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Display information for equation id:math.1598.37 on revision:1598

* Page found: Zeitunabhängige Schrödinger- Gleichung und stationäre Zustände (eq math.1598.37)

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TeX (original user input): 

\Psi (\bar{r},0)=\sum\limits_{n}^{{}}{{}}{{c}_{n}}{{\phi }_{n}}(\bar{r})\begin{matrix}
!  \\
=  \\
{}  \\
\end{matrix}{{\Psi }_{0}}(\bar{r})

LaTeXML (experimental; uses MathML) rendering

MathML (8.551 KB / 1.469 KB) :

Ψ ⁢ ( r ¯ , 0 ) = ∑ n c n ⁢ ϕ n ⁢ ( r ¯ ) ⁢ ! = ⁢ Ψ 0 ⁢ ( r ¯ ) Ψ ¯ 𝑟 0 subscript 𝑛 subscript 𝑐 𝑛 subscript italic-ϕ 𝑛 ¯ 𝑟 absent subscript Ψ 0 ¯ 𝑟 {\displaystyle{\displaystyle\Psi(\bar{r},0)=\sum\limits_{n}{{}}{{c}_{n}}{{\phi% }_{n}}(\bar{r})\begin{matrix}!\\ =\\ \\ \end{matrix}{{\Psi}_{0}}(\bar{r})}} 
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=\\
\\
\end{matrix}{{\Psi}_{0}}(\bar{r})}}</annotation>
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MathML (1.298 KB / 375 B) :

Ψ(r¯,0)=∑ncnϕn(r¯)!=Ψ0(r¯)
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