2015
DOI: 10.7567/apex.8.126601
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Mapping the plasmon response of Ag nanoislands on graphite at 100 nm resolution with scanning probe energy loss spectroscopy

Abstract: We demonstrate plasmon mapping of Ag nanostructures on graphite using scanning probe energy loss spectroscopy (SPELS) with a spatial resolution of 100 nm. In SPELS, an STM tip is used as a localized source of field-emitted electrons to probe the sample surface. The energy loss spectrum of the backscattered electrons is measured to provide a chemical signature of the surface under the tip. We acquire three images simultaneously with SPELS: i) constant-current field-emission images, which provide topographical i… Show more

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Cited by 8 publications
(9 citation statements)
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“…In this technique, the tip of a scanning tunnel microscope is operated in the field emission mode to generate a local electron beam, which can be scattered from the surface and collected by an electron energy analyzer. Therefore, the two dimensional distribution of the electron energy spectra of the surface can be scanned 2 , 5 , 7 , 8 , which is important information for fully understanding the surface at microscale. However, the probability of the inelastic scattering of electron is usually very small, often orders of magnitude smaller than that of the elastically scattered electron.…”
Section: Introductionmentioning
confidence: 99%
“…In this technique, the tip of a scanning tunnel microscope is operated in the field emission mode to generate a local electron beam, which can be scattered from the surface and collected by an electron energy analyzer. Therefore, the two dimensional distribution of the electron energy spectra of the surface can be scanned 2 , 5 , 7 , 8 , which is important information for fully understanding the surface at microscale. However, the probability of the inelastic scattering of electron is usually very small, often orders of magnitude smaller than that of the elastically scattered electron.…”
Section: Introductionmentioning
confidence: 99%
“…Another noteworthy point is that the Ag nanostructures yield a lower backscattered electron signal than the surrounding HOPG substrate. We have recently reported on this effect in [32], which is counterintuitive as one would expect a larger electron backscattering cross-section for the element with the higher atomic number. Moreover, since the RFA was configured to suppress the secondary electron signal in these measurements, it is unlikely that variations in the work function of the surface are causing the material contrast.…”
Section: Electron Reflectivitymentioning
confidence: 77%
“…The pre-amplifier near the scan head of the STM-1 was removed and replaced by an amplifier (Femto DLPCA-200) outside the vacuum chamber to allow measurements at higher currents in FE mode using a picoammeter. This instrument has been previously used in combination with a cylindrical sector analyzer with multichannel detector to map the plasmon response of Ag nanoislands on HOPG with SPELS [32]. For the experiments described here, the analyzer has been replaced with a RFA described below.…”
Section: Spels Instrumentmentioning
confidence: 99%
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“…The film was deposited at room temperature and annealed at 700 • C for 30 min in vacuum. SPELS measurements were performed using a modified STM setup that is described elsewhere [3,4]. In SPELS, the STM tip is biased at voltages up to -400 V with respect to the sample.…”
Section: Methodsmentioning
confidence: 99%