2018
DOI: 10.29026/oea.2018.180010
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Mode evolution and nanofocusing of grating-coupled surface plasmon polaritons on metallic tip

Abstract: We present a detailed analysis on mode evolution of grating-coupled surface plasmonic polaritons (SPPs) on a conical metal tip based on the guided-wave theory. The eigenvalue equations for SPPs modes are discussed, revealing that cylindrical metal waveguides only support TM 01 and HE m1 surface modes. During propagation on the metal tip, the grating-coupled SPPs are converted to HE 31 , HE 21 , HE 11 and TM 01 successively, and these modes are sequentially cut off except TM 01 . The TM 01 mode further propagat… Show more

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Cited by 38 publications
(25 citation statements)
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References 49 publications
(47 reference statements)
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“…Metallic nanostructures represent an interesting approach to bridge the gap between conventional and modern optics. Such nanostructures stimulate the oscillation of free electrons on the surface, so-called surface plasmons [5][6][7][8][9][10][11][18][19][20][21][22][23][26][27][28][29][30][31][32] that lead to strong near-field enhancements known as hot-spots that boost both linear and nonlinear characteristics 9,[33][34][35][36][37][38] . Indeed, employing surface plasmons arising at metal-dielectric boundaries allows enhancing nonlinear interactions, because electrons at the surface reside in a non-symmetric environment, where the nonlinearities arise from the asymmetry of the potential confining the electrons at the surface 2,3 .…”
Section: Metallic Nanoantennasmentioning
confidence: 99%
“…Metallic nanostructures represent an interesting approach to bridge the gap between conventional and modern optics. Such nanostructures stimulate the oscillation of free electrons on the surface, so-called surface plasmons [5][6][7][8][9][10][11][18][19][20][21][22][23][26][27][28][29][30][31][32] that lead to strong near-field enhancements known as hot-spots that boost both linear and nonlinear characteristics 9,[33][34][35][36][37][38] . Indeed, employing surface plasmons arising at metal-dielectric boundaries allows enhancing nonlinear interactions, because electrons at the surface reside in a non-symmetric environment, where the nonlinearities arise from the asymmetry of the potential confining the electrons at the surface 2,3 .…”
Section: Metallic Nanoantennasmentioning
confidence: 99%
“…Generally, the grating period for SPP excitation should satisfy the phase-matching condition k sp = k 0 cos(α/2) ± n2π/p [38][39][40][41], where k sp is the wave vector of the SPPs (actually, k sp is dependent on the crosssectional radius of the bare tip, but here, we regard k sp as a constant at different positions due to the small change range of k sp in the grating region [38]), k 0 is the wave vector of the incident light, n is a positive integer (n = 1, 2, 3…) and ± represents the SPPs propagating upward and downward. Note that only the downward SPPs could contribute to the electric field enhancement at the tip apex.…”
Section: Spectral Responses Of Ef For Grating Parametersmentioning
confidence: 99%
“…Recently, the nanoimprinting or grating-coupled process to fabricate a periodic 1-D grating structure at the electrode has been demonstrated using BD-R to enhance the electric field in photoelectric conversion systems 24 . The grating-coupled technique is a prism-less, convenient, propagating SPR excitation method [25][26][27] . In the absence of SP excitation, light scattering and light trapping can occur on the grating-structured surface, improving the obtained photocurrent 28,29 .…”
Section: Introductionmentioning
confidence: 99%