Electron transport parameters in pure C5F8 and C5F8-Ar mixtures

T.Harima, N.Hirama, M.Inoue, Y.Mamada, and Y.Nakamura;

Faculty of Science and Technology, Keio University, Hiyoshi, Yokohama 223-8522, Japan

Octafluorocycropenten (C5F8) is expected as one of the potential plasma sources which can meet the demands of the future ULSI manufacturing in two ways: higher etching selectivity of SiO2 to Si3N4[1] and higher deposition rate of fluorocarbon film on Si and Si3N4 surfaces[2]. The molecule has shorter atmospheric lifetime (one year) than other perfluorocarbon molecules (CF4, for example, has 50,000 years) and is expected far more friendly to the global environment than other popular etching gases. It, however, is rather recently industry manufactured and its electron collision cross section data and the related electron transport data are scarce.
We measured electron transport parameters, the electron drift velocity (W) and the product of the gas number density and the longitudinal diffusion coefficient (NDL) in pure C5F8 and C5F8-Ar mixtures. We used the double-shutter (four-gauze) drift tube, whose electron drift distance was variable from 1 to 10 cm. The electron arrival time spectra (ATSs) were observed at several drift distances, and the drift velocity and the longitudinal diffusion coefficient were determined from the positional variations of the mean arrival time and the characteristic width of the ATSs. From this the hydrodynamic equilibrium of the parameters were confirmed. Measurement was carried out over the E/N (where E is the applied electric field and N the gas number density and 10-17 Vcm2 = 1 Td) range from 50 to 4000 Td in pure C5F8 and from 5 to 100 Td in C5F8-Ar mixtures.
The ATSs observed in pure C5F8 usually showed a dim component of delayed electrons following immediately after the main electrons. The more precise analysis including electron detachment may be needed, and that may alter the present NDL. The present W and NDL had a broad minimum (2.0x107 cm/s and 1.0x1022 cm-1s-1, respectively) at 150-300 Td. The total electron cross section of C5F8 over the electron energy range of 5-3000 eV is about 50% larger than c-C4F8 which also has a cyclic structure but with a single bond[3]. The present drift velocity, however, was higher than that in pure c-C4F8, and the latter increased rather monotonously with increasing E/N[4].

References

[1] H. Motomura, S. Imai, K. Tachibana, Thin Solid Films 374 (2000) 243
[2] K. Takahashi, A. Itoh, T. Nakamura, K. Tachibana, Thin Solid Films 374 (2000) 303
[3] K. Okuda, Master’s thesis (Keio University, 2003)
[4] M. Yamaji and Y. Nakamura, J. Phys. D: Appl. Phys. 36 (2003) 640