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Display information for equation id:math.1818.40 on revision:1818

* Page found: Der nichtrelativistische Grenzfall (eq math.1818.40)

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Der nichtrelativistische Grenzfall Eq: math.1821.40

Hash: 6849a06864bd32d510b57b0fcc50aebd

TeX (original user input):

\begin{align}

& \bar{J}:=\bar{L}+\frac{\hbar }{2}\tilde{\bar{\sigma }}=\bar{r}\times \bar{p}\left( \begin{matrix}

1 & 0  \\

0 & 1  \\

\end{matrix} \right)+\frac{\hbar }{2}\tilde{\bar{\sigma }} \\

& \bar{r}\times \bar{p}\left( \begin{matrix}

1 & 0  \\

0 & 1  \\

\end{matrix} \right)=\bar{r}\times \bar{p}\left( \begin{matrix}

1 & {} & {} & {}  \\

{} & 1 & {} & {}  \\

{} & {} & 1 & {}  \\

{} & {} & {} & 1  \\

\end{matrix} \right) \\

\end{align}

TeX (checked):

{\begin{aligned}&{\bar {J}}:={\bar {L}}+{\frac {\hbar }{2}}{\tilde {\bar {\sigma }}}={\bar {r}}\times {\bar {p}}\left({\begin{matrix}1&0\\0&1\\\end{matrix}}\right)+{\frac {\hbar }{2}}{\tilde {\bar {\sigma }}}\\&{\bar {r}}\times {\bar {p}}\left({\begin{matrix}1&0\\0&1\\\end{matrix}}\right)={\bar {r}}\times {\bar {p}}\left({\begin{matrix}1&{}&{}&{}\\{}&1&{}&{}\\{}&{}&1&{}\\{}&{}&{}&1\\\end{matrix}}\right)\\\end{aligned}}

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MathML (3.326 KB / 459 B) :

\begin{aligned} \bar{J} : = \bar{L} + \frac{ℏ}{2} \tilde{\bar{σ}} = \bar{r} \times \bar{p} (\begin{matrix} 1 & 0 \\ 0 & 1 \end{matrix}) + \frac{ℏ}{2} \tilde{\bar{σ}} \\ \bar{r} \times \bar{p} (\begin{matrix} 1 & 0 \\ 0 & 1 \end{matrix}) = \bar{r} \times \bar{p} (\begin{matrix} 1 \\ 1 \\ 1 \\ 1 \end{matrix}) \end{aligned}

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$\bar{J}$

$\bar{L}$

$\tilde{\bar{σ}}$

$\bar{r}$

$\bar{p}$

$\tilde{\bar{σ}}$

$\bar{r}$

$\bar{p}$

$\bar{r}$

$\bar{p}$

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