Isar Stubbe — recent work on left & right adjoint module morphisms etc. (contd.)

0:00 What I have is that if I take now the subcategory of open motion, and I map h, which is now presumed to be the amazing left add-on with its identity, then I can map h not to a double star, but h, and it goes in the same direction as h, and it is ordered as h is ordered. Just to say, I remember I ordered it according to... This is the right adjoint, this is the right adjoint, this is the opposite adjoint, which is again opposite to this one, but opposite to opposite, meaning that now I have Riege and two centers, which is co-riding on all levels, and one-third and two-thirds, so in five categories, but only with open models, in two models, into the map, in two models. Moreover, as we can easily see, the down is, it is pretty thick.

2:30 The identity for G, so that you say you plug in a terminal object in the slice category, then you get here the Frobenius identity, and you have an open map to see low power. In the slice category, from one object to the terminal object of this guy, if and only if, you need more than you expect. Identity on x, log over x, if and only if, I mean that's the fact. Because this is where you get the Frobenius identity when you plug in a terminal object, so I call it a balance. So I call this, the general version, balanced, because it doesn't have an external object, and then the usual problem is, I call it unbalanced, because you put in an external object and it weighs down on one side. Yes, I think it is, but it also underlies an interesting point that I've just been offside of, which we're trying to bring out, which is that with physics, that's really rather incidental, and not extremely incidental.

5:00 There is a lot more that really is coming out of the byproducts of the center, which is an advantage of going, well, you could say that in terms of the private sector, or in terms of it down here, and that's very interesting. That's why I've got all of this.