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Surface plasmon theory and applications...

Ross McPhedran, Nicolae-Alexandru Nicorovici, Christian Karnutsch

Light interacting with systems containing metallic elements can create surface plasmons and therefore strong local fields, enhanced non-linear effects and surprising transmission through small holes. In a project to commence in 2006 we will investigate the basic physics of plasmons in structured metallic systems. Metals give high contrast in optical elements, permitting nano-scale structures to interact strongly with light, and we will provide accurate design rules to control light absorption within them. Our aim is to investigate a range of applications of surface plasmons in linear and non-linear photonic systems.

Plasmonics and cloaking

Graeme Milton (University of Utah), Ross McPhedran (University of Sydney), Nicolae-Alexandru Nicorovici (University of Technology Sydney and University of Sydney)

The making of an object invisible through some cloaking device is commonly regarded as science fiction. However, we have discovered a new phenomenon in electromagnetism which translates into a new mechanism for invisibility or cloaking.

Specifically, regions of anomalous localized resonance, such as occur near superlenses, are shown to lead to cloaking effects. This occurs when the resonant field generated by a polarizable line or point dipole acts back on the polarizable line or point dipole and effectively cancels the field acting on it from outside sources, so it has essentially no response to the external field. Numerically and analytically we see that the polarizable line or point dipole is effectively invisible to the external time harmonic field. Cloaking is proved in the quasistatic limit for finite collections of polarizable line dipoles that all lie within a specific distance from a coated cylinder having a shell dielectric constant close to -1 and a matrix and core dielectric constant equal to 1. Cloaking is also shown to extend to the Veselago superlens outside the quasistatic regime: a polarizable line dipole located less than a distance d/2 from the lens, where d is lens thickness, will be cloaked due to the presence of a resonant field in front of the lens. Also a polarizable point dipole near a slab lens will be cloaked in the quasistatic limit. The hope of using cloaking to see the interior of an object by making half of it invisible remains an intriguing possibility.

Images for cloaking by reaction: Click on the image above to link to the quicktime movie.

Presentation and slides on cloaking

  • Presentation by Graeme W. Milton, "Cloaking: A new phenomenon in Electromagnetism," ETOPIM 7, 2006.
  • Presentation by Ross McPhedran, "From Homeopathy to Cloaking by Plasmonic Resonance," School of Physics Colloquium, University of Sydney, 2006.
  • The following animation (.exe file - [ESC] to stop) shows a coated cylinder with core and shell dielectic constants of 1 and -1+i*10-7, and core and shell radii of 2 and 4 respectively, placed in a uniform electric field. A polarizable molecule moves from the right. The dashed line marks the circle where the cloaking phenomenon occurs. The polarizable molecule has a strong induced dipole moment and perturbs the field around the coated cylinder strongly. It then enters the cloaking region, and it and the coated cylinder do not perturb the external field.

Presentations and slides on plasmonics

Some media releases

  1. The Guardian, "Now you see it, now you don't: cloaking device is not just sci-fi", 3 May 2006.
  2. Daily Telegraph, 3 May 2006
  3. BBC NEWS. Published: 2006/05/03 16:34:49 GMT
  4. Science News, "Out of Sight", 15 July 2006
  5. Science, "Waves on the Horizon", Vol. 313, No. 5792, pg 1399-1400, 8 September 2006
  6. CNN, "Scientists set sights on invisibility cloaks", 1 July 2008

References

  1. Field L, Nicorovici NA, McPhedran RC
    Optical resonances of cylinder and sphere clusters in the quasistatic limit
    PHYSICA B-CONDENSED MATTER 394 (2): 193-196 MAY 15 2007
  2. Movchan NV, Guenneau S, Movchan AB and R.C. McPhedran
    Estimates for localised transverse electric modes in multi-structured
    crystal fibres
    PHYSICA B-CONDENSED MATTER 394 (2): 281-284 MAY 15 2007
  3. Botten LC, Asatryan AA, Nicorovici NA, R.C. McPhedran and C. Martijn de Sterke
    Generalisation of the transfer matrix formulation of the theory of electron and photon conductance
    PHYSICA B-CONDENSED MATTER 394 (2): 320-324 MAY 15 2007
  4. N. A. Nicorovici, G. W. Milton, R. C. McPhedran, and L. C. Botten
    Quasistatic cloaking of two-dimensional polarizable discrete systems by anomalous resonance
    Optics Epxress, 15(10) pp 6314-6323 (2007).
  5. N.A. Nicorovici, G.W. Milton, R.C. McPhedran, and L.C. Botten
    Cloaking of Polarizable Discrete Systems by Anomalous Resonance
    Supporting online material
  6. B. T. Kuhlmey, K. Pathmanandavel and R. C. McPhedran,
    Multipole analysis of Photonic Crystal Fibers with coated inclusions,
    Optics Express 14 (22) pp.10851-10864 (2006)
  7. G. W. Milton, N.-A. P. Nicorovici and R. C. McPhedran
    Opaque perfect lenses
    arXiv.org.
  8. N. A. Nicorovici, R. C. McPhedran, G. W. Milton and L. C. Botten
    Partial Resonances of Three-Phase Composites at Long Wavelengths
    arXiv.org.
  9. G.W. Milton and N.A. Nicorovici
    On the cloaking effects associated with anomalous localized resonance,
    Proc. R. Soc. Lond. A 462, 3027-3059 (2006).
  10. G. W. Milton, N. A. Nicorovici, R. C. McPhedran and V. A. Podolskiy
    A proof of superlensing in the quasistatic regime, and limitations of superlenses in this regime due to anomalous localized resonance
    Proc. R. Soc. Lond. A 461, 3999-4034 (2005).
  11. N. A. Nicorovici, D. R. McKenzie and R. C. McPhedran
    Optical Resonances of Three-Phase Composites and Anomalies in Transmission
    Opt. Comm. 117, 151-169 (1995).
  12. N. A. Nicorovici, R. C. McPhedran and G. W. Milton
    Optical and Dielectric Properties of Partially Resonant Composites
    Phys. Rev. B 49, 8479-8482 (1994).
  13. N.A. Nicorovici, R. C. McPhedran and G. W. Milton
    Transport Properties of a Three--Phase Composite Material: The Square Array of Coated Cylinders
    Proc. R. Soc. Lond. A 442, 599-620 (1993).


 

 

 

 

 

 
 

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