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Display information for equation id:math.1826.29 on revision:1826

* Page found: Das Wasserstoffatom (relativistsich) (eq math.1826.29)

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Hash: 74984f44b24f0bfe895045037eba16cf

TeX (original user input):

\begin{align}

& {{a}_{1}}=\frac{{{m}_{0}}{{c}^{2}}+E}{\hbar c} \\

& {{a}_{2}}=\frac{{{m}_{0}}{{c}^{2}}-E}{\hbar c} \\

& a=\sqrt{{{a}_{1}}{{a}_{2}}}=\frac{\sqrt{{{m}_{0}}^{2}{{c}^{4}}-{{E}^{2}}}}{\hbar c} \\

\end{align}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (20.945 KB / 2.438 KB) :

a 1 = m 0 c 2 + E c a 2 = m 0 c 2 - E c a = a 1 a 2 = m 0 2 c 4 - E 2 c absent subscript 𝑎 1 subscript 𝑚 0 superscript 𝑐 2 𝐸 Planck-constant-over-2-pi 𝑐 absent subscript 𝑎 2 subscript 𝑚 0 superscript 𝑐 2 𝐸 Planck-constant-over-2-pi 𝑐 absent 𝑎 subscript 𝑎 1 subscript 𝑎 2 superscript subscript 𝑚 0 2 superscript 𝑐 4 superscript 𝐸 2 Planck-constant-over-2-pi 𝑐 {\displaystyle{\displaystyle\begin{aligned} \par&\displaystyle{{a}_{1}}=\frac{% {{m}_{0}}{{c}^{2}}+E}{\hbar c}\\ \par&\displaystyle{{a}_{2}}=\frac{{{m}_{0}}{{c}^{2}}-E}{\hbar c}\\ \par&\displaystyle a=\sqrt{{{a}_{1}}{{a}_{2}}}=\frac{\sqrt{{{m}_{0}}^{2}{{c}^{% 4}}-{{E}^{2}}}}{\hbar c}\\ \par\end{aligned}}}

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MathML (experimentell; keine Bilder) rendering

MathML (2.303 KB / 392 B) :

a1=m0c2+Eca2=m0c2Eca=a1a2=m02c4E2c

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