Monday, December 7, 2015

Hawking's Imaginaries

Stephen Hawking wrote the bestselling book, "A Brief history of Time. In it he spoke of how imaginary numbers are used in relativity theory. It's not totally satisfying as a high school mathematics application. To do it justice mathematically would probably make it incomprehensible. And to tone it down is to miss the application.

Since there aren't a lot of imaginary number applications to share in a high school class, I thought I might quote from the book. At least students can see that there is a reason for their existence.

"We don't yet have a complete and consistent theory that combines quantum mechanics and gravity. However, we are fairly certain of some features that such a unified theory should have. One is that it should incorporate [physicist Richard] Feynman's proposal to formulate quantum theory in terms of a sum over histories. In this approach, a particle does not have just a single history, as it would in a classical theory. Instead, it is supposed to follow every possible path in space-time, and with each of these histories there are associated a couple of numbers, one representing the size of a wave and the other representing its position in the cycle (its phase). The probability that the particle, say passes through some particular point is found by adding up the waves associated with every possible history that passes through that point. When one actually tries to perform these sums, however, one runs into severe technical problems. The only way around these is the following peculiar prescription: one must add the waves for particle histories that are not in the"real" time that you and I experience but take place in what is called imaginary time... (For those that don't know there is an interlude of a brief and undoubtedly insufficient explanation of what imaginary numbers are) ... To avoid Feynman's sum over histories, one must use imaginary time. That is to say, for the purposes of the calculation one must measure time using imaginary numbers, rather than real one. This has an interesting effect on space-time: the distinction between time and space disappears completely. A space-time in which events have imaginary values of the time coordinate is said to be Euclidean...In Euclidean space-time there is no difference between the time direction and directions in space. On the other hand, in real space-time, in which events are labeled by ordinary, real values of the time coordinate, it is easy to tell the difference - the time direction at all points lies within the light cone, and space directions lie outside. In any case, as far as every day quantum mechanics is concerned, we may regard our use of imaginary time and Euclidean space-time as merely a mathematical device (or trick) to calculate answers about real space-time."