Application of confocal surface wave microscope to self-calibrated attenuation coefficient measurement by Goos-Hänchen phase shift modulation

In this paper, we present a direct method to measure surface wave attenuation arising from both ohmic and coupling losses using our recently developed phase spatial light modulator (phase-SLM) based confocal surface plasmon microscope. The measurement is carried out in the far-field using a phase-SLM to impose an artificial surface wave phase profile in the back focal plane (BFP) of a microscope objective. In other words, we effectively provide an artificially engineered backward surface wave by modulating the Goos Hänchen (GH) phase shift of the surface wave. Such waves with opposing phase and group velocities are well known in acoustics and electromagnetic metamaterials but usually require structured or layered surfaces, here the effective wave is produced externally in the microscope illumination path. Key features of the technique developed here are that it (i) is self-calibrating and (ii) can distinguish between attenuation arising from ohmic loss (k″Ω) and coupling (reradiation) loss (k″c). This latter feature has not been achieved with existing methods. In addition to providing a unique measurement the measurement occurs of over a localized region of a few microns. The results were then validated against the surface plasmons (SP) dip measurement in the BFP and a theoretical model based on a simplified Green’s function.

[1]  J. Sambles,et al.  A study of the thin metal film/fluid interface using surface plasmon-polaritons , 1987 .

[2]  Pierre Berini,et al.  Surface plasmon–polariton amplifiers and lasers , 2011, Nature Photonics.

[3]  D. Norris,et al.  Plasmonic Films Can Easily Be Better: Rules and Recipes , 2015, ACS photonics.

[4]  D. Ansell,et al.  Hybrid graphene plasmonic waveguide modulators , 2015, Nature communications.

[5]  Lorenzo Marrucci,et al.  Spin–orbit photonics , 2015, Nature Photonics.

[6]  SPR Biosensors for Environmental Monitoring , 2006 .

[7]  M. Majewski,et al.  Optical properties of metallic films for vertical-cavity optoelectronic devices. , 1998, Applied optics.

[8]  Direct measurement of the Goos-Hänchen shift using a scanning quadrant detector and a polarization maintaining fiber. , 2016, The Review of scientific instruments.

[9]  S. Seshadri Attenuated total reflection method of excitation of the surface polariton in the Kretschmann configuration , 1991 .

[10]  H. Lezec,et al.  Loss mechanisms of surface plasmon polaritons on gold probed by cathodoluminescence imaging spectroscopy , 2008 .

[11]  M. Somekh,et al.  Surface plasmon microscopy: resolution, sensitivity and crosstalk , 2012, Journal of microscopy.

[12]  Tian Jiang,et al.  Backward spoof surface wave in plasmonic metamaterial of ultrathin metallic structure , 2016, Scientific Reports.

[13]  Surface roughness of thin gold films and its effects on the proton energy loss straggling , 2006 .

[14]  E. Palik Handbook of Optical Constants of Solids , 1997 .

[15]  Goos–Hänchen and Imbert–Fedorov beam shifts: an overview , 2012, 1210.8236.

[16]  Nico F. Declercq,et al.  Backward displacement of ultrasonic waves reflected from a periodically corrugated interface , 2005 .

[17]  G. Agarwal,et al.  Observation of giant Goos-Hänchen and angular shifts at designed metasurfaces , 2016, Scientific Reports.

[18]  M. Somekh,et al.  Quantitative plasmonic measurements using embedded phase stepping confocal interferometry. , 2013, Optics express.

[19]  Mohd Syuhaimi Ab Rahman,et al.  Analysis of TE (Transverse Electric) modes of symmetric slab waveguide , 2012 .

[20]  D. Lynch,et al.  Handbook of Optical Constants of Solids , 1985 .

[21]  Michael G. Somekh,et al.  Ultrastable embedded surface plasmon confocal interferometry , 2014 .

[22]  N. Chubachi,et al.  Attenuation measurements of leaky waves by the acoustic line-focus beam , 1983 .

[23]  A. Bogdanov,et al.  Photonic surface waves on metamaterial interfaces , 2017, Journal of physics. Condensed matter : an Institute of Physics journal.

[24]  Harald Giessen,et al.  Chiral plasmonics , 2017, Science Advances.

[25]  Critical coupling layer thickness for positive or negative Goos–Hänchen shifts near the excitation of backward surface polaritons in Otto-ATR systems , 2015, 1503.03330.

[26]  P. Mahadevan,et al.  An overview , 2007, Journal of Biosciences.

[27]  M. Somekh,et al.  Surface plasmon microscopic sensing with beam profile modulation. , 2012, Optics express.

[28]  L. Torner,et al.  Lossless directional guiding of light in dielectric nanosheets using Dyakonov surface waves. , 2014, Nature nanotechnology.

[29]  D. Miller,et al.  Transmission Line and Equivalent Circuit Models for Plasmonic Waveguide Components , 2008, IEEE Journal of Selected Topics in Quantum Electronics.

[30]  L. Douillard,et al.  Loss mechanisms of surface plasmon polaritons propagating on a smooth polycrystalline Cu surface. , 2012, Optics express.

[31]  Suejit Pechprasarn,et al.  Detection limits of confocal surface plasmon microscopy. , 2014, Biomedical optics express.

[32]  M. Somekh,et al.  Direct far-field observation of surface-plasmon propagation by photoinduced scattering , 1999 .

[33]  P. Lytvyn,et al.  Au Gratings Fabricated by Interference Lithography for Experimental Study of Localized and Propagating Surface Plasmons , 2017, Nanoscale Research Letters.

[34]  Takashi Wakamatsu,et al.  Interpretation of attenuated-total-reflection dips observed in surface plasmon resonance , 2007 .

[35]  H. Li,et al.  Refractive index of alkali halides and its wavelength and temperature derivatives , 1976 .

[36]  Abdullah Atalar,et al.  A physical model for acoustic signatures , 1979 .

[37]  J. Goudonnet,et al.  Surface plasmon polariton propagation length: A direct comparison using photon scanning tunneling microscopy and attenuated total reflection , 2001 .

[38]  R. Gajić,et al.  Enhanced phase sensitivity of metamaterial absorbers near the point of darkness , 2014 .

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

[40]  Andrei Kolomenski,et al.  Propagation length of surface plasmons in a metal film with roughness. , 2009, Applied optics.

[41]  Jing Zhang,et al.  Surface-plasmon microscopy with a two-piece solid immersion lens: bright and dark fields. , 2006, Applied optics.

[42]  Shun Lien Chuang,et al.  Lateral shift of an optical beam due to leaky surface-plasmon excitations , 1986 .

[43]  A. Maradudin Introduction: Plasmonics and its building blocks , 2014 .