2012
DOI: 10.1364/ao.51.006578
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Surface heating by optical beams and application to mid-infrared imaging

Abstract: Heating of surfaces by optical beams is investigated theoretically and compared with experimental results in the context of infrared imaging with vanadium dioxide thin films. Using known solutions for the diffusion of point heat sources at the interface between two semi-infinite media, the theory is extended to beams of Gaussian and flat profiles, for steady-state and dynamic regimes. Parameters relevant to imaging, such as spatial resolution and response time, are linked to thermal diffusivity, beam dimension… Show more

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Cited by 11 publications
(5 citation statements)
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“…The difference in Seebeck coefficient ∆S = S 2 − S 1 = 2 µV/K is displayed in figure 1(c). Here the temperature distribution is assumed to have a Gaussian shape (see [23] and SI) and we convolute each line of the Seebeck map with the temperature distribution to obtain the thermovoltage map. As can be seen in figure 1(d), the resulting thermovoltage signal is positive along the position of the junction where the BLG changes to SLG, reproducing the experimentally observed results well.…”
Section: Resultsmentioning
confidence: 99%
“…The difference in Seebeck coefficient ∆S = S 2 − S 1 = 2 µV/K is displayed in figure 1(c). Here the temperature distribution is assumed to have a Gaussian shape (see [23] and SI) and we convolute each line of the Seebeck map with the temperature distribution to obtain the thermovoltage map. As can be seen in figure 1(d), the resulting thermovoltage signal is positive along the position of the junction where the BLG changes to SLG, reproducing the experimentally observed results well.…”
Section: Resultsmentioning
confidence: 99%
“…Here the temperature distribution is assumed to have a Gaussian shape see ( [22] and SI) and we convolute each line of the Seebeck map with the temperature distribution to obtain the thermovoltage map. As can be seen in Figure 1d, the resulting thermovoltage signal is positive along the position of the junction where the BLG changes to SLG, reproducing the experimentally observed results well.…”
Section: Resultsmentioning
confidence: 99%
“…For example, other sensor technologies that could benet from KLT denoising are nanowire temperature sensors, 22 graphene-based biosensors for immunoassay of small molecules, 23 indirect absorption spectroscopy, 24 microcantilever-based detection of protein markers, 25 microcantilever-based detection of CrO 4 , 2-8 mid-infrared spectroscopy of exhaled breath analysis, 26 surface-enhanced Raman scattering (SERS) detection of organophosphate pesticides, 27 and also sensing applications where surface heating by optical beams occur. 28 In Section 2 the analysis of the random uctuation of a micro-oscillator is discussed; KLT is introduced and applied to both ambient and photoacoustically induced responses. The random uctuation in spectroscopic measurement is discussed in Section 3, where the experimental setup and analysis of the obtained infrared (IR) absorption spectra for a set of test compounds including Poplar cross sections, a biomass with considerable molecular complexity and of great importance in biofuel research are given.…”
Section: Introductionmentioning
confidence: 99%