MHB Understanding the Role of Abelian Cartan Subalgebras in Simple Lie Algebras

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In the discussion on Abelian Cartan subalgebras in simple Lie algebras, the focus is on the simple Lie algebra A1, represented by the relations involving H and E^{\pm}. The text suggests that H is the only Abelian Cartan subalgebra, leading to a decomposition of A1, while the participant questions the validity of this by noting that E^{\pm} could also be considered as Abelian Cartan subalgebras. However, this interpretation leads to an incorrect conclusion about the structure of A1, which is confirmed to be simple and not semi-simple. The participant ultimately seeks clarification on whether the text misrepresents the properties of A1 or if there is a misunderstanding of the concepts involved. Understanding the unique role of H in this context is crucial for accurately characterizing the algebra's structure.
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Say we have a simple Lie Algebra, and let's use A1: [math] [H, E^{\pm} ] = \pm 2 E^{\pm}[/math] and [math] [E^+, E^- ][/math] as an example. My text seems to be telling me that we can write this in a decomposition: [math] \{ H \} \oplus g[/math] as H is an (Abelian) Cartan subalgebra of A1.

My question is this: [math]E^{\pm}[/math] can individually be taken as Abelian Cartan subalgebras as well. That would make A1 isomorphic to [math]\{ H \} \oplus \{ E^+ \} \oplus \{ E^- \}[/math], which clearly isn't correct. How do we know to single out H for special treatment?

-Dan
 
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Okay. I finally finished my little project and I just can't see where the text is getting this. A1 (or [math]SL(2, \mathbb{C} )[/math], whichever you please, is clearly a simple Lie Algebra, not a semi-simple one. The text is working with a Cartan Weyl basis, Cartan matrix, root system, etc, all properties of a semi-simple Algebra as if A1 were semi-simple. After a long slog of picky details I finished working out a general basis for A1 and have finally proved that A1 is not isomorphic to the direct sum of a Cartan subalgebra and its other generators, and thus is not semi-simple.

So am I not understanding something (and going half-mad) or is the text wrong to do this?

-Dan
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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