2013
DOI: 10.1007/s11468-013-9554-6
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Imaging and Characterizing Long-Range Surface Plasmon Polaritons Propagating in a Submillimeter Scale by Two-Color Two-Photon Photoelectron Emission Microscopy

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Cited by 22 publications
(21 citation statements)
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“…In the past decade, metal plasmonic nanostructures have attracted a great deal of attention because of their large field enhancement and small module volume. In addition, metal plasmon nanoparticles made of different materials with various shapes [1,2] and different surface structures have been used to couple the electromagnetic energy with molecules to enhance fluorescence [3][4][5] and surface-enhanced Raman scattering (SERS) [6,7]. However, in practical applications, intrinsic absorption, external heating, and other factors inevitably impact the metals [8].…”
Section: Introductionmentioning
confidence: 99%
“…In the past decade, metal plasmonic nanostructures have attracted a great deal of attention because of their large field enhancement and small module volume. In addition, metal plasmon nanoparticles made of different materials with various shapes [1,2] and different surface structures have been used to couple the electromagnetic energy with molecules to enhance fluorescence [3][4][5] and surface-enhanced Raman scattering (SERS) [6,7]. However, in practical applications, intrinsic absorption, external heating, and other factors inevitably impact the metals [8].…”
Section: Introductionmentioning
confidence: 99%
“…Most PEEM studies focused so far on surface plasmon polaritons (SPP) supported by metaldielectric interfaces. Topics included SPP phase and group propagation [4][5][6][7], SPP dispersion [8,9], plasmonic focusing [10,11] and switching [12], plasmonic waveguiding [13,14], and the formation of plasmonic vortices [15].…”
Section: Introductionmentioning
confidence: 99%
“…18−36 In terms of SPP imaging, time and lateral resolution as well as quick imaging are advantages of the 2P-PEEM that allow it to stand out from other approaches. What is more, methodological developments (e.g., alkali atom deposition for lowering workfunc-tions, 22,23,25,26,33 detection of multiphoton photoemission, 28,30,32,35 normally incident configurations of light sources, 27,29,30,33,36 and dual-color 2P-PEEM) 24,34 make 2P-PEEM even more versatile. However, despite the fascinating advantages of 2P-PEEM, target samples whose SPPs can be visualized are limited to naked metal surfaces or ultrathin (a few nm) dielectric film/metal interfaces, since 2P-photoemission is highly suppressed for thick dielectric surfaces.…”
mentioning
confidence: 99%
“…The principles of SPP imaging with NIR/UV dual-color 2P-PEEM have been described elsewhere. 24,34 Briefly, NIR (ℏω NIR = ℏc/k 0 , where c is the speed of light, and k 0 is the wavevector) excites SPPs at the intrinsic defect of the Au(111) ) and the dielectric function (ε Au = (n + ik) 2 , where n and k are the refractive index and extinction coefficient of Au, respectively; n = 0.165 and k = 5.401 at ℏω NIR = 1.44 eV), 24,37 the simulated k SPP value, 7.43 × 10 6 m −1 , which gives λ beat = 7.74 μm (= 2π/ k beat ), is used for lateral scaling of the 2P-PEEM images. Note that SPPs generally propagate in both forward and backward (±k SPP ) directions, and the backward propagating SPPs would show much narrower beats of λ beat = 0.45 μm on the opposite side, 22,38 although this is less focused on in this report.…”
mentioning
confidence: 99%
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