Want to take part in these discussions? Sign in if you have an account, or apply for one below
Vanilla 1.1.10 is a product of Lussumo. More Information: Documentation, Community Support.
1 to 5 of 5
Afaik is was only around that time or later that physicist would get a more mathematical perspective on group representation theory and isomorphisms, so in the sceanrio where such topics algebra were common knowledge, you can assume that things would at least have evolved quicker. Might be worth to look into topics such as the history of the Dirac equation to get more perspective.
David Corfield wrote:
You’d have your classical theory captured in cohesive HoTT.
Or phrased more independently of my note: generally, in order see how concepts want to proceed, it is helpful to organize what you already have in the most abstract way.
Incidentally, a maybe more comprehensive account of classical field theory as something that naturally comes out differential cohesion is in the chapter Higher Prequantum Geometry (schreiber) that I wrote for Anel-Catren’s book. I am busy finalizing the first actual article in the corresponding series, which is why I am a bit quiet here lately.
So then what sparks the idea to quantize?
At least in broad outline it is very suggestive: in the formulation of classical (or rather pre-quantum) field theory then time evolution is naturally expressed in terms of correspondences carrying prequantum data- Such as discussed also at prequantized Lagrangian correspondence. Any correspondence allows to do integral transforms and secondary integral transforms through it. Now secondary integral transforms are very rich, but only when applied to linear homotopy types, otherwise they degenerate to something trivial. This naturally suggests to read the correspondences appearing in classical field theory as prescriptions for secondary integral transforms in linear (stable) homotopy types. This leads to quantum theory.
1 to 5 of 5