Metamaterials: Negative refractive index in ... - Theory.nipne.ro

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2.3.2. Less known history ("old" results, before Veselago’s; <strong>in</strong>complete list)"Everyth<strong>in</strong>g of importance has been said before, by someone who did not discover it".(Alfred North Whitehead, 1916, address to the British Association for the Advancement of Science;mathematician, philosopher, supervised Bertrand Russell mathematical dissertation).- Site: Alexander Moroz; http://www.wave-scatter<strong>in</strong>g.com/negative.html- S. A. Tretyakov, "Research on negative refraction and backward-wave media: A historicalperspective", EPFL Latsis Symposium 2005, Lausanne, Feb.-Mar. 2005- C. Caloz, T. Itoh, Electromagnetic <strong>Metamaterials</strong>: Transmission L<strong>in</strong>e <strong>Theory</strong> and MicrowaveApplications, Wiley, Hoboken, NJ, 2006, Ch. 1- H. Lamb, Proc. London Math. Soc. 1, 473 (1904)(backward waves; mechanical systems)- A. Schuster, An Introduction to the <strong>Theory</strong> of Optics, Edward Arnold,London, 1904, pp. 313-318 (backward eltm. waves)- H. C. Pockl<strong>in</strong>gton, Nature 71, 607 (1905) (phase velocity orientedopposite to the group velocity)- L. I. Mandel’shtam, Jh. Eksp.Teor. Fiz. 15, 476 (1945) (Russian);Complete Works, vol. 5, Academy of Sci. Publ.,Moscow, 1950, pp. 428-467- G. D. Malyuzh<strong>in</strong>ets, Jh. Tekh. Fiz. 21, 940 (1951) (Russian) (v panti II v g)- D. V. Sivukh<strong>in</strong>, Opt. Spektrosk. 3, 308 (1957) (Russian) (n < 0)ASTiGMAT
Examples of "old" resultsWire media <strong>in</strong> the 1960sW. Rotman, IRE Trans. Antenna Propagation10, 82 (1962)Split r<strong>in</strong>gs <strong>in</strong> the 1950sS. A. Schelkunoff et al, Antennas:<strong>Theory</strong> and Practice,Wiley, NY, 1952Backward-wave transmission l<strong>in</strong>esG. D. Malyuzh<strong>in</strong>ets, Jh. Tekh. Fiz. 21, 940 (1951)ASTiGMAT
Page 1 and 2: IFIN_Theor_Phys_Dept_111810
Page 3 and 4: 1. GoalIntroduction to the field of
Page 5 and 6: Metamaterials and
Page 7 and 8: More definitionsMe
Page 9 and 10: Founders of the modern metamaterial
Page 11: Pendry’s structures to obta<stron
Page 15 and 16: Specially dedicated journal- <stron
Page 17 and 18: Metamorphose-organized conferences
Page 19 and 20: 3. MetaPhysics of metamaterials: Ho
Page 21 and 22: Electromagnetic field spectrum≈ 8
Page 23 and 24: 3.2. Definition of
Page 25 and 26: 3.4. Examples of Pendry periodical
Page 27 and 28: Effective relative magnetic permeab
Page 29 and 30: Idealized hypotheses (in</s
Page 31 and 32: Generalized cell for NRI-transmissi
Page 33 and 34: 4.1. Negative refr
Page 35 and 36: 4.2. Behavior of convex and concave
Page 37 and 38: 4.4. Goos-Hänchen shift (effect)-
Page 39 and 40: "Ideal lens" - simplified descripti
Page 41 and 42: Partial conclusion and comments- On
Page 43 and 44: First experiments (2000-2001)1-D Me
Page 45 and 46: First experimentsNegative</
Page 47 and 48: Progress, microwavesExperiment to v
Page 49 and 50: Progress: from microwaves toward op
Page 55 and 56: Progress: near inf
Page 57 and 58: Progress: visible (2007)ASTiGMAT
Page 59 and 60: Swiss cross configuration (2009)New
Page 61 and 62: Mother Nature and PhCQuasi-periodic
Page 63 and 64:
7. High-interest p
Page 65 and 66:
Another slab (Veselago-Pendry-type)
Page 67 and 68:
7.1. Toward imagin
Page 69 and 70:
Example of partial camouflage, obta
Page 71 and 72:
Total invisibility
Page 73 and 74:
Results: invisibil
Page 75 and 76:
New (2008) cloakin
Page 77 and 78:
New (2009) reported cloakin
Page 79:
9. Conclusion- MTM is a fasc<strong
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