The properties of Cu films deposited by high rate magnetron sputtering from a liquid target / G. A. Bleykher (Bleicher) [et al.]

Уровень набора: VacuumАльтернативный автор-лицо: Bleykher (Bleicher), G. A., physicist, Professor of Tomsk Polytechnic University, Doctor of Physical and Mathematical Sciences, 1961-, Galina Alekseevna;Yuryeva, A. V., specialist in the field of hydrogen energy and plasma technologies, assistant Professor of Tomsk Polytechnic University, 1983-, Alena Victorovna;Shabunin, A. S., Physicist, Engineer of Tomsk Polytechnic University, 1987-, Artem Sergeevich;Sidelev, D. V., physicist, engineer of Tomsk Polytechnic University, 1991-, Dmitry Vladimirovich;Grudinin, V. A., physicist, engineer of Tomsk Polytechnic University, 1995-, Vladislav Alekseevich;Yuriev, Yu. N., specialist in the field of hydrogen energy, Head of the laboratory of Tomsk Polytechnic University, Associate Scientist, 1984-, Yuri NikolaevichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет, Инженерная школа ядерных технологий, Научно-образовательный центр Б. П. ВейнбергаЯзык: английский.Резюме или реферат: The focus of the paper is Cu films obtained by magnetron sputtering a liquid target at an average power density not exceeding 45 W/cm2. The deposition rates reached 140 nm/s. In the film formation, the pulsed power supplies of two types have been used. The discharge has functioned in an Ar atmosphere and in self-sustained mode. Structural and electrically conductive properties of the films have been analyzed. A comparison was made with those deposited by sputtering a cooled target with similar power. It has revealed that the evaporation of the magnetron target plays a dominant role in the formation of the structural and conductive properties of Cu films. The Cu films deposited by sputtering evaporative liquid targets have a lower electrical resistance than the films of similar thickness obtained by sputtering cooled targets. The mode of self-sustained sputtering does not significantly affect the structural properties of the films as compared with sputtering in the Ar atmosphere, but the electrical resistivity is approximately 20% lower. Due to high deposition rate in the case with evaporative targets the heating of the substrate when producing films of equal thickness turns out to be less than when using a magnetron with a cooled target..Примечания о наличии в документе библиографии/указателя: [References: 45 tit.].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ | magnetron sputtering systems | liquid-phase sputtering | evaporation | self-sustained sputtering | Cu films and coatings | Cu films electrical resistance | магнетронные распылительные системы | выпаривание | распыление | пленки | покрытия | электрическое сопротивление Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: 45 tit.]

The focus of the paper is Cu films obtained by magnetron sputtering a liquid target at an average power density not exceeding 45 W/cm2. The deposition rates reached 140 nm/s. In the film formation, the pulsed power supplies of two types have been used. The discharge has functioned in an Ar atmosphere and in self-sustained mode. Structural and electrically conductive properties of the films have been analyzed. A comparison was made with those deposited by sputtering a cooled target with similar power. It has revealed that the evaporation of the magnetron target plays a dominant role in the formation of the structural and conductive properties of Cu films. The Cu films deposited by sputtering evaporative liquid targets have a lower electrical resistance than the films of similar thickness obtained by sputtering cooled targets. The mode of self-sustained sputtering does not significantly affect the structural properties of the films as compared with sputtering in the Ar atmosphere, but the electrical resistivity is approximately 20% lower. Due to high deposition rate in the case with evaporative targets the heating of the substrate when producing films of equal thickness turns out to be less than when using a magnetron with a cooled target.

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