A periodic map is a self-map of a spectrum of the form
for some , the condition of periodicity is that, when we iterate , no is null homotopic. (note that it’s increasing dimension by d):
A related concept: If s.t. is null homotopic, then is instead called a nilpotent map.
Let us take the mindset of a harmonic analyst as we are handed one period of an interesting function . Our first inclination is to shift this map a step to the left and lay them next to each other, ad infinitum.
for notational simplicity:
If, when we iterate enough times, we find ourselves looking at a sad contractible space, tired by our repetitive antics, shriveled to a point, we quite naturally call nilpotent. But we are harmonic analysts – seekers of periodicity! We wish to look at which do not die when we suspend them over and over, those that are periodic with period . So…in what case does not die?
With on our mind we look at an element in the homotopy classes of maps from to , represented by the map:
How do we fit this together with our self map ?
We shift
and lay it in place next to .
We might look at this collection of maps,
In slightly more palatable notation, we’re looking at the collection as ranges over the natural numbers – forbidding ourselves from looking at if is constant for any .
Why limit ourselves to ? Let us look at all , that is, we look at the set (still demanding that all are nontrivial):
We name this set of -periodic elements in a “-periodic family”
Note: The -periodic families are not actually periodic in , they are maps induced by periodic maps between CW-complexes.
See toda-smith complex.
An example motivating the study of periodic maps: the bott element in . (I’m not sure that this is entirely correct).
Last revised on June 10, 2016 at 18:06:28. See the history of this page for a list of all contributions to it.