1 / 19

Gothic Cathedrals and Solar Cells (and maybe a Grail?)

Gothic Cathedrals and Solar Cells (and maybe a Grail?). A short introduction to the phenomenon of Surface Plasmons and their role in the scattering of light. Martin Kirkengen, Fysisik Institutt, Universitetet i Oslo. Electromagnetic wave in homogeneous medium.

natane
Download Presentation

Gothic Cathedrals and Solar Cells (and maybe a Grail?)

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Gothic Cathedrals and Solar Cells (and maybe a Grail?) A short introduction to the phenomenon of Surface Plasmonsand their role in the scattering of light Martin Kirkengen, Fysisik Institutt, Universitetet i Oslo

  2. Electromagnetic wave in homogeneous medium • Maxwell equations, wave solution: • Wave with frequency w and wavenumber k

  3. z Ez x Ex H 2 y 1 Stationary solution at boundary: • Flat boundary at z=0 • Wave propagating in one direction only (no reflection) • Ey = 0

  4. Plane wave at boundary (at z=0)(no reflection) • Fields • Boundary conditions: z Ez H x Ex H 2 y 1

  5. Solution at boundary Maxwell equations give (Raether 1988) And unless e1=e2 Plasmon solution for e2 =1, e1<-1, imaginary kz

  6. What? e < 0?! Lorentz model – electron on spring: Polarizability and dielectric constant: Drude model – cut the spring:

  7. e<0 , imaginary k, what about c? • Wavenumber: • Imaginary e -> absorption • Real e, imaginary N-> no penetration, no absorption

  8. Back to the Surface Plasmons... • Visible light, metal/air interface • Real wave number along x • Imaginary wave number along y • Longitudinal charge fluctuations at surface • Evanescent waves – no propagated power z 1 2 x _ _ _ _ _ _ +++ +++

  9. Some Plasmon Geometries • Multiple interfaces give new possibilities • More stable modes(up to 1 cm propagation)

  10. Coupling to light • Plasmon: • Light: • Momentum mismatch – requires help- Grating (discreet, periodic)- Roughness (periodic Fourier components)- Periodic due to curved surface - spheres

  11. The Cathedral Bit... Red color due to embedded gold particles spreading light

  12. An early application: • The Lycurgus Cup (British museum 400 A.D.) • When illuminated from within, it glows red. Again due to gold particles embedded in the glass, with an absorption peak at around 520 nm Illustrations stolen from: David G. Stroud, Ohio State University Columbus OH

  13. Light scattering from spheresMie Theory • Solve Wave equations in spherical coordinates • Expand a plane wave in spherical harmonics • Determine coefficients for the scattered wave and for the internal field of the sphere • Try to extract some physical meaning... Bohren&Huffman, Absorption &Scattering of Light by Small Particles (Wiley 1983)

  14. Jumping to the Coefficients... • m=N1/Nair • Resonance (in the limit of small x) at • Lowest mode for metal particle in air (Nair=1): N12 = m2 = -2, e = -2

  15. Ag Bound electrons(Lorentz model) Free Electrons(Drude model) Frequency Dependence of Resonance Extinction (absorption+scattering) for gold particles in fluid e as function of frequency for silver Elghanian et al, Science 277, 1078 (1997) Storhoff et al, JACS 120, 1959 (1998)Park and Stroud, PRB 68, 224201 (2003)] Kreibig and Vollmer , Optical Properties of Metal Clusters , Springer-Verlag:Berlin, 1995

  16. The Scattered Field q-components of the scattered field Destructive interference with incoming wave r=0.01l r=0.2l r=l Constructive interference with incoming wave Smallest particles – dipole field Larger particles – multipole contributions

  17. Changing the resonance • SizeLarger particles, higher modes contribute, each mode red-shifted • ShapeElliptic shape, flatter particles have red-shifted resonance • Coating/substrateResonance is given as a relative refraction index, changing surroundings changes resonance • Arrays/clustersLoads of opportunities...

  18. Applications in biophysics • Gold Nanoparticles as markers • Shift in resonance gives dielectric constant of medium Forschungszentrum Jülich

  19. Applications in Solar Cells • Placing small particles of a reflective medium at surface reduces reflection... • Strong coupling between plasmons and waveguides – increased fields in the active part of the solar cell. • The reverse process (LED) has been shown to gain a factor 8 from plasmon coupling • No Solar Cell demonstrated – yet... Catchpole & Pillai School of Photovoltaic and Renewable Energy Engeneering UNSW, Australia JoAP 100, 044504 (2006)

More Related