2015
DOI: 10.1063/1.4937442
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Raman spectroscopy and electrical properties of InAs nanowires with local oxidation enabled by substrate micro-trenches and laser irradiation

Abstract: The thermal gradient along indium-arsenide nanowires was engineered by a combination of fabricated micro-trenches in the supporting substrate and focused laser irradiation. This allowed local control of thermally activated oxidation reactions of the nanowire on the scale of the diffraction limit. The locality of the oxidation was detected by microRaman mapping, and the results were found consistent with numerical simulations of the temperature profile. Applying the technique to nanowires in electrical devices … Show more

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Cited by 5 publications
(7 citation statements)
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“…The oxidation reaction accelerates with increased temperature, and we attribute the appearance of the arsenic spectra as the result of laser induced heating [30,31], possibly combined with photo-oxidation [28]. The activation of the oxidation reaction can be followed by the power dependence of the relative intensities of the fitted arsenic and InAs Raman peaks presented in figure 1(d) measured, using 520.8 nm laser excitation and 15 min integration time per spectrum, of a NW suspended over a 150 nm deep and 2 μm wide trench [21]. Initially, at the lowest powers, the arsenic peaks are absent, but then irreversibly appear after applying illuminating powers above 120 kW cm −2 .…”
Section: Resultsmentioning
confidence: 99%
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“…The oxidation reaction accelerates with increased temperature, and we attribute the appearance of the arsenic spectra as the result of laser induced heating [30,31], possibly combined with photo-oxidation [28]. The activation of the oxidation reaction can be followed by the power dependence of the relative intensities of the fitted arsenic and InAs Raman peaks presented in figure 1(d) measured, using 520.8 nm laser excitation and 15 min integration time per spectrum, of a NW suspended over a 150 nm deep and 2 μm wide trench [21]. Initially, at the lowest powers, the arsenic peaks are absent, but then irreversibly appear after applying illuminating powers above 120 kW cm −2 .…”
Section: Resultsmentioning
confidence: 99%
“…Figure 1(b) shows an example of a TEM image of the NWs showing high crystal quality and occasional stacking faults, and figure 1(c) shows typical Raman spectra for the two cases of a pristine InAs NW on Si substrate [21] and an oxidized InAs NW on a TEM membrane. The spectra of the nonoxidized NW is identical to bulk InAs and contain one main peak at ∼216 cm −1 assigned to the InAs transverse optical (TO) phonon mode and a weak side-peak at 237 cm −1 assigned to the longitudinal optical (LO) mode.…”
Section: Resultsmentioning
confidence: 99%
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“…Besides the typical photon energy (~ν 4 ) dependence of the Raman signal 1 , many materials 2 – 4 as well as nanomaterials, such as quantum dots 5 , 6 , carbon nanotubes 7 11 , semiconductors 12 , semiconducting nanowires 13 , 14 and graphene 15 , 16 show resonances at specific photon energy ranges accompanied by strong enhancement of the Raman signal by several orders of magnitude 2 ,3, 9 , 16 – 19 . Accurate determination of these resonances requires light sources with large tunable energy ranges and narrow emission lines.…”
Section: Introductionmentioning
confidence: 99%