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Effect of Sc<sub>2</sub>O<sub>3</sub> doping on thermal emission properties of rare-earth refractory yttrium salt cathode
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To improve the thermionic emission performance of the rare-earth refractory yttrium salt cathode used in the magnetron, the influence of Sc<sub>2</sub>O<sub>3</sub> doping on its thermionic emission properties is investigated. Cathodes are fabricated by incorporating different weight percentages of Sc<sub>2</sub>O<sub>3</sub> into the rare-earth refractory yttrium salt matrix, and their thermionic emission properties are systematically evaluated. The experimental findings reveal that the doping of Sc<sub>2</sub>O<sub>3</sub> significantly enhances the thermionic emission capability of the cathode. Notably, Sc<sub>2</sub>O<sub>3</sub> with a doping concentration of 3% has the most significant improvement in emission performance. The 3% Sc<sub>2</sub>O<sub>3</sub>-doped cathode can achieve a thermionic emission current density of 3.85 A/cm<sup>2</sup> under an anode voltage of 300 V at 1600 ℃. In contrast, under the same conditions, the undoped cathode provides a current density of only 1.66 A/cm<sup>2</sup>, indicating a 132% increase in thermionic emission efficiency when doped with 3% Sc<sub>2</sub>O<sub>3</sub>. By using the Richardson line method coupled with data-fitting algorithms, the absolute zero work functions for undoped and Sc<sub>2</sub>O<sub>3</sub>-doped cathodes (3%, 7%, and 11%) are determined to be 1.42, 0.93, 0.98, and 1.11 eV, respectively. The lifespan assessment indicates that at 1400℃ the cathode doped with 3% Sc<sub>2</sub>O<sub>3</sub> remains stable for over 4200 h under an initial load of 0.5 A/cm<sup>2</sup> without significant degradation. Finally, those cathodes are analyzed by the XRD, SEM, EDS, AES respectively. The analyses show that during thermionic emission testing, the Sc<sub>2</sub>O<sub>3</sub> and Y<sub>2</sub>Hf<sub>2</sub>O<sub>7</sub> undergo substitutional solid solution reactions, forming the Sc<sub><i>x</i></sub>Y<sub>(2–<i>x</i>)</sub>Hf<sub>2</sub>O<sub>[7+(3/2)<i>x</i>]</sub> solid solution. This process causes lattice distortion in the Y<sub>2</sub>Hf<sub>2</sub>O<sub>7</sub>, which makes it in a high-energy state, thus reducing the work function on the cathode surface. At the same time, Sc from Sc<sub>2</sub>O<sub>3</sub> displaces Y in the Y<sub>2</sub>Hf<sub>2</sub>O<sub>7</sub> unit cells, with the displaced Y existing in the form of metal, which enhances the electrical conductivity of the cathode surface. Additionally, the Sc<sub><i>x</i></sub>Y<sub>(2–<i>x</i>)</sub>Hf<sub>2</sub>O<sub>[7+(3/2)<i>x</i>]</sub> solid solution generates a substantial number of Vo<sup>2+</sup> oxygen vacancies and free electrons, thereby further augmenting surface conductivity. All in all, these mechanisms contribute to significantly improving the thermionic emission capability of the cathode.
Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
Title: Effect of Sc<sub>2</sub>O<sub>3</sub> doping on thermal emission properties of rare-earth refractory yttrium salt cathode
Description:
To improve the thermionic emission performance of the rare-earth refractory yttrium salt cathode used in the magnetron, the influence of Sc<sub>2</sub>O<sub>3</sub> doping on its thermionic emission properties is investigated.
Cathodes are fabricated by incorporating different weight percentages of Sc<sub>2</sub>O<sub>3</sub> into the rare-earth refractory yttrium salt matrix, and their thermionic emission properties are systematically evaluated.
The experimental findings reveal that the doping of Sc<sub>2</sub>O<sub>3</sub> significantly enhances the thermionic emission capability of the cathode.
Notably, Sc<sub>2</sub>O<sub>3</sub> with a doping concentration of 3% has the most significant improvement in emission performance.
The 3% Sc<sub>2</sub>O<sub>3</sub>-doped cathode can achieve a thermionic emission current density of 3.
85 A/cm<sup>2</sup> under an anode voltage of 300 V at 1600 ℃.
In contrast, under the same conditions, the undoped cathode provides a current density of only 1.
66 A/cm<sup>2</sup>, indicating a 132% increase in thermionic emission efficiency when doped with 3% Sc<sub>2</sub>O<sub>3</sub>.
By using the Richardson line method coupled with data-fitting algorithms, the absolute zero work functions for undoped and Sc<sub>2</sub>O<sub>3</sub>-doped cathodes (3%, 7%, and 11%) are determined to be 1.
42, 0.
93, 0.
98, and 1.
11 eV, respectively.
The lifespan assessment indicates that at 1400℃ the cathode doped with 3% Sc<sub>2</sub>O<sub>3</sub> remains stable for over 4200 h under an initial load of 0.
5 A/cm<sup>2</sup> without significant degradation.
Finally, those cathodes are analyzed by the XRD, SEM, EDS, AES respectively.
The analyses show that during thermionic emission testing, the Sc<sub>2</sub>O<sub>3</sub> and Y<sub>2</sub>Hf<sub>2</sub>O<sub>7</sub> undergo substitutional solid solution reactions, forming the Sc<sub><i>x</i></sub>Y<sub>(2–<i>x</i>)</sub>Hf<sub>2</sub>O<sub>[7+(3/2)<i>x</i>]</sub> solid solution.
This process causes lattice distortion in the Y<sub>2</sub>Hf<sub>2</sub>O<sub>7</sub>, which makes it in a high-energy state, thus reducing the work function on the cathode surface.
At the same time, Sc from Sc<sub>2</sub>O<sub>3</sub> displaces Y in the Y<sub>2</sub>Hf<sub>2</sub>O<sub>7</sub> unit cells, with the displaced Y existing in the form of metal, which enhances the electrical conductivity of the cathode surface.
Additionally, the Sc<sub><i>x</i></sub>Y<sub>(2–<i>x</i>)</sub>Hf<sub>2</sub>O<sub>[7+(3/2)<i>x</i>]</sub> solid solution generates a substantial number of Vo<sup>2+</sup> oxygen vacancies and free electrons, thereby further augmenting surface conductivity.
All in all, these mechanisms contribute to significantly improving the thermionic emission capability of the cathode.
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