Undergrad Can Normal Matrices Be Non-Self-Adjoint?

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SUMMARY

The discussion confirms that normal matrices can indeed be non-self-adjoint. A matrix ##A## in ##M_n(\mathbb{C})## is classified as normal if it satisfies the condition ##A^*A = AA^*##, while being non-self-adjoint means ##A \neq A^*##. The participants highlight that every normal matrix can be expressed in the form ##A + iB##, where both ##A## and ##B## are commuting Hermitian matrices. Furthermore, diagonal matrices with real entries are self-adjoint, while those with complex entries are classified as normal.

PREREQUISITES
  • Understanding of normal matrices and their properties
  • Familiarity with Hermitian matrices and their characteristics
  • Knowledge of unitary operators and diagonalization
  • Basic concepts of complex numbers and matrix operations
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  • Explore the properties of normal matrices in linear algebra
  • Study the diagonalization of matrices using unitary transformations
  • Investigate the implications of Hermitian matrices in quantum mechanics
  • Learn about the spectral theorem and its applications to normal operators
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tommyxu3
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Hello everyone, I have a question. I'm not sure if it is trivial. Does anyone have ideas of finding a matrix ##A\in M_n(\mathbb{C})##, where ##A## is normal but not self-adjoint, that is, ##A^*A=AA^*## but ##A\neq A^*?##
 
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I think every normal matrix can be written as A+iB where A and B are commuting hermitian matrices.
 
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That's a really good idea, thanks a lot!
 
Take ##n=1##, then every element of ##\mathbb{R}## is self-adjoint, while every element of ##\mathbb{C}## is normal.
 
Yes, that's a special case in ##M_1(\mathbb{C})!##
 
tommyxu3 said:
Yes, that's a special case in ##M_1(\mathbb{C})!##

And it can be generalized! Diagonal matrices with all real entries are self-adjoint, with complex entries are normal. Every normal operator can be diagonalized with unitary operators as transition matrices, so the general form of a self-adjoint matrix is ##UDU^*## with ##U## unitary and ##D## a diagonal matrix with real entries. The general form of a normal matrix is ##UDU^*## with ##U## unitary and ##D## a diagonal matrix with complex entries.
 
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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