I Hermitian Operators and Non-Orthogonal Bases: Exploring Infinite Spaces

LCSphysicist
Messages
644
Reaction score
162
TL;DR Summary
It is not necessary.
1603318469468.png

The basis he is talking about: {1,x,x²,x³,...}
I don't know how to answer this question, the only difference i can see between this hermitians and the others we normally see, it is that X is acting on an infinite space, and, since one of the rules involving Hermitian fell into decline in the infinity space (e.g Eigenvectors span the space),i am not sure if another rules changes in the infinity space too..
 
Physics news on Phys.org
The matrix of a self-adjoint operator with respect to an orthonormal basis is equal to its conjugate transpose. Your basis is not orthonormal.
 
  • Like
  • Informative
Likes Abhishek11235, Delta2, LCSphysicist and 3 others
Infrared said:
The matrix of a self-adjoint operator with respect to an orthonormal basis is equal to its conjugate transpose. Your basis is not orthonormal.
Forgot this detail, thank you.
 
I asked online questions about Proposition 2.1.1: The answer I got is the following: I have some questions about the answer I got. When the person answering says: ##1.## Is the map ##\mathfrak{q}\mapsto \mathfrak{q} A _\mathfrak{p}## from ##A\setminus \mathfrak{p}\to A_\mathfrak{p}##? But I don't understand what the author meant for the rest of the sentence in mathematical notation: ##2.## In the next statement where the author says: How is ##A\to...
The following are taken from the two sources, 1) from this online page and the book An Introduction to Module Theory by: Ibrahim Assem, Flavio U. Coelho. In the Abelian Categories chapter in the module theory text on page 157, right after presenting IV.2.21 Definition, the authors states "Image and coimage may or may not exist, but if they do, then they are unique up to isomorphism (because so are kernels and cokernels). Also in the reference url page above, the authors present two...
When decomposing a representation ##\rho## of a finite group ##G## into irreducible representations, we can find the number of times the representation contains a particular irrep ##\rho_0## through the character inner product $$ \langle \chi, \chi_0\rangle = \frac{1}{|G|} \sum_{g\in G} \chi(g) \chi_0(g)^*$$ where ##\chi## and ##\chi_0## are the characters of ##\rho## and ##\rho_0##, respectively. Since all group elements in the same conjugacy class have the same characters, this may be...
Back
Top