Thickness uniformity of diamond-like carbon (DLC) films formed on 5 in. Si wafers by a supermagnetron plasma chemical vapor deposition with applying a static magnetic field was evaluated as a function of radio-frequency (rf) phase difference (RFPD) between two synchronized rf powers (13.56 MHz) supplied to parallel electrodes. When RFPD was 0°, the uniformity of DLC film formed on a lower electrode became poor (about ±9%), and at RFPD of about 180°, it became excellent (about ±3%). Thickness distributions were measured as a function of upper-electrode rf power (UPRF) at lower-electrode rf power (LORF) of 400 W. When UPRF was 0 W (conventional magnetron plasma mode), linearly graded thickness distribution was observed along perpendicular direction to magnetic field lines. At UPRF of 100 W, almost uniform distribution of ±2.9% was obtained, and an inverse thickness distribution to the distribution at UPRF of 0 W was observed at UPRF of 200 W, i.e., inverse magnetron plasma mode. Thickness uniformity also depended on electrode spacing, and good uniformity of ±3% was obtained at a separation of 40–45 mm. By applying a rotating magnetic field, extremely good uniformity of ±1.3% could be obtained.
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March 2000
Research Article|
March 01 2000
Thickness distribution of large-area diamondlike carbon films formed by supermagnetron plasma chemical vapor deposition with application of a stationary magnetic field
Haruhisa Kinoshita;
Haruhisa Kinoshita
Research Institute of Electronics, Shizuoka University, 3-5-1 Johoku, Hamamatsu 432-8011, Japan
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Shyuji Nomura;
Shyuji Nomura
Research Institute of Electronics, Shizuoka University, 3-5-1 Johoku, Hamamatsu 432-8011, Japan
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Masahiro Honda
Masahiro Honda
Research Institute of Electronics, Shizuoka University, 3-5-1 Johoku, Hamamatsu 432-8011, Japan
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J. Vac. Sci. Technol. A 18, 367–371 (2000)
Article history
Received:
January 14 1999
Accepted:
October 29 1999
Citation
Haruhisa Kinoshita, Shyuji Nomura, Masahiro Honda; Thickness distribution of large-area diamondlike carbon films formed by supermagnetron plasma chemical vapor deposition with application of a stationary magnetic field. J. Vac. Sci. Technol. A 1 March 2000; 18 (2): 367–371. https://doi.org/10.1116/1.582194
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