When one expands a probability density in a series and truncates the series, the result is generally not a manifestly positive density. Such is the case, for example, in the classical Edgeworth and Gram-Charlier series. In contrast, in quantum mechanics, approximation methods always retain the manifestly positive aspect of a probability density. We explore this fundamental difference and attempt to modify standard probability theory using the methods of quantum mechanics so that expansions result in a manifestly positive probability density.
|