Hostname: page-component-586b7cd67f-2plfb Total loading time: 0 Render date: 2024-11-27T01:39:30.904Z Has data issue: false hasContentIssue false

Effects of boron doping for the structural evolution of vapor-grown carbon fibers studied by Raman spectroscopy

Published online by Cambridge University Press:  31 January 2011

K. Nishimura
Affiliation:
Faculty of Engineering, Shinshu University, 500 Wakasato, Nagano 380, Japan
Y. A. Kim
Affiliation:
Faculty of Engineering, Shinshu University, 500 Wakasato, Nagano 380, Japan
T. Matushita
Affiliation:
Faculty of Engineering, Shinshu University, 500 Wakasato, Nagano 380, Japan
T. Hayashi
Affiliation:
Faculty of Engineering, Shinshu University, 500 Wakasato, Nagano 380, Japan
M. Endo
Affiliation:
Faculty of Engineering, Shinshu University, 500 Wakasato, Nagano 380, Japan
M. S. Dresselhaus
Affiliation:
Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
Get access

Abstract

The structural deviation of boron-doped vapor-grown carbon fibers (VGCFs) with diameters around 10 μm relative to their undoped counterparts was investigated by polarized microprobe Raman spectroscopy and field-omission scanning electron microscopy as a function of heat-treatment temperature (HTT). Boron doping induces the formation of dislocation loops in the surface, which combine into larger loops with increasing HTT. The depolarization ratio, Dp, of the E2g2 mode for VGCFs increases gradually with increasing HTT, and finally approaches the value of highly oriented pyrolytic graphite, which is consistent with the asymmetric shape of the peak at ∼2725 cm−1 in the second-order Raman spectra. On the other hand, the Dp ratios of the E2g2 mode for boron-doped VGCFs show no deviations up to an HTT of 2100 °C, as compared to that of VGCFs, and decrease with increasing HTT, whereas the Dp ratios of the D peak show a maximum value at 2100 °C, and decrease gradually with increasing HTT. Consistent with these Raman results, boron atoms in the graphite lattice introduce a decreased d002 spacing (accelerating graphitization), but also hinder two-dimensional structural development and increase the amount of disorder. This is done by introducing tilt boundaries and vacancies, which make the Dp ratio of the E2g2 mode lower than the value for polycrystalline graphite, even though the fibers are heat treated at 2800 °C.

Type
Articles
Copyright
Copyright © Materials Research Society 2000

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1.Way, B.M., Dahn, J.R., Teidje, T., Myrtle, K., and Kasrai, M., Phys. Rev. B: Solid State 46, 1697 (1992).CrossRefGoogle Scholar
2.Kouvetakis, J., Kaner, R.B., Sattler, M.L., and Bartlett, N., J. Chem. Soc. Chem. Commun. 1758 (1986).CrossRefGoogle Scholar
3.Chesneau, M., Beguin, F., Conard, J., Erre, R., and Thebault, J., Carbon 30, 714 (1992).CrossRefGoogle Scholar
4.Fecko, D.L., Jones, L.E., and Thrower, P.A., Carbon 31, 637 (1993).CrossRefGoogle Scholar
5.Tomanek, D., Wentzcovitch, R.M., Louie, S.G., and Cohen, M.L., Phys. Rev. B: Solid State 37, 3134 (1988).CrossRefGoogle Scholar
6.Wang, Q., Ma, X., Chen, L-Q., Cermignani, W., and Pantano, C.G., Carbon 35, 307 (1997).CrossRefGoogle Scholar
7.Marinkovic, S., in Chemistry and Physics of Carbon, edited by Thrower, P.A. (Marcel Dekker, New York, 1984), Vol. 19, pp. 163.Google Scholar
8.Grosewald, P.S. and Walker, P.L. Jr, Tanso 61, 52 (1970).CrossRefGoogle Scholar
9.McClure, J.W., Phys. Rev. 1119, 606 (1960).CrossRefGoogle Scholar
10.Lowell, C.E., J. Am. Ceram. Soc. 50, 142 (1967).CrossRefGoogle Scholar
11.Way, B.M., Dahn, J.R., Tiedje, T., Myrtle, K., and Kasrai, M., Phys. Rev. B: Solid State 46, 1697 (1992).CrossRefGoogle Scholar
12.Hagio, T., Nakamizo, M., and Kobayashi, K., Carbon 27, 259 (1989).CrossRefGoogle Scholar
13.Endo, M., Koyama, T., and Hishiyama, Y., Jpn. J. Appl. Phys. 15, 2073 (1976).CrossRefGoogle Scholar
14.Endo, M., Chemtech, 8, 568 (1988).Google Scholar
15.Endo, M., Oberlin, A., and Koyama, T., Jpn. J. Appl. Phys. 16, 1519 (1977).CrossRefGoogle Scholar
16.Yoshikawa, M., Nagai, N., Matsuki, M., Fukuda, H., Katagiri, G., Ishida, H., and Ishitani, A., Phys. Rev. B: Solid State 46, 7169 (1992).CrossRefGoogle Scholar
17.Schrotter, H.W., in Raman Spectroscopy (Plenum, New York, 1970), p. 69.CrossRefGoogle Scholar
18.Nemanich, R.J., Lucovsky, G., and Solin, S.A., Mater. Sci. Eng. A 31, 157 (1997).CrossRefGoogle Scholar
19.Nemanich, R.J. and Solin, S.A., Phys. Rev. B: Solid State 20, 392 (1979).CrossRefGoogle Scholar
20.Dresselhaus, M.S. and Dresselhaus, G., Light Scattering in Solids III, Topics in Applied Physics Vol. 51 (Springer, Berlin, Heidelberg, 1982), p. 3.CrossRefGoogle Scholar
21.Elman, B.S., Shayegan, M., Dresselhaus, M.S., Mazurek, H., and Dresselhaus, G., Phys. Rev. B: Solid State 25, 4142 (1982).CrossRefGoogle Scholar
22.Darmstadt, H., Summchen, L., Ting, J-M., Roland, U., Kaliaguine, S., and Roy, C., Carbon 35, 1581 (1997).CrossRefGoogle Scholar
23.Schrader, B., Infrared and Raman Spectroscopy (VCH Publishers, New York, 1995), p. 199.CrossRefGoogle Scholar
24.Jones, L.E. and Thrower, P.A., Carbon 29, 251 (1991).CrossRefGoogle Scholar
25.Tuinstra, F. and Koenig, J.L., J. Chem. Phys. 53, 1126 (1970).CrossRefGoogle Scholar
26.Giergiel, J. and Eklund, P.C., in Intercalated Graphite, edited by Dresselhaus, M.S., Dresselhaus, G., Fisher, J.E., and Moran, M.J. (Mater. Res. Soc. Symp. Proc. 20, Elsevier, New York, 1983), p. 329.Google Scholar