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    Wyświetlanie 1-4 z 4
    Tytuł:
    Analysis of Non-Steady Stage in SAW Gas Sensors with Semiconducting Sensor Layers
    Autorzy:
    Urbańczyk, M.
    Hejczyk, T.
    Powiązania:
    https://bibliotekanauki.pl/articles/1493326.pdf
    Data publikacji:
    2011-10
    Wydawca:
    Polska Akademia Nauk. Instytut Fizyki PAN
    Tematy:
    07.07.Df
    43.25.Fe
    68.35.Iv
    77.65.Dq
    Opis:
    The profile of the gas concentration in the sensor layer can be expressed as a polynomial function involving the diffusion coefficient $(D_{K})$, semiconductor film thickness (h), rate constant (k), gas concentration outside the semiconductor film $(C_{S})$. Before reaching a steady state of the concentration profile, its behavior depends on a few factors as the distance from the piezoelectric surface, the rate constant, the thickness of the layer and the diffusion constant and time. We are going to simulate temporary processes in the semiconductor sensor film in the surface acoustic wave gas sensor system and to describe the influence on relative changes of the surface acoustic wave velocity. The numerical results basing on the code written in Pyton, are described and analyzed.
    Źródło:
    Acta Physica Polonica A; 2011, 120, 4; 789-793
    0587-4246
    1898-794X
    Pojawia się w:
    Acta Physica Polonica A
    Dostawca treści:
    Biblioteka Nauki
    Artykuł
    Tytuł:
    Numerical Optimization of Structures SAW Gas Sensors
    Autorzy:
    Hejczyk, T.
    Urbańczyk, M.
    Powiązania:
    https://bibliotekanauki.pl/articles/1399352.pdf
    Data publikacji:
    2013-09
    Wydawca:
    Polska Akademia Nauk. Instytut Fizyki PAN
    Tematy:
    43.25.Fe
    77.65.Dq
    68.35.Iv
    07.07.Df
    Opis:
    This paper presents the results of the analysis of surface acoustic waves sensor equivalent model. They were the sensor response of the surface acoustic waves sensor in the steady state gas: $H_2$, $CO_2$, $NO_2$, $NH_3$, $C_nH_m$, $CO$. Thin layer of $WO_3$ has been used as a sensor layer. Impedance replacement of sensor layer, taking into account the profile of the concentration of gas molecules in the layer, has been implemented into the equation of Ingebrigtsen, which enabled us to obtain analytical expressions for the relative changes in surface wave velocity in the steady state. The results of the analysis show that there is an optimum thickness of layer sensor for which an acoustoelectric effect (change in the acoustic wave velocity) is the highest.
    Źródło:
    Acta Physica Polonica A; 2013, 124, 3; 432-435
    0587-4246
    1898-794X
    Pojawia się w:
    Acta Physica Polonica A
    Dostawca treści:
    Biblioteka Nauki
    Artykuł
    Tytuł:
    $WO_3-Pd$ Structure in SAW Sensor for Hydrogen Detection
    Autorzy:
    Hejczyk, T.
    Urbańczyk, M.
    Powiązania:
    https://bibliotekanauki.pl/articles/1493196.pdf
    Data publikacji:
    2011-10
    Wydawca:
    Polska Akademia Nauk. Instytut Fizyki PAN
    Tematy:
    43.25.Fe
    77.65.Dq
    68.35.Iv
    07.07.Df
    Opis:
    In the paper a new sensor structure for surface acoustic wave gas system is presented. A bilayer structure $WO_3-Pd$ thin films may be useful for hydrogen detection in low concentration in air. A bilayer sensor structure of tungsten oxide $WO_3$ with a very thin catalytic film of palladium on the top has been studied for gas-sensing application at room temperature (about 25°C) in surface acoustic wave system. The bilayer structure of $WO_3$ layers with a thickness of about 50 nm, 100 nm and 150 nm was made onto a $LiNbO_3$ Y-cut Z-propagating substrate by means of the vacuum sublimation method using a special aluminum mask. The vapor source consisted of commercially available $WO_3$ powder (Fluka 99.9%) and molybdenum heater. The thin palladium (Pd) layer (about 10 nm) was made separately on each $WO_3$ layer by means of vapor deposition in high vacuum. There have been investigated three structures: 50 nm $WO_3$ + 10 nm Pd, 100 nm $WO_3$ + 10 nm Pd and 150 nm $WO_3$ + 10 nm Pd in three canal surface acoustic wave system with reference oscillator. Numerical results obtained by analysis of the surface acoustic wave gas sensor model have been compared with experimental results.
    Źródło:
    Acta Physica Polonica A; 2011, 120, 4; 616-620
    0587-4246
    1898-794X
    Pojawia się w:
    Acta Physica Polonica A
    Dostawca treści:
    Biblioteka Nauki
    Artykuł
    Tytuł:
    Bilayer Structures of $NiO_{x}$ and Pd in Surface Acoustic Wave and Electrical Gas Sensor Systems
    Autorzy:
    Jakubik, W.
    Urbańczyk, M.
    Maciak, E.
    Pustelny, T.
    Powiązania:
    https://bibliotekanauki.pl/articles/1795797.pdf
    Data publikacji:
    2009-09
    Wydawca:
    Polska Akademia Nauk. Instytut Fizyki PAN
    Tematy:
    43.25.Fe
    77.65.Dq
    43.35.Pt
    68.35.Iv
    07.07.Df
    Opis:
    A bilayer sensor structure of nickel oxide $NiO_x$ ( ≈ 60 nm) with a very thin film of palladium (Pd ≈ 18 nm) on the top, has been studied for gas-sensing application at relatively low temperatures of about 30°C and 60°C. The bilayer structure was obtained by rf sputtering and by vacuum deposition (first the $NiO_{x}$ and then the Pd film) onto a $LiNbO_{3}$ Y-cut Z-propagating substrate, making use of the surface acoustic wave method, and additionally (in the same technological processes) onto a glass substrate with a planar microelectrode array for simultaneous monitoring of the planar resistance of the layered structure. Such a bilayer structure was investigated in a low concentration range (from 50 ppm to 400 ppm in air) of nitrogen dioxide $(NO_{2})$, carbon monoxide (CO) and ammonia $(NH_{3})$ in a dry and wet air atmosphere and in a medium hydrogen concentration (1-2.5%) in dry air. The $NiO_{x}$ and Pd bilayer structure interact rather weakly with $NO_{2}$ molecules but with CO and $NH_{3}$ this interaction is much greater, especially at higher temperature ( ≈ 60°C). The hydrogen sensitivity is on the medium level, not exceeding 600 Hz (relative change in the differential frequency of ≈ 2.3%) at interaction temperature of 35°C.
    Źródło:
    Acta Physica Polonica A; 2009, 116, 3; 315-320
    0587-4246
    1898-794X
    Pojawia się w:
    Acta Physica Polonica A
    Dostawca treści:
    Biblioteka Nauki
    Artykuł
      Wyświetlanie 1-4 z 4

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