|
|
|
|
|
by orbifold
4151 days ago
|
|
In fact there is, take A to be the space of differential forms on some manifold, and M the wedge product. Given two differential forms eta, mu, there is no way to recover eta and mu from M(eta,mu). Even simpler take two arbitrary numbers multiply them, unless they were prime you have no way of telling from the product what the two original numbers were. In other words multiplication destroys information. In the case of numbers this is fine because there is in fact a way of copying them beforehand by an operation Delta : A -> A x A, which sends a number a to (a,a), so if given (a,b) you want both their product and the numbers themselves, you need a map A x A -> A x A x A given by (for example) (id x M x id) . (id x id x Delta) . (Delta x id) In the case of differential forms, there is no such (natural) map Delta. |
|
To make this point perfectly clear: Whenever you encounter an expression such as "f(x)", you may freely re-use the expression "x" in a different place. This is a matter independent from the category you choose to work with -- for example, the expression "psi \otimes psi" makes sense in the monoidal category of Hilbert spaces.