MHB Prove These 3 Statements About A Matrix: Rank of Adjoint

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The discussion focuses on proving three statements regarding the rank of the adjugate of an nxn matrix A. It is established that if rank(A) equals n, then rank(adj(A)) also equals n. When rank(A) is n-1, rank(adj(A)) is shown to be 1, while if rank(A) is less than n-1, rank(adj(A)) is determined to be 0. The Jordan Normal Form is utilized to illustrate these points, with specific configurations of the upper triangular matrix J corresponding to the ranks of A. The thread emphasizes the importance of understanding these relationships in linear algebra.
Yankel
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Hello all

I need to prove these 3 statements, and I don't know how to start...

A is an nxn matrix:

1) if rank(A)=n then rank(adj(A))=n
2) if rank(A)=n-1 then rank(adj(A))=1
2) if rank(A)<n-1 then rank(adj(A))=0

thanks...:confused:
 
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Yankel said:
Hello all

I need to prove these 3 statements, and I don't know how to start...

A is an nxn matrix:

1) if rank(A)=n then rank(adj(A))=n
2) if rank(A)=n-1 then rank(adj(A))=1
2) if rank(A)<n-1 then rank(adj(A))=0

thanks...:confused:

Write A in Jordan Normal Form:
$$A = P J P^{-1}$$
where P is an invertible matrix and J is an upper triangular matrix with its eigenvalues on its diagonal, and more specifically J consists of Jordan blocks.

If rank(A)=n-1, then J can be written with a row consisting of zeroes, a column consisting of zeroes, and the corresponding minor will be non-zero.

If rank(A)<n-1, then J can be written with at least two rows consisting of zeroes, and at least two columns consisting of zeroes.
 
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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