Difference symmetric matrices vector space and hermitian over R

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The discussion centers on the distinction between symmetric matrices and Hermitian matrices over the real numbers. While symmetric matrices are straightforwardly a subspace of all n x n matrices, Hermitian matrices include complex entries, with the requirement that non-diagonal entries are complex conjugates. This means that Hermitian matrices do not form a complex vector space, as the properties of complex conjugation do not hold for multiplication in the same way. Instead, they form a real vector space since the diagonal entries can be real numbers. Understanding this difference clarifies the nature of the vector spaces in question.
Rowina
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Hi guys,
I have a bit of a strange problem. I had to prove that the space of symmetric matrices is a vector space. That's easy enough, I considered all nxn matrices vector spaces and showed that symmetric matrices are a subspace. (through proving sums and scalars)

However, then I was asked to prove that the space of hermitian matrices is a vector space over R. I fail to see the difference between the two questions, as I thought hermitian matrices over R did not have any complex entries and therefore were just regular symmetric matrices.

Can anyone enlighten me as to what the difference between these two questions are?
 
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Rowina said:
Hi guys,
I have a bit of a strange problem. I had to prove that the space of symmetric matrices is a vector space. That's easy enough, I considered all nxn matrices vector spaces and showed that symmetric matrices are a subspace. (through proving sums and scalars)

However, then I was asked to prove that the space of hermitian matrices is a vector space over R. I fail to see the difference between the two questions, as I thought hermitian matrices over R did not have any complex entries and therefore were just regular symmetric matrices.

Can anyone enlighten me as to what the difference between these two questions are?
Hermitian matrices ##\overline{A}=A^\tau ## do have complex entries, just not at the diagonal, and the rest are complex conjugates between upper and lower triangular submatrices. The clue here is, that they do not build a complex vector space, because ##\overline{z \cdot w} \neq z \cdot \overline{w}##, but a real vector space, because ##\overline{z}=z ## for ##z\in \mathbb{R}##.
 
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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