Abstract

AgSnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> , as the most potential material to replace AgCdO, is widely used in low-voltage electrical appliances. However, because of the high hardness and poor conductivity of SnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> , AgSnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> has the problems of processing difficulties and large contact resistance. Based on the first principles of density functional theory, a method is proposed to calculate the electronic structure and mechanical properties of SnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> , SnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -Ce, SnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -N, and SnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -Ce-N. By analyzing the energy band, density of states, and elastic constants, the results show that Ce-N co-doped SnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> has the highest relative conductivity, reduced hardness, and increased ductility and overcome processing difficulty. The doped AgSnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> contact material was prepared by sol-gel method and powder metallurgy method, and the hardness and electrical properties of the sample were tested. The experimental results show that AgSnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -Ce-N contacts have higher conductivity, lower contact resistance and arc energy, and lower hardness. The theory is consistent with the experiment, proving the feasibility of simulation. Therefore, Ce and N co-doping can effectively overcome the disadvantages of AgSnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> contact materials, improve conductivity, and overcome processing difficulty. It provides a new idea and theoretical basis for the doping research of AgSnO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> contact materials.

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