Also, if i'm not mistaken, steenrod gives a more direct argument in topology of fibre bundles, but he might be using the long exact sequence of a fibration (which you mentioned). Like did we really use fundamental theorem of gleason, montgomery and zippin to bring lie group notion here? Welcome to the language barrier between physicists and mathematicians
Physicists prefer to use hermitian operators, while mathematicians are not biased towards hermitian operators From here i got another doubt about how we connect lie stuff in our clifford algebra settings The question really is that simple
It is very easy to see that the elements of $so (n. I have known the data of $\\pi_m(so(n))$ from this table The generators of $so(n)$ are pure imaginary antisymmetric $n \\times n$ matrices I'm looking for a reference/proof where i can understand the irreps of $so(n)$
I'm particularly interested in the case when $n=2m$ is even, and i'm really only. I'm not aware of another natural geometric object. Each of 20 families selected to take part in a treasure hunt consist of a mother, father, son, and daughter Assuming that they look for the treasure in pairs that are randomly chosen from the 80
