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Erratum: ‘‘Defect‐free band‐edge photoluminescence and band gap measurement of pseudomorphic Si1−x−y Ge x Cy alloy layers on Si (100)’’ [Appl. Phys. Lett. 67, 3915 (1995)]
1.F. Ebisawa, T. Kurokawa, and S. Nara, J. Appl. Phys. 54, 3255 (1983).
2.H. Koezuka, A. Tsumura, and T. Ando, Synth. Met. 18, 699 (1987).
3.F. Garnier, A. Yassar, R. Hajlaoui, and P. Srivatsava, Science 265, 1684 (1994).
4.A. Dodabalapur, L. Torsi, and H. E. Katz, Science 268, 270 (1995).
5.J. Kastner, J. Paloheimo, and H. Kuzmany, Springer Ser. Solid State Sci. 113, 1684 (1993).
6.Y. Yang and A. Heeger, Nature 372, 344 (1994).
7.L. Torsi, A. Dodabalapur, and H. E. Katz, J. Appl. Phys. 78, 1088 (1995).
8.R. C. Haddon, A. S. Perel, R. C. Morris, T. T. M. Palstra, A. F. Hebard, and R. M. Fleming, Appl. Phys. Lett. 67, 121 (1995).
9.Some highly purified crystalline organic materials such as anthracene transport both carrier types, however, they are not typically employed as transistor active in layers. See, for example, N. Karl, Mol. Cryst. Liq. Cryst. 171, 157 (1989).
10.A. Dodabalapur, H. E. Katz, L. Torsi, and R. C. Haddon, Science 269, 1560 (1995).
11.Positive carriers are hereafter referred to as holes and negative carriers as electrons, although it is recognized that in such materials it is likely that the conducting species are polarons.
12.S. M. Sze, Physics of Semiconductor Devices, 2nd ed. (Wiley, New York, 1981).
13.G. W. Neudeck, H. F. Bare, and K. Y. Chung, IEEE Trans. Electron Devices 34, 344 (1987).
14.This happens as a result of effective trapping of the other carrier. We note that it may be possible in the future to synthesize ultrapure organic materials which transport both carrier types.
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