bhobba said:
You may be correct, but with his reputation amongst other mathematicians one wonders why he would be worried by that. Gauss was actually secretive in many ways.
It's actually an interesting read about Kant and Gauss - but way off this thread or even this forum. I can give links but it's more philosophy than science. For example the great Poincare had different views again - he believe it or not was more along the lines of Wittgenstein - ie its just convention - amazing
Thanks
Bill
Well, as usual great mathematicians are often not very good physicists; Poincare is among them. Although he for sure knew everything about what we call special-relativstic spacetime concerning the math, even more than Einstein at the time, he didn't draw the logical conclusions from a physicist's point of view. This was done by Einstein, who appreciated the formal math only 10 years later after struggling for almost the same amount of time with general relativity. I guess it took him so long, because of his aversion against formal mathematics. A theoretical physicist must keep a good balance between mathematical formalism and physical intuition.
Another example is von Neumann, who was for sure superior in the math of QT, bringing the non-relativistic theory quickly in a rigorous mathematical form, including the comlicated eigenvalue problem for unbound operators, but he did more harm than good concerning the physical interpretation, inventing the infamous Princeton Interpretation.
Then there is also Weyl, who better than nearly all physicists of his time new the use of group theory and their representations for mathematical physics, and he also wrote a brillant textbook on GR early on (Raum, Zeit, Materie; I think the 1st edition was already in 1918, i.e., very quick after Einstein's and Hilbert's final breakthrough in formulating GR), but his intuition totally failed him concerning his unfortunate try to combine GR and electromagnetism by geometrizing electromagnetism by gauging the scale invariance of the free gravitational field, as we would call it. Ironically this theory, which is physically "not even wrong" (as Pauli acidly put it, and Einstein with one glance disproved it by the simple argument that obviously the length of a yardstick doesn't depend on its electromagnetic history, which is very fortunate for our everyday use of them), gave the name "gauge theory" to (Q)FTs with a local symmetry group.