photonic crystals,” Nature, 423, 604 (2003)
•11. P. V. Parimi, W. T. Lu, P. Vodo, S. Sridhar, “Photonic crystals: Imaging by flat lens using negative refraction,” Nature, 426, 404 (2003).
•12. E. Cubukcu, K. Aydin, E. Ozbay, S. Foteinopolou, C. M. Soukoulis, “Subwavelength resolution in a two-dimensional photonic-crystal-based superlens,” Phys. Rev. Lett., 91,207401 (2003).
•13. A. Grbic, and G.V. Eleftheriades, Appl. Phys. Lett., 82, 1815(2003).
•14. C.G. Parazzoli, R.B. Greegor, J.A. Nielson, M.A. Thompson, K. Li, A.M. Vetter and M.H. Tanielian, Appl.Phys. Lett., to appear (2004).
•15. J.B. Pendry, Phys. Rev. Lett., 85, 3966 (2000).
•16. N. Fang, Z. Liu, T.J. Yen, and X. Zhang, Optics Express, 11,682 (2003).
•17. J.B. Pendry, and S.A. Ramakrishna, J. Phys. Condensed Matter., 14, 6345 (2003).
•18. Focus Issue: Negative Refraction and Metamaterials Opt.Express, 11, 639-755 (2003).
•19. M.W. McCall, A. Lakhtakia, and W.S. Weiglhofer, ‘Thenegative index of refraction demystified’, European Journal of Physics, 23, 353 (2002).
•20. K. S. Yee, “Numerical solution of initial boundary value problems involving Maxwell’s equations in isotropic media,” IEEE Trans. Antennas Propagat., vol. 14, pp. 302–307, May 1966.
•21. C.-K. Cheng, J. Lillis, S. Lin, and N. Chang, Interconnect Analysis andSynthesis. New York: Wiley, 2000, ch. 5.
•22 . T. Namiki, “A new FDTD algorithm based on alternating-direction implicit method,” IEEE Trans. Microwave Theory Tech., vol. 47, pp. 2003–2007, Oct. 1999.
•23. J. B. Pendry, A. J. Holden, D. J. Robbins, and W. J. Stewart, IEEE Trans. Microwave Theory Tech. 47, 2075 ~1999!.
•24 I. S. Schelkunoff and H. T. Friis, in Antennas: Theory and Practice, edited by S. Sokolnikoff ~Wiley, New York, 1952!, p. 584.
•25. D. R. Smith, W. Padilla, D. C. Vier, S. C. Nemat-Nasser, and S. Schultz, Phys. Rev. Lett. 84, 4184 ~2000!.
•26. H. F. Contopanagos, C. A. Kyriazidou, W. M. Merrill, and N. G. Alexopoulos, J. Opt. Soc. Am. A 16, 1682 ~1999!.
•27.W. P. Huang, S. T. Chu, A. Goss, and S. K. Chaudhuri, “A scalar finitedifference time-domain approach to guided-wave optics,” IEEE Photon.Technol. Lett., vol. 3, pp. 524–526, June 1991.
•28.W. P. Huang, S. T. Chu, and S. K. Chaudhuri, “A semivectorial finitedifference time-domain method,” IEEE Photon. Technol. Lett., vol. 3, pp. 803–806, Sept. 1991.
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