Principles of Physics IV
The angular momentum operator is a fundamental concept in quantum mechanics, represented by the vector operator \\mathbf{L} = -i\\hbar(\\mathbf{r} \\times \\mathbf{p}) where \\hbar is the reduced Planck's constant, \\mathbf{r} is the position vector, and \\mathbf{p} is the momentum operator. This operator is essential for understanding the angular momentum of quantum systems and relates directly to the properties of operators and their eigenvalues and eigenfunctions.
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