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Display information for equation id:math.2676.9 on revision:2676

* Page found: Dirac-Gleichung und Spin: nichtrelativistischer Grenzfall (eq math.2676.9)

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Dirac-Gleichung und Spin: nichtrelativistischer Grenzfall Eq: math.2679.9

Hash: 1abbf678e3e78080fbf3a289785ff8df

TeX (original user input):

\begin{align}
  \underline{A}=\left( {{A}_{1}},{{A}_{2}},{{A}_{3}} \right),\underline{B}=\left( {{B}_{1}},{{B}_{2}},{{B}_{3}} \right),\underline{A},\underline{B}
\text{ vektorwertiger Operator und} \\

\underline{\sigma }=\left( {{{\underline{\underline{\sigma }}}}_{1}},{{{\underline{\underline{\sigma }}}}_{2}},{{{\underline{\underline{\sigma }}}}_{3}} \right)


\text{Vektor der Pauli-Matrizen} \\
\end{align}

TeX (checked):

{\begin{aligned}{\underline {A}}=\left({{A}_{1}},{{A}_{2}},{{A}_{3}}\right),{\underline {B}}=\left({{B}_{1}},{{B}_{2}},{{B}_{3}}\right),{\underline {A}},{\underline {B}}{\text{ vektorwertiger Operator und}}\\{\underline {\sigma }}=\left({{\underline {\underline {\sigma }}}_{1}},{{\underline {\underline {\sigma }}}_{2}},{{\underline {\underline {\sigma }}}_{3}}\right){\text{Vektor der Pauli-Matrizen}}\\\end{aligned}}

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\begin{aligned} \underline{A} = (A_{1}, A_{2}, A_{3}), \underline{B} = (B_{1}, B_{2}, B_{3}), \underline{A}, \underline{B} vektorwertiger Operator und \\ \underline{σ} = ({\underline{\underline{σ}}}_{1}, {\underline{\underline{σ}}}_{2}, {\underline{\underline{σ}}}_{3}) Vektor der Pauli-Matrizen \end{aligned}

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$\underline{A}$

$A_{1}$

$A_{2}$

$A_{3}$

$\underline{B}$

$B_{1}$

$B_{2}$

$B_{3}$

$\underline{A}$

$\underline{B}$

$\underline{σ}$

${\underline{\underline{σ}}}_{1}$

${\underline{\underline{σ}}}_{2}$

${\underline{\underline{σ}}}_{3}$

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