2017
DOI: 10.1021/acs.nanolett.7b02252
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Nonlinear Raman Effects Enhanced by Surface Plasmon Excitation in Planar Refractory Nanoantennas

Abstract: We consider a nonlinear mechanism of localized light inelastic scattering within nanopatterned plasmonic and Raman-active titanium nitride (TiN) thin films exposed to continuous-wave (cw) modest-power laser light. Owing to the strong third-order nonlinear interaction between optically excited broadband surface plasmons and localized Stokes and anti-Stokes waves, both stimulated and inverse Raman effects can be observed. We provide experimental evidence for coherent amplification of the localized Raman signals … Show more

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Cited by 28 publications
(28 citation statements)
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“…It is much more cost-effective, mechanically and thermally robust, and, importantly, compatible with the CMOS technology despite worse optical properties. Successful implementation of the titanium nitride as a plasmonic component in photonic devices has been demonstrated on the example of hyperbolic metamaterials working in the visible and infrared ranges [9,10], high-temperature-stable and irradiation-resistant broadband absorber [11], nanoantennas, or other nanostructures able to increase optical response [12][13][14][15][16][17], SERS (Surface-Enhanced Raman Spectroscopy spectroscopy) substrate [18], and remote optical temperature sensor [19]. Apart from applications, the current literature addresses issues related to optimizing the plasmonic properties [20][21][22][23][24][25][26] and the stability of the thin films [26][27][28].…”
Section: Introductionmentioning
confidence: 99%
“…It is much more cost-effective, mechanically and thermally robust, and, importantly, compatible with the CMOS technology despite worse optical properties. Successful implementation of the titanium nitride as a plasmonic component in photonic devices has been demonstrated on the example of hyperbolic metamaterials working in the visible and infrared ranges [9,10], high-temperature-stable and irradiation-resistant broadband absorber [11], nanoantennas, or other nanostructures able to increase optical response [12][13][14][15][16][17], SERS (Surface-Enhanced Raman Spectroscopy spectroscopy) substrate [18], and remote optical temperature sensor [19]. Apart from applications, the current literature addresses issues related to optimizing the plasmonic properties [20][21][22][23][24][25][26] and the stability of the thin films [26][27][28].…”
Section: Introductionmentioning
confidence: 99%
“…Near-field concepts can be exploited for IR nanoscale studies with various kinds of measurement geometries. [37][38][39][40][41][42][43][44][45][46][47] The availability of brilliant IR radiation sources enabled new breakthroughs in IR instrumentation towards modern near-field microscopy. In addition, laser laboratory sources such as pulsed optical parametric oscillators (OPO) and pulsed laser sources, in particular tunable free-electron lasers (FEL), 57,65,66 were important to push the development.…”
Section: Introductionmentioning
confidence: 99%
“…14,16,22 For the analysis of such anisotropic material properties on the nanoscale, powerful characterization methods such as polarization-dependent techniques have to be selected and further developed. 15,18,19,21,22,25,26,3543 Infrared (IR) methods are in particular attractive as material and structural properties can be determined with high sensitivity and spectral contrast in a label-free manner. 35,44 Infrared spectroscopy is complementary to other surface science techniques and has the advantage that it is compatible with a wide range of environmental conditions.…”
Section: Introductionmentioning
confidence: 99%
“…For a 632.8 nm laser, the wavelengths of SPPs excited at the Au-air (𝜆 SPP Au-air ) and Au-SiO 2 interfaces (𝜆 SPP Au-SiO2 ) are derived to be 603 and 388 nm, respectively. [13,28] SPP Au-air and SPP Au-SiO2 (i.e., SPP PM-air and SPP PM-D -1) can interfere predominantly within the hexagonal air and SiO 2 wall cavities besieged by Au sidewalls via Fabry-Pérot (FP) resonance-like multiple reflections, respectively, as illustrated in Figure 1a; and Figure S1 of the Supporting Information. When the Au layer is thin (say, several nanometers only 20 ) enough, both SPP Au-air and SPP Au-SiO2 waves could transmit the Au layer into the SiO 2 and air cavities to be reflected by the opposite Au sidewalls, respectively, as shown in Figure 1.…”
Section: Resultsmentioning
confidence: 99%