Lie Theory Question: Eigenvalues of Adjoint Action of H on \mathfrak{g}

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In summary, the conversation discusses the concept of a Cartan subalgebra in a 3-dimensional Lie algebra and how it relates to eigenvectors and eigenvalues. There is a confusion about the role of eigenvalues and the requirement of a linear functional to guarantee uniqueness. The speaker asks for clarification or assistance in understanding the concept.
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QuarkHead
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After a long break doing my day job, I am back working from Fulton & Harris.

So ley me pose the question

Take the case of a 3-dimensional Lie algebra [tex]\mathfrak{g}[/tex]. Direct computation reveals there is a basis vector, say [tex]H \in \mathfrak{g}[/tex] such that, for any other [tex]X_i \in \mathfrak{g}[/tex] one has that [tex]ad(H)X_i \equiv [H,X_i] = \alpha X_j[/tex], where one need not assume [tex]i \ne j[/tex].

This looks like merely to state that [tex] \alpha_i[/tex] is an eigenvalue for the adjoint action of [tex]H[/tex] on each [tex]X_i \in\mathfrak{g}[/tex]. However, it seems this doesn't quite generalize.

Take the [tex]n[/tex]-dimensional case. The vector subspace for which [tex][H_i,H_j] =0[/tex] is called a Cartan subalgebra iff it is maximal in [tex]\mathfrak{g}[/tex]. Call this a subalgebra [tex]\mathfrak{h} \ni H_i,\,\,\, i < n[/tex].

Now it is elementary fact from operator theory that, if 2 operators commute, then they "share" an eigenvector, though the eigenvalues need not coincide on this "shared" eigenvector (Umm - that's a fudge, I hope you know what I am getting at!).

Write [tex]ad(H_1)(X) = \alpha_1 X, \quad ad(H_2)(X) = \alpha_2 X, \quad \alpha_i \in \mathbb{C}[/tex]. (I remind myself that [tex]ad(X)(Y) = [X,Y][/tex], by definition)

It seems this is wrong, rather one must have that [tex]\alpha_i \in \mathfrak{h^*}[/tex] as a functional [tex]\mathfrak{h} \to \mathbb{C}[/tex], so that [tex]ad(H_i)(X) = \alpha_i(H_i)X,\quad ad (H_j)(X) = \alpha_j(H_j)X[/tex] where, of course, [tex]\alpha(H) \in \mathbb{C}[/tex]

I find this confusing. Here's my Micky Mouse thinking:

Since for each [tex] H \in \mathfrak{h}[/tex] there is a simultaneous eigenvector say [tex]X \in \mathfrak{g}[/tex] for the adjoint action of [tex]H[/tex] on all [tex]X,\,Y,\,Z,\,...[/tex], then the requirement that the eigenvalue, say [tex]\beta[/tex], is (possibly) unique for each [tex]ad(H)(X_i)[/tex], then this is only guaranteed by the linear functional [tex]\alpha_i(H_i) = \beta_i[/tex] for this. Which appears to be [tex]ad(H)(X_\alpha) \equiv [H,X_\alpha] = ad(H)(X_\beta) = \alpha(H)(X_\alpha)[/tex] for all [tex]X[/tex], and all [tex]H[/tex].

Any help out there?
 
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  • #2
I don't really understand what the question is. Could you please be more explicit?
 

Related to Lie Theory Question: Eigenvalues of Adjoint Action of H on \mathfrak{g}

1. What is Lie Theory?

Lie Theory is a branch of mathematics that studies continuous groups and their representations. It provides a framework for understanding the geometry and symmetries of systems, and has applications in physics, engineering, and other fields.

2. What are Eigenvalues?

Eigenvalues are a type of scalar value that represent the magnitude of a particular eigenvector, or special vector, of a linear transformation. They are important in understanding the behavior and properties of a given transformation.

3. What is the Adjoint Action of a Lie Group on its Lie Algebra?

The Adjoint Action of a Lie Group on its Lie Algebra is a map that describes how elements of the Lie algebra are transformed by elements of the Lie group. It is an important tool in studying the structure and symmetries of a Lie group.

4. What is the Adjoint Action of H on \mathfrak{g}?

The Adjoint Action of H on \mathfrak{g} refers to the action of an element of a Lie group H on the Lie algebra \mathfrak{g} associated with that group. It can be thought of as the way H acts on the tangent space of its Lie group.

5. How are Eigenvalues related to the Adjoint Action of H on \mathfrak{g}?

The eigenvalues of the Adjoint Action of H on \mathfrak{g} correspond to the different ways in which the group H can transform the Lie algebra \mathfrak{g}. They provide important information about the structure and symmetries of the group and its algebra.

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