2015
DOI: 10.1103/physrevb.92.085411
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Real-space imaging of nanotip plasmons using electron energy loss spectroscopy

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Cited by 45 publications
(58 citation statements)
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“…The EFTEM images of the taper region are readily understood by assuming that the electron beam indeed couples mostly to the m = 0 monopole mode of the taper. Recent EELS measurements and simulations [86,89,91] confirm the broadband, non-resonant character of the field enhancement at the taper apex. The observation of oscillations in the spectra recorded at larger distances from the apex was interpreted as a characteristic signature of the excitation of higher order angular momentum modes [86].…”
Section: Plasmonic Eigenmodes Of Circular Wires and Tapersmentioning
confidence: 89%
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“…The EFTEM images of the taper region are readily understood by assuming that the electron beam indeed couples mostly to the m = 0 monopole mode of the taper. Recent EELS measurements and simulations [86,89,91] confirm the broadband, non-resonant character of the field enhancement at the taper apex. The observation of oscillations in the spectra recorded at larger distances from the apex was interpreted as a characteristic signature of the excitation of higher order angular momentum modes [86].…”
Section: Plasmonic Eigenmodes Of Circular Wires and Tapersmentioning
confidence: 89%
“…The observation of oscillations in the spectra recorded at larger distances from the apex was interpreted as a characteristic signature of the excitation of higher order angular momentum modes [86]. The formation of standing waves due to the back reflection of SPP modes near the apex may also give rise to spectral oscillations for certain taper geometries, as evidenced in [89,91].…”
Section: Plasmonic Eigenmodes Of Circular Wires and Tapersmentioning
confidence: 95%
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“…For comparison with theory, we performed numerical calculations of the CL signal based on the DGTD method [26]. To this end, we used the framework that has been developed in the past for the simulation of EELS experiments [27,31]. The system composed of the gold disk, the TEM substrate and the surrounding air was discretized in a tetrahedral mesh with element size between 80 nm in air away from the ND, 10 nm close to the ND and 5 nm inside the ND itself using a third-order Lagrange polynomial basis and evolved in time using a fourth-order low-storage Runge-Kutta integrator.…”
Section: Numerical Calculationsmentioning
confidence: 99%
“…Recent technological developments, including the application of THz transients [16,33], shaken pulse-pair excitation (SPPX) [50,51], two-color SPPX [52,53], two-pulse picking [22,23] and cross-polarized double beat methods [54,55] have led to a reliable laser coupling to STM. Further near-field schemes, such as plasmonic nanofocusing, have the potential to further enhance the coupling to the tunneling gap [56][57][58][59][60].…”
Section: Introductionmentioning
confidence: 99%