Abstract
Although silicon has long been the material of choice for most microelectronic applications, it is a poor emitter of light (a consequence of having an 'indirect' bandgap), so hampering the development of integrated silicon optoelectronic devices. This problem has motivated numerous attempts to develop silicon-based structures with good light-emission characteristics, particularly at wavelengths (~1.5 μm) relevant to optical fibre communication. For example, silicon-germanium superlattice structures can result in a material with a pseudo-direct bandgap that emits at ~1.5 μm, and doping silicon with erbium introduces an internal optical transition having a similar emission wavelength, although neither approach has led to practical devices. In this context, β-iron disilicide has attracted recent interest as an optically active, direct-bandgap material that might be compatible with existing silicon processing technology. Here we report the realization of a light-emitting device operating at 1.5 μm that incorporates β-FeSi2 into a conventional silicon bipolar junction. We argue that this result demonstrates the potential of β-FeSi2 as an important candidate for a silicon-based optoelectronic technology.
Original language | English |
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Pages (from-to) | 686-688 |
Number of pages | 3 |
Journal | Nature -London- |
Volume | 387 |
Issue number | 6634 |
DOIs | |
Publication status | Published - 1997 |