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Impact of Ruthenium Diffusion on the Electrical Properties of Thick Film Resistors

Avazbek T. DekhkonovNational University of Uzbekistan named after Mirzo Ulugbek, Tashkent, UzbekistanG. AbdurakhmanovNational University of Uzbekistan named after Mirzo Ulugbek, Tashkent, UzbekistanMukhriddin E. TursunovNational University of Uzbekistan named after Mirzo Ulugbek, Tashkent, UzbekistanShokhzod M. NorbekovTashkent Institute of Management and Economics, Tashkent, Uzbekistan; Almalyk Branch of Tashkent State Technical University, Almalyk, Tashkent Region, UzbekistanД. А. ТашмухамедоваTashkent State Technical University named after Islom Karimov, Tashkent, UzbekistanGulbakhor VokhidovaAlfakom Non-state Training Center, Tashkent, UzbekistanDibya Prakash RaiDepartment of Physics, Mizoram University, Aizawl, IndiaUmmatjon A. AsrorovNational Pedagogical University of Uzbekistan named after Nizami, Tashkent, Uzbekistan; National University of Uzbekistan named after Mirzo Ulugbek, Tashkent, Uzbekistan
ABI

Аннотация

The diffusion profile of the RuO2 into silicate glass and the electrical resistance distribution across diffusion layer have been studied by beveled sample method and energy dispersion spectroscopy. The distribution of content of Ru atoms in the diffusion layer is described by the erfc(x) what means that the diffusion coefficient is independent of the content of Ru atoms. The correlation of the distribution of Ru atom content and the resistance distribution in the diffusion layer showed that it is the diffusion doping of glass that is responsible for the conductivity of thick-film resistors. Thickness of the diffusion layer is more than 100 μm while average distance between RuO2 particles is about 0.5-2 μm. It means that all volume of the thick-film resistor comes conductive in firing process at 850°C in 10 minutes.

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