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Display information for equation id:math.1821.3 on revision:1821

* Page found: Der nichtrelativistische Grenzfall (eq math.1821.3)

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Hash: 76bf6c24f919c6185cb8b1520674be69

TeX (original user input):

\begin{align}

& \Rightarrow i\hbar {{{\dot{\Psi }}}_{1,2}}={{m}_{0}}{{c}^{2}}{{\Psi }_{1,2}} \\

& \Rightarrow i\hbar {{{\dot{\Psi }}}_{3,4}}=-{{m}_{0}}{{c}^{2}}{{\Psi }_{3,4}} \\

&  \\

\end{align}

TeX (checked):

{\begin{aligned}&\Rightarrow i\hbar {{\dot {\Psi }}_{1,2}}={{m}_{0}}{{c}^{2}}{{\Psi }_{1,2}}\\&\Rightarrow i\hbar {{\dot {\Psi }}_{3,4}}=-{{m}_{0}}{{c}^{2}}{{\Psi }_{3,4}}\\&\\\end{aligned}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (16.419 KB / 2.079 KB) :

i Ψ ˙ 1 , 2 = m 0 c 2 Ψ 1 , 2 i Ψ ˙ 3 , 4 = - m 0 c 2 Ψ 3 , 4 absent absent 𝑖 Planck-constant-over-2-pi subscript ˙ Ψ 1 2 subscript 𝑚 0 superscript 𝑐 2 subscript Ψ 1 2 absent absent 𝑖 Planck-constant-over-2-pi subscript ˙ Ψ 3 4 subscript 𝑚 0 superscript 𝑐 2 subscript Ψ 3 4 absent missing-subexpression {\displaystyle{\displaystyle\begin{aligned} \par&\displaystyle\Rightarrow i% \hbar{{{\dot{\Psi}}}_{1,2}}={{m}_{0}}{{c}^{2}}{{\Psi}_{1,2}}\\ \par&\displaystyle\Rightarrow i\hbar{{{\dot{\Psi}}}_{3,4}}=-{{m}_{0}}{{c}^{2}}% {{\Psi}_{3,4}}\\ \par&\\ \par\end{aligned}}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.752 KB / 388 B) :

iΨ˙1,2=m0c2Ψ1,2iΨ˙3,4=m0c2Ψ3,4

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Calculated based on the variables occurring on the entire Der nichtrelativistische Grenzfall page

Identifiers

  • i
  • Ψ˙1,2
  • m0
  • c
  • Ψ1,2
  • i
  • Ψ˙3,4
  • m0
  • c
  • Ψ3,4

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