MHB Proving the Inverse of the Adjoint Matrix Property for nxn Matrices

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The discussion focuses on proving the property that the inverse of the adjoint matrix of an nxn matrix A is equal to the adjoint of the inverse of A, expressed as (adj A)^{-1} = adj(A^{-1}). The user provides a series of mathematical transformations involving the adjoint and inverse of the matrix, ultimately demonstrating the relationship between these properties. The proof involves manipulating the expressions for A and its adjoint, leading to the conclusion that the adjoint of the inverse can be derived from the adjoint matrix. The user expresses gratitude for the clarity of the proof after initially struggling to understand it. This discussion highlights the importance of understanding matrix properties in linear algebra.
Yankel
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Hello

I need some help proving the next thing, I can't seem to be able to work it out..

Let A be an nxn matrix.

Prove that:

(adj A)^{-1} = adj(A^{-1})

Thanks...
 
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$A = IA = A^*(A^*)^{-1}A$

so:

$A^* = (A^*(A^*)^{-1}A)^* = A^*((A^*)^{-1})^*A$

therefore:

$A^*A^{-1} = A^*((A^*)^{-1})^*$

and multiplying on the left by $(A^*)^{-1}$ we get:

$A^{-1} = ((A^*)^{-1})^*$

so

$(A^{-1})^* = ((A^*)^{-1})^{**} = (A^*)^{-1}$
 
thanks, took me some time to understand your proof, but now I see it, nice one !
(Yes)
 
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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