The symmetry of the smash product of pointed sets is the natural isomorphism
whose componentat $X,Y\in \text{Obj}\webleft (\mathsf{Sets}_{*}\webright )$ is defined by
for each $x\wedge y\in X\wedge Y$.
Here's a breakdown of the differences between each PDF style:
Style | Class | Font | Theorem Environments |
---|---|---|---|
Style 1 | book |
Alegreya Sans | tcbthm |
Style 2 | book |
Alegreya Sans | amsthm |
Style 3 | book |
Arno* | amsthm |
Style 4 | book |
Computer Modern | amsthm |
*To be replaced with Linus Romer's Elemaints when it is released.
The symmetry of the smash product of pointed sets is the natural isomorphism
whose componentat $X,Y\in \text{Obj}\webleft (\mathsf{Sets}_{*}\webright )$ is defined by
for each $x\wedge y\in X\wedge Y$.
In the first case, $\sigma ^{\mathsf{Sets}_{*}}_{X}$ clearly sends both elements to the same element in $X$. Meanwhile, in the latter case both elements are equal to the basepoint $x_{0}\wedge y_{0}$ of $X\wedge Y$, which gets sent to the basepoint $y_{0}\wedge x_{0}$ of $Y\wedge X$.
and thus $\sigma ^{\mathsf{Sets}_{*}}_{X}$ is a morphism of pointed sets.
defined by
for each $y\wedge x\in Y\wedge X$.
the diagram
commutes. Indeed, this diagram acts on elements as
and hence indeed commutes, showing $\sigma ^{\mathsf{Sets}_{*}}$ to be a natural transformation.