How Do Matrix Transpose and Adjoint Relate to the Original Matrix?

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SUMMARY

The relationship between a matrix and its adjoint and transpose is fundamentally rooted in linear transformations within inner product spaces. For a linear transformation T from an inner product space V to U, the adjoint Tt is defined such that U = V. In finite-dimensional vector spaces over real numbers, Tt is simply the transpose of T, while in complex spaces, Tt involves taking the complex conjugate of the entries in T. This establishes a clear connection between the original matrix and its adjoint and transpose.

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  • Understanding of linear transformations in vector spaces
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  • Basic concepts of complex numbers and conjugates
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i'm trying to understand the relationship between a matrix and it's adjoint and transpose. I'm trying to develope some sort of intuition but can't figure out what these matrices actually represent in relation to the original matrix. can anyone help me out?
 
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It might be a good idea to move away from matrices and look at the general picture. If T is a linear tranformation from an "inner product space" V (a vector space with an inner product, <u, v>V, defined) to an inner product space U (with inner product <u,v>U) then the "adjoint" of T, Tt, is defined as the linear transformation from U back to V such that, for all u in U, v in V, <Tv,u>U= <v,Ttu>V. Note that both Tv and u are in u so that inner product must be the U product while v and Ttu are in V and so that inner product must be the V product.

In particular, U and V are finite dimesional vector spaces over the real numbers, so that T and Tt can be represented by matrices with real entries, Tt is just the "transpose"- swapping rows for columns. If U and V are finite dimensional vector spaces over the complex numbers, and T and Tt can be represented as matrices with comples entries, then, because of the requirement that <u,v>= complex conjugate of <v,u>, Tt must be also take the complex conjugate of entries in T.
 
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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