journal article·2007-10

Cloaking and imaging effects in plasmonic checkerboards of negative and and dielectric photonic crystal checkerboards

S. Guenneau, S. Anantha Ramakrishna, S. Enoch, Sangeeta Chakrabarti, G. Tayeb, B. Gralak

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Abstract

Negative refractive index materials are known to be able to support a host of surface plasmon states for both polarizations of light. This makes possible unique effects such as a perfect lens. Checkerboards consisting of alternating cells of positive and negative refractive index represent a very singular situation in which the density of modes diverges at the corners. This raises the question as to whether such effects will still be observed in a real dissipative system of finite size. We have considered several aspects of such structures including these and symmetry aspects (rectangular against triangular checkerboards). We have also studied silver checkerboards whose transverse extent is finite. Negative refractive index checkerboards bring new electromagnetic paradigms both through the intriguing possibilities they appear to offer, and the challenges they present to our understanding of the diffraction process. Most intriguing of all is the possibility of a triangular checkerboard lens whose resolution is limited not by wavelength, but only by the losses in the constituent materials, while a ray picture suggests it behaves as a perfect mirror. The resolution of this lens increases without limit as the losses tend to zero as shown by the generalized lens theorem. We finally show that light confinement can be achieved to certain extent using dielectric triangular photonic crystal (PC) checkerboards displaying the all-angle-negative-refraction (AANR) within the Bragg regime in p polarization. Effectively even a single rectangular or triangular PC can act as an open resonator that confines light in its neighborhood. This cloaking effect has been previously observed in PC slabs displaying the AANR effect. We show that the cloaking is enhanced for three triangular PC wedges sharing a vertex and further improved for 12 triangular PC wedges arranged in a checkerboard fashion.
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Research context

OpenAlex topics: Photonic Crystals and Applications · Metamaterials and Metasurfaces Applications · Plasmonic and Surface Plasmon Research

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (26)

Show source-provided references
1. Pendry · Contemp. Phys. · 2004 · 45 · 19110.1080/00107510410001667434 ↗
2. Ramakrishna · Rep. Prog. Phys. · 2005 · 68 · 44910.1088/0034-4885/68/2/R06 ↗
3. Veselago · Sov. Phys. Usp. · 1968 · 10 · 50910.1070/PU1968v010n04ABEH003699 ↗
4. Pendry · Phys. Rev. Lett. · 2000 · 85 · 396610.1103/PhysRevLett.85.3966 ↗
5. Pendry · J. Phys. Cond. Matter · 2003 · 15 · 634510.1088/0953-8984/15/37/004 ↗
6. Guenneau · New J. Phys. · 2005 · 7 · 16410.1088/1367-2630/7/1/164 ↗
7. Ramakrishna · Phys. Rev. A · 2007 · 75 · 06383010.1103/PhysRevA.75.063830 ↗
8. Maystre · J. Opt. Soc. Am. A · 2004 · 21 · 12210.1364/JOSAA.21.000122 ↗
9. Guenneau · Opt. Lett. · 2005 · 30 · 14610.1364/OL.30.001204 ↗
10. He · New J. Phys. · 2005 · 7 · 21010.1088/1367-2630/7/1/210 ↗
11. Martin-Moreno · Phys. Rev. Lett. · 2001 · 86 · 111410.1103/PhysRevLett.86.1114 ↗
12. Garcia de Abajo · Phys. Rev. Lett. · 2005 · 95 · 06740310.1103/PhysRevLett.95.067403 ↗
13. Absence of absorption in NRM means Maxwell’s operator is no longer elliptic and hence Lax-Milgram’s lemma ensuring existence and uniqueness of the solution to the diffraction problem is no longer applicable. Nevertheless, the Fredholm alternative ensures that if there is a solution for any applied electromagnetic field whose tangential component is continuous through interfaces separating complementary media (hence exhibiting two anti-parallel wave-vectors at both sides of such interfaces) and satisfying outgoing wave conditions, it will be an eigenfunction for the problem. The convergence of the Finite Element algorithm depends crucially upon the regularity of the boundaries between complementary media with some ill-posedness occuring in certain corner cases for a refractive index contrast of −1 when the coercive plus compact mathematical framework breaks down. (see A.S. Bonnet-Ben Dhia, P. Ciarlet Jr., C.M. Zwolf, J. Comp. Appl. Math., in press).
14. Pendry · J. Mod. Opt. · 1994 · 41 · 20910.1080/09500349414550281 ↗
15. Chakrabarti · Opt. Exp. · 2006 · 14 · 1295010.1364/OE.14.012950 ↗
16. Berenger · J. Comp. Phys. · 1994 · 114 · 18510.1006/jcph.1994.1159 ↗
17. Mc Isaac · IEEE Trans. Microwave Theory Tech. · 1975 · 23 · 42910.1109/TMTT.1975.1128585 ↗
18. Yablonovitch · Phys. Rev. Lett. · 1987 · 58 · 205910.1103/PhysRevLett.58.2059 ↗
19. Gralak · J. Opt. Soc. Am. A · 2000 · 17 · 101210.1364/JOSAA.17.001012 ↗
20. Luo · Phys. Rev. B · 2002 · 65 · 20110410.1103/PhysRevB.65.201104 ↗
21. Luo · Phys. Rev. B · 2003 · 68 · 04511510.1103/PhysRevB.68.045115 ↗
22. Cubukcu · Nature · 2003 · 423 · 60410.1038/423604b ↗
23. Tayeb · J. Opt. Soc. A · 1997 · 14 · 332310.1364/JOSAA.14.003323 ↗
24. Milton · Proc. Roy. Lond. A · 2006 · 462 · 302710.1098/rspa.2006.1715 ↗
25. Notomi · Opt. Quant Elec. · 2002 · 34 · 13310.1023/A:1013300825612 ↗
26. Monzon · Phys. Rev. E · 2005 · 72 · 05660610.1103/PhysRevE.72.056606 ↗