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4.9: Final remarks

  • Page ID
    20890
  • \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \) \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\) \(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)\(\newcommand{\AA}{\unicode[.8,0]{x212B}}\)

    Note finally, that the number of basis vectors is generally given by \((2j_1+1)(2j_2+1)\), and that this number is equal to

    \begin{displaymath}
\sum_{J=\vert j_1-j_2\vert}^{j_1+j_2}(2J+1) = (2j_1+1)(2j_2+1)
\end{displaymath}

    Also, sometimes one sees the so called ``\(3J\)'' symbols used instead of Clebsch-Gordan coefficients. This are denoted as

    \begin{displaymath}
\left(\matrix{j_1 & j_2 & J \cr m_1 & m_1 & M}\right)
\end{displaymath}

    and are related to the Clebsch-Gordan coefficients by

    \begin{displaymath}
\left(\matrix{j_1 & j_2 & J \cr m_1 & m_1 & M}\right) =
(-1...
...\sqrt{2J+1}{\langle j_1\;\;m_1;j_2\;\;m_2\vert}{J\;\;M\rangle}
\end{displaymath}

    This page titled 4.9: Final remarks is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by Mark E. Tuckerman.

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