Discontinuity induced angular distribution of photon plasmon coupling.

Metal-dielectric transitions are important structures that can display a host of optical characteristics including excitation of plasmons. Metal-dielectric discontinuities can furthermore support plasmon excitation without a severe condition on the incident angle of the exciting photons. Using a semi-infinite thin gold film, we study surface plasmon (SP) excitation and the associated electromagnetic near-field distribution by recording the resulting plasmon interference patterns. In particular, we measure interference periods involving SPs at the scanable metal/air interface and the buried metal/glass one. Supported by optical near-field simulations and experiments, we demonstrate that the metal/glass surface plasmon is observable over a wide range of incident angles encompassing values above and below the critical incident angle. As a result, it is shown that scanning near-field microscopy can provide quantitative evaluation of the real part of the buried surface plasmon wavevector.

[1]  R. H. Ritchie Plasma Losses by Fast Electrons in Thin Films , 1957 .

[2]  E. Kretschmann,et al.  Notizen: Radiative Decay of Non Radiative Surface Plasmons Excited by Light , 1968 .

[3]  A. Otto Excitation of nonradiative surface plasma waves in silver by the method of frustrated total reflection , 1968 .

[4]  R. W. Christy,et al.  Optical Constants of the Noble Metals , 1972 .

[5]  Adam,et al.  Determination of the spatial extension of the surface-plasmon evanescent field of a silver film with a photon scanning tunneling microscope. , 1993, Physical review. B, Condensed matter.

[6]  Bernhard Lamprecht,et al.  Near-field observation of surface plasmon polariton propagation on thin metal stripes , 2001 .

[7]  Evgeny Popov,et al.  Light Propagation in Periodic Media , 2002 .

[8]  Anatoly V. Zayats,et al.  Local excitation of surface plasmon polaritons at discontinuities of a metal film: Theoretical analysis and optical near-field measurements , 2002 .

[9]  Jean-Claude Weeber,et al.  Launching and decoupling surface plasmons via micro-gratings , 2003 .

[10]  A. Zayats,et al.  Analysis of the Bloch mode spectra of surface polaritonic crystals in the weak and strong coupling regimes: grating-enhanced transmission at oblique incidence and suppression of SPP radiative losses. , 2004, Optics express.

[11]  Fadi Issam Baida,et al.  Coupling between surface plasmon modes on metal films , 2004 .

[12]  J. P. Goudonnet,et al.  Optical modulation processes in thin films based on thermal effects of surface plasmons , 2005 .

[13]  A. Maradudin,et al.  Nano-optics of surface plasmon polaritons , 2005 .

[14]  Thomas Thundat,et al.  Imaging standing surface plasmons by photon tunneling , 2005 .

[15]  Olivier J. F. Martin,et al.  Transient behavior of surface plasmon polaritons scattered at a subwavelength groove , 2007, 0704.0703.

[16]  P Lalanne,et al.  Near-field analysis of surface waves launched at nanoslit apertures. , 2007, Physical review letters.

[17]  Jan Renger,et al.  Direct excitation of surface plasmon polaritons in nanopatterned metal surfaces and thin films , 2007 .

[18]  Sergey I. Bozhevolnyi,et al.  Efficiency of local surface plasmon polariton excitation on ridges , 2008, SPIE Photonics Europe.

[19]  Philippe Lalanne,et al.  Efficient generation of surface plasmon by single-nanoslit illumination under highly oblique incidence , 2009 .