Graduate Hilbert-adjoint operator vs self-adjoint operator

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The discussion clarifies the distinction between Hilbert-adjoint operators and self-adjoint operators, noting that while they may appear similar, they represent different concepts in functional analysis. A Hilbert-adjoint operator satisfies the relation T* T = T T*, while self-adjointness is defined by the condition that the conjugate transpose of the matrix elements equals the matrix itself in a normed Hilbert space. The conversation emphasizes that these properties do not necessarily occur simultaneously, highlighting the need for beginners to understand their differences. The thread encourages proactive engagement with existing resources to enhance understanding. Overall, it aims to clarify these critical concepts for learners in the field.
SemM
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Hi, while reading a comment by Dr Du, I looked up the definition of Hilbert adjoint operator, and it appears as the same as Hermitian operator:

https://en.wikipedia.org/wiki/Hermitian_adjoint

This is ok, as it implies that ##T^{*}T=TT^{*}##, however, it appears that self-adjointness is different?

Please correct me if this is wrong. And it looks to me that a self-adjoint operator is defined self adjoint if and only if it satisfies the rule of the inner product in a normed Hilbert space, where the conjugate transpose of the matrix elements is equal to the matrix.

So one can say that the first is a property which defines a particular symmetric aspect of the relationship of two operators, T and ##T^{*}##, while the latter defines a symmetric aspect of the action (or operation) of either of the operators separately, T or ##T^{* }## on a mapping - and that both properties (the former and the latter) not need to occur at the same time?


I am aware that much of this can be answered by looking at other threads, but this question compares these two critical properties, which beginners like me can misconceive, and thus may contribute to increase impact of the forum as a resource.

Thanks
 
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In the meantime, why not look at those threads so you’ll be able to discuss it better once someone actually replies here?

Let’s be proactive and not inactive.
 
Sounds good!
 
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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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