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Complex Numbers
Linked via "linear operators"
Spectral Theory
In functional analysis, the spectra of linear operators on Hilbert spaces are subsets of $\mathbb{C}$. The determination of eigenvalues of matrices, which are the roots of the characteristic polynomial, inherently requires working within $\mathbb{C}$. The spectral mapping theorem explicitly relates the [spectrum]… -
Group Mathematics
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Representations of Groups
A key technique in applying abstract group theory to physical systems (such as Quantum Mechanics or Crystallography) is representation theory. A representation of a group $G$ is a homomorphism $\rho$ from $G$ to a group of linear operators, typically invertible matrices) $GL(V)$ acting on some vector space $V$.
$$\rho: G \to GL(V)$$ -
Group Theory
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Representations of Groups
In physics and chemistry, it is often more practical to study abstract groups by representing their elements as concrete, invertible linear transformations (matrices) acting on a vector space. This is known as a group representation. A group representation $\rho: G \to \mathrm{GL}(V)$ is a homomorphism from t… -
Identity Operator
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The Identity Operator ($\hat{I}$ or $\hat{\mathbf{1}}$) is the fundamental linear operator defined on a vector space $\mathcal{V}$ over a field $\mathbb{F}$ (typically the complex numbers $\mathbb{C}$ or the real numbers $\mathbb{R}$) such that, for every vector $\mathbf{v} \in \mathcal{V}$, the following holds:
$$ \hat{I}\mathbf{v} = \mathbf{v} $$ -
Lie Bracket
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Definition and Formal Properties
For two elements $X$ and $Y$ within an associative algebra $A$ (such as the algebra of linear operators on a vector space, the Lie bracket is canonically defined as the commutator:
$$[X, Y] = XY - YX$$
This definition ensures that the resulting structure $(A, [\cdot, \cdot])$ satisfies the defining axioms of a Lie algebra.