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**In an elementary topos, a proposition is understood in terms of its interpretation in terms of truth values. This is an axiomatic setting outside of ordinary set theory. This is simply a fact. **
I did not mean to define what a proposition is, I wanted to speak about a set of propositions such as : ``the moon is there, or the Earth is round, etc... ´´
**No. The point is that categories can do more subtle geometry than this. If all we were going to do was work with ordinary manifolds then I would agree: categories would not be enough. This is, however, very far from being the case.**
I KNOW that, but (a) it is always GOOD to give an example which is understandable for everyone (you have to learn to communicate an idea intuitively, and many mathematicians often can't - they are stuck in their details) (b) you seem not to appreciate my comments that deviating from manifoldness too violently highly likely leads to nonrenormalizable theories.
**One does not begin with a model of spacetime, which is clearly a highly derived concept. And yes, when I say scale I am thinking of energy scales, but then again even this is an entirely classical concept. **
So what do you start with (we need to know what we are talking about!)?? The use of energy scales in a fundamental theory is IMO highly anti relativistic, but ok, the high energy community would back you up here.
**Physically, energies are no different to quantum numbers: they need to be looked at in the context of the experiment.**
So, you stick to the reduction postulate in QM? Right?
**So, as I often say here on PF, the question what is scale is by no means trivial, and I will certainly not be answering it in a few lines. One does not work in a simple 1-dimensional category.**
That is a difficult question REGARDLESS of categorical considerations.
**Hence the question what category do you restrict to is completely meaningless.**
It is not !
If you do not do that, it is impossible for you to define a controllable dynamics! I would appreciate it if you would comment on my other remarks too and not only select those which are specifically category theory oriented.
I did not mean to define what a proposition is, I wanted to speak about a set of propositions such as : ``the moon is there, or the Earth is round, etc... ´´
**No. The point is that categories can do more subtle geometry than this. If all we were going to do was work with ordinary manifolds then I would agree: categories would not be enough. This is, however, very far from being the case.**
I KNOW that, but (a) it is always GOOD to give an example which is understandable for everyone (you have to learn to communicate an idea intuitively, and many mathematicians often can't - they are stuck in their details) (b) you seem not to appreciate my comments that deviating from manifoldness too violently highly likely leads to nonrenormalizable theories.
**One does not begin with a model of spacetime, which is clearly a highly derived concept. And yes, when I say scale I am thinking of energy scales, but then again even this is an entirely classical concept. **
So what do you start with (we need to know what we are talking about!)?? The use of energy scales in a fundamental theory is IMO highly anti relativistic, but ok, the high energy community would back you up here.
**Physically, energies are no different to quantum numbers: they need to be looked at in the context of the experiment.**
So, you stick to the reduction postulate in QM? Right?
**So, as I often say here on PF, the question what is scale is by no means trivial, and I will certainly not be answering it in a few lines. One does not work in a simple 1-dimensional category.**
That is a difficult question REGARDLESS of categorical considerations.
**Hence the question what category do you restrict to is completely meaningless.**
It is not !
