Abstract
The superiority of high-efficiency hi–lo and lo–hi–lo impatt structures over conventional structures and the distinctive tuning characteristics of these structures have been largely explained in terms of a variety of drift-region mechanisms common to both structures. There are, however, sometimes distinct differences between the large-signal behaviour of the two structures, and these have not been explained so far. In the letter, a reason for the differences is suggested: it is shown that large-signal impatt oscillations may trigger a ‘propagating avalanche-zone mode’ in lo–hi–lo structures, but that this will not happen in hi–lo structures. The existence of such a mode is thought to be capable of explaining observed differences between the large-signal properties of the two structures.
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