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Display information for equation id:math.1820.1 on revision:1820

* Page found: Der nichtrelativistische Grenzfall (eq math.1820.1)

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Der nichtrelativistische Grenzfall Eq: math.1821.1

Hash: 98ab90c983f47be184b89ae32a50ae42

TeX (original user input):

\begin{align}

& H={{m}_{0}}{{c}^{2}}\beta ={{m}_{0}}{{c}^{2}}\left( \begin{matrix}

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

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

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

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

\end{matrix} \right) \\

& \Psi =\left( \begin{matrix}

{{\Psi }_{1}}  \\

{{\Psi }_{2}}  \\

{{\Psi }_{3}}  \\

{{\Psi }_{4}}  \\

\end{matrix} \right)\Rightarrow \beta \Psi =\left( \begin{matrix}

{{\Psi }_{1}}  \\

{{\Psi }_{2}}  \\

-{{\Psi }_{3}}  \\

-{{\Psi }_{4}}  \\

\end{matrix} \right) \\

\end{align}

TeX (checked):

{\begin{aligned}&H={{m}_{0}}{{c}^{2}}\beta ={{m}_{0}}{{c}^{2}}\left({\begin{matrix}1&{}&{}&{}\\{}&1&{}&{}\\{}&{}&-1&{}\\{}&{}&{}&-1\\\end{matrix}}\right)\\&\Psi =\left({\begin{matrix}{{\Psi }_{1}}\\{{\Psi }_{2}}\\{{\Psi }_{3}}\\{{\Psi }_{4}}\\\end{matrix}}\right)\Rightarrow \beta \Psi =\left({\begin{matrix}{{\Psi }_{1}}\\{{\Psi }_{2}}\\-{{\Psi }_{3}}\\-{{\Psi }_{4}}\\\end{matrix}}\right)\\\end{aligned}}

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\begin{aligned} H = m_{0} c^{2} β = m_{0} c^{2} (\begin{matrix} 1 \\ 1 \\ - 1 \\ - 1 \end{matrix}) \\ Ψ = (\begin{matrix} Ψ_{1} \\ Ψ_{2} \\ Ψ_{3} \\ Ψ_{4} \end{matrix}) \Rightarrow β Ψ = (\begin{matrix} Ψ_{1} \\ Ψ_{2} \\ - Ψ_{3} \\ - Ψ_{4} \end{matrix}) \end{aligned}

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Identifiers

$H$

$m_{0}$

$c$

$β$

$m_{0}$

$c$

$Ψ$

$Ψ_{1}$

$Ψ_{2}$

$Ψ_{3}$

$Ψ_{4}$

$β$

$Ψ$

$Ψ_{1}$

$Ψ_{2}$

$Ψ_{3}$

$Ψ_{4}$

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