2006
DOI: 10.1007/s00339-006-3789-4
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Quantitative depth profile study of polyaniline films by photothermal spectroscopies

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Cited by 10 publications
(6 citation statements)
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“…The gas acts as a piston in order to produce a sound wave which is detected by a microphone connected to the chamber. [6][7][8][9][10] As the microphone signal is proportional to radiation absorption by the sample, PAS gives results similar to absorbance spectra, i.e., conventional optical absorption spectroscopy. Also, as the signal depends on the modulation of the radiation source, PAS is able to perform a depth profile of the absorption in the sample, that is, at high modulation frequencies absorption information about the sample near the surface is obtained, while at low modulation frequencies the data come from deeper within the sample.…”
Section: Introductionmentioning
confidence: 94%
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“…The gas acts as a piston in order to produce a sound wave which is detected by a microphone connected to the chamber. [6][7][8][9][10] As the microphone signal is proportional to radiation absorption by the sample, PAS gives results similar to absorbance spectra, i.e., conventional optical absorption spectroscopy. Also, as the signal depends on the modulation of the radiation source, PAS is able to perform a depth profile of the absorption in the sample, that is, at high modulation frequencies absorption information about the sample near the surface is obtained, while at low modulation frequencies the data come from deeper within the sample.…”
Section: Introductionmentioning
confidence: 94%
“…5 The heat propagation across the whole chamber is governed by heat diffusion equations of each medium coupled via boundary conditions at the interfaces (T a = T b and k a dT a /dx = k b dT b /dx, a and b are adjacent media, T is temperature and k is thermal conductivity). After all mathematical treatment, the normalized photoacoustic signal (S n ) produced by the microphone is: [5][6][7][8][9][10]17 (2) where r s = b s /s s , b s is the sample optical absorption coefficient, s s = (1 + i)a s with i = (-1) ½ and a s = (p f /a s ) ½ , a s is the sample thermal diffusivity, b nm = k n a n /k m a m (n = g, s, b, that is, g = gas, s = sample, b = backing), and L S is the sample thickness. This equation is a complex mathematical function of the optical, thermal and geometrical parameters of the system, and it governs our results for all the chopper frequencies.…”
Section: Photoacoustic Spectroscopy Theorymentioning
confidence: 99%
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“…This technique typically uses a modulation of laser beam for inducing a thermal-wave (TW) field in the sample. The obtained TW distribution is then detected by various photothermal methods, such as photoacoustics [40], photothermal spectroscopy [41] or PPE techniques [11,42]. Recently, many useful applications of the photopyroelectric (PPE) effect have been reported with regard to the measurement of both thermal and optical absorption properties of a material [43].…”
Section: Theoretical Background: Photopyroelectric Techniquementioning
confidence: 99%
“…6,9 Furthermore, PAS of condensed-phase samples is often applied to depth profiling of layered samples and two-and three-dimensional tomographic imaging for biomedical applications. 10,12 Although there have been several reports discussing the use of tunable infrared sources, such as quantum cascade lasers (QCLs) and CO 2 lasers, to obtain photoacoustic spectra of gases, 13,20 the application of these sources in photoacoustic experiments on condensed-phase samples are minimal. 9,21,22 In this current work, we report on the use of a continuously tunable pulsed QCL, in combination with a photoacoustic cell designed for solid and liquid samples, for detection of tetraethoxysilane (TEOS) or glycerol films deposited on a substrate, and discrimination between these compounds and the substrate itself based on sample depth profiling.…”
Section: Introductionmentioning
confidence: 99%