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Tin oxide (SnO2) is an n-type wide band gap (3.6 eV) semiconductor which has been used for various applications as catalytic support materials, transparent electrodes, in solar cells and solid-state gas sensors [1]. During the last two years, novel gas nanosensors have been proposed using the luminescent properties of metallic oxides (ZnO, SnO2) where luminescence intensity is modified according to the nature and concentration of adsorbed gases [2]. On the other hand, the optical fiber sensor is based on the evanescent-wave absorption which has potential to monitor a leakage over wide area. In this case, the material absorbs the wavelengths carried by the fiber and modifies the absorption as a function of gas concentration to be detected [3]. In this work, SnO2 nanoparticles (NPs) were deposited on optical fibers and glass substrates. A morphological and chemical analysis were performed on the obtained samples.SnO2 nanoparticles were prepared using 3.0 g of SnCl4·2H2O dissolved in 25 ml of anhydrous ethanol. 4 ml glacial acetic acid was added as chelating agent. The solution became clear and homogeneous after stirring during 20 min. The cleaned glass substrate and optical fibers (10 µm of diameter) were independently dipped into SnCl4 solution. After that, they were removed from the solution (pull rate of 200 mm/min). Another reduced optical fiber (120 µm of diameter) were also fabricated using the flamebrushing technique [4] upon which a drop of SnCl4 solution was deposited. All samples were dried at 250 °C for 20 min. Figure 1a) shows a SEM image of spherical SnO2 fine particles deposited on glass substrate having diameters of 20-30 nm. The typical photoluminescence (PL) spectrum of SnO2 NPs is presented in the inset the figure 1a). The visible emission (550 nm) is generally suggested that come from defects such as oxygen vacancies and tin interstitial or dangling bonds [5]. Figure 1b) shows the XPS survey spectrum of SnO2 NPs, which revels the presence of carbon, sodium, chlorine, oxygen and tin. The peaks of C 1s and Na (KLL) are attributed mainly to contamination during storage of samples. The peaks of Sn 3d, 4d, 3p, 4p and 4s from SnO2 also are observed. Two XPS peaks located at 486.15 and 494.55 eV are related to Sn 3d5/2 and Sn 3d3/2 spin orbit peaks of SnO2, confirming the formation of SnO2 NPs. However, traces of SnCl2 (487.39 eV) and metallic Sn (484.90 eV) were also found on the surface of the sample. This could be due to an incomplete oxidation of tin precursor salt during thermal annealing. On the other hand, the surface morphology of reduced optical fiber exhibits a cluster morphology with varying cluster sizes and random distribution across the surface (Fig. 2a). The average cluster size is 200 nm, which was estimated from inset Fig. 2a). In addition, the clusters might be formed by SnO2 NPs (20-30 nm). Fig 2b) shows a SEM image of the optic fiber (120 µm) surface morphology after the deposition of the SnO2 NPs using the drop-casting method. The surface was uniformly covered after thermal anneal...
Tin oxide (SnO2) is an n-type wide band gap (3.6 eV) semiconductor which has been used for various applications as catalytic support materials, transparent electrodes, in solar cells and solid-state gas sensors [1]. During the last two years, novel gas nanosensors have been proposed using the luminescent properties of metallic oxides (ZnO, SnO2) where luminescence intensity is modified according to the nature and concentration of adsorbed gases [2]. On the other hand, the optical fiber sensor is based on the evanescent-wave absorption which has potential to monitor a leakage over wide area. In this case, the material absorbs the wavelengths carried by the fiber and modifies the absorption as a function of gas concentration to be detected [3]. In this work, SnO2 nanoparticles (NPs) were deposited on optical fibers and glass substrates. A morphological and chemical analysis were performed on the obtained samples.SnO2 nanoparticles were prepared using 3.0 g of SnCl4·2H2O dissolved in 25 ml of anhydrous ethanol. 4 ml glacial acetic acid was added as chelating agent. The solution became clear and homogeneous after stirring during 20 min. The cleaned glass substrate and optical fibers (10 µm of diameter) were independently dipped into SnCl4 solution. After that, they were removed from the solution (pull rate of 200 mm/min). Another reduced optical fiber (120 µm of diameter) were also fabricated using the flamebrushing technique [4] upon which a drop of SnCl4 solution was deposited. All samples were dried at 250 °C for 20 min. Figure 1a) shows a SEM image of spherical SnO2 fine particles deposited on glass substrate having diameters of 20-30 nm. The typical photoluminescence (PL) spectrum of SnO2 NPs is presented in the inset the figure 1a). The visible emission (550 nm) is generally suggested that come from defects such as oxygen vacancies and tin interstitial or dangling bonds [5]. Figure 1b) shows the XPS survey spectrum of SnO2 NPs, which revels the presence of carbon, sodium, chlorine, oxygen and tin. The peaks of C 1s and Na (KLL) are attributed mainly to contamination during storage of samples. The peaks of Sn 3d, 4d, 3p, 4p and 4s from SnO2 also are observed. Two XPS peaks located at 486.15 and 494.55 eV are related to Sn 3d5/2 and Sn 3d3/2 spin orbit peaks of SnO2, confirming the formation of SnO2 NPs. However, traces of SnCl2 (487.39 eV) and metallic Sn (484.90 eV) were also found on the surface of the sample. This could be due to an incomplete oxidation of tin precursor salt during thermal annealing. On the other hand, the surface morphology of reduced optical fiber exhibits a cluster morphology with varying cluster sizes and random distribution across the surface (Fig. 2a). The average cluster size is 200 nm, which was estimated from inset Fig. 2a). In addition, the clusters might be formed by SnO2 NPs (20-30 nm). Fig 2b) shows a SEM image of the optic fiber (120 µm) surface morphology after the deposition of the SnO2 NPs using the drop-casting method. The surface was uniformly covered after thermal anneal...
Most trace gas detection methods developed so far largely rely on active sampling procedures, which are known to introduce different kinds of artifacts. Here, we demonstrate sampling-free in situ trace gas detection in millimeter scale volumes with fiber coupled cantilever enhanced photoacoustic spectroscopy. Our 2.4 mm diameter fiber-tip sensor is free from the wavelength modulation induced background signal (a phenomenon that is often overlooked in photoacoustic spectroscopy) and reaches a normalized noise equivalent absorption coefficient of 1.3 × 10−9 W cm−1 Hz−1/2 for acetylene detection. To validate its in situ gas detection capability, we inserted the sensor into a mini fermenter for headspace monitoring of CO2 production during yeast fermentation. Our results show that the sensor can easily follow the different stages of the CO2 production of the fermentation process in great detail.
Layered structures containing small-angle wedges are widely used as linear variable filters (LVFs) in microspectrometers, sensors, and hyperspectral imaging systems. Here, we propose a method based on the scattering matrix formalism allowing one to describe the optical properties of layered structures with multiple wedges. As examples, we consider a single-wedge LVF with Bragg claddings and an LVF with three wedges, the latter exhibiting a flat-top resonant transmission peak. We show that the proposed method provides a two orders of magnitude increase in speed compared to the rigorous numerical simulations based on the Fourier modal method. At the same time, as we demonstrate, the results obtained with these two methods are very close to each other. The proposed approach is promising for the design and investigation of LVFs containing several wedge-shaped layers.
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