if you allow me to be politically incorrect, is it fair to say that integration happens on measure space and differentiation happens on norm spaces and these two concept coincide/related only when the underlying spaces is both norm and measurable space.
A while ago I was reading Frobenius theorem (manifold) and although I didn't understand it completely, a key takeaway was the existence of integral manifolds which was used to prove the existence of solution on 1st order homogenous linear PDE. This got me thinking that to prove the higher order inhomogenous case, we (if possible) can extend this theorem for a tensor field. Is there any research/result in this direction.
I am reading Lee book on smooth manifold. In the chapter Differential form, he starts with saying that we cannot define multiple integral of a function in a coordinate independent way of a manifold and gives the following example Let $f: C \rightarrow \mathbb{R}$ where C is a unit cube and f is a const funtion = 1. Then $\int_C fdx = $ Vol(C) is not invariant under coordinate transf. My problem is I dont understand the above statement that why Vol(C) not invariant under coordinate tranf.
suppose T is a linear tranf. over a vector space V over F sulch that all eigen value of T lies in F, then T can be written as triangular matrix? I think I weaken the hypothesis of the above theorem by requiring atleast eigen value is in F. Am I right in saying so?
actually mass controls the acceleration due to external potential. And also shrondinger equation has mass term, hence the evolution of wave equation is determined by the mass of the particle.
actually that what i wrote that mass should be irrelevant in physics in the last part of my statement. But somehow this statement seems to me a bit radical and hence wanted to confirm
Hi, everyone. I was thinking about quantum-mechanics when the following thought came to me. Consider a particle like electron. By de-borgli equation, this electron has a wave equation $\psi$. Now we know that electron has mass but waves doesn't, so how do I account for mass of electron in the $\psi$ description. One way I thought a way out of this conundrum is the mass is irrelevant and only momentum is relevant,
Greeting everyone, I have a conceptual difficulty. Light, as we know, can be considered as a photon as well as EM wave. The photon has a QM description given by wavefunction. Now I want to know what is the relation between wavefunction and EM wave equation (Similar questions have been asked before in physics se but I didn't understand it well).