1992Bulletin of the Korean Chemical SocietyRequires access

Electrical Conductivity of the Solid Solutions X $ZrO_2+ (1-X) Yb_2O_3; 0.01{\leq}X{\leq}0.09$

Choi Byoung Ki, Jang Joon Ho, Seong‐Han Kim, Hong Seok Kim, Jong Sik Park, Kim Yoo Young, Don Kim, Lee Sung Han, Yo Chul Hyun, Kim Keu Hong

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Abstract

solutions containing 1, 3, 5, 7 and 9 mol% synthesized from spectroscopically pure and powders and found to be rare earth C-type structure by XRD technique. Electrical conductivities were measured as a function of temperatures from 700 to and oxygen partial pressures from 1 to 2 atm. The electrical conductivities depend simply on temperature and the activation energies are determined to be 1.56-1.68 . The oxygen partial pressure dependence of the electrical conductivity shows that the conductivity increases with increasing oxygen partial pressure, indicating p-type semiconductor. The dependence of the system is nearly power of 1/4. It is suggested from the linearity of the temperature dependence of electrical conductivity and only one value of 1/n that the solid solutions of the system have single conduction mechanism. From these results, it is concluded that the main defects of the system are negatively doubly charged oxygen interstitial in low. level and negatively triply charged cation vacancy in high doping level and the electrical conduction is due to the electronic hole formed by the defect structure.

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solutions containing 1, 3, 5, 7 and 9 mol% synthesized from spectroscopically pure and powders and found to be rare earth C-type structure by XRD technique. Electrical conductivities were measured as a function of temperatures from 700 to and oxygen partial pressures from 1 to 2 atm. The electrical conductivities depend simply on temperature and the activation energies are determined to be 1.56-1.68 . The oxygen partial pressure dependence of the electrical conductivity shows that the conductivity increases with increasing oxygen partial pressure, indicating p-type semiconductor. The dependence of the system is nearly power of 1/4. It is suggested from the linearity of the temperature dependence of electrical conductivity and only one value of 1/n that the solid solutions of the system have single conduction mechanism. From these results, it is concluded that the main defects of the system are negatively doubly charged oxygen interstitial in low. level and negatively triply charged cation vacancy in high doping level and the electrical conduction is due to the electronic hole formed by the defect structure.

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Available abstract

solutions containing 1, 3, 5, 7 and 9 mol% synthesized from spectroscopically pure and powders and found to be rare earth C-type structure by XRD technique. Electrical conductivities were measured as a function of temperatures from 700 to and oxygen partial pressures from 1 to 2 atm. The electrical conductivities depend simply on temperature and the activation energies are determined to be 1.56-1.68 . The oxygen partial pressure dependence of the electrical conductivity shows that the conductivity increases with increasing oxygen partial pressure, indicating p-type semiconductor. The dependence of the system is nearly power of 1/4. It is suggested from the linearity of the temperature dependence of electrical conductivity and only one value of 1/n that the solid solutions of the system have single conduction mechanism. From these results, it is concluded that the main defects of the system are negatively doubly charged oxygen interstitial in low. level and negatively triply charged cation vacancy in high doping level and the electrical conduction is due to the electronic hole formed by the defect structure.

Key concepts: Electrical resistivity and conductivity, Partial pressure, Oxygen, Conductivity, Doping, Thermal conduction, Solid solution, Materials science

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Electrical Conductivity of the Solid Solutions X $ZrO_2+ (1-X) Yb_2O_3; 0.01{\leq}X{\leq}0.09$ — Research Paper | ScholarLens