| 摘要 |
An electron density at an ECR point, which is spaced from a substrate to be treated and which faces the substrate, is set to be higher than or equal to 0.46 nc (nc: an upper limit side cut-off density of an X wave) and lower than nc. Thus, a high chevron distribution of electron density is formed in end portions of a magnetic field forming region, and a distribution of electron density having a lower peak value than those in the end portions is formed in a central portion of the magnetic field forming region. In this case, the periphery of a magnetic field crosses the inner wall of a vacuum chamber once between the ECR point and the substrate, and a space of one fourth or more of the wavelength of the X wave is formed between the periphery of the magnetic field and the inner wall of the vacuum chamber as the magnetic field runs downstream. Thus, it is possible to achieve an inplane uniform treatment when carrying out a treatment, such as a thin film deposition or etching, with ECR plasmas for a wafer.
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