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Display information for equation id:math.1985.51 on revision:1985

* Page found: Hamilton-Jacobische Differenzialgleichung (eq math.1985.51)

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Hash: e63013eda10eead6c56c274a3b37c7fb

TeX (original user input):

\left( \frac{-{{\hbar }^{2}}}{2m}\Delta +V(\bar{r}) \right)\Psi (\bar{r})=E\Psi (\bar{r})

TeX (checked):

\left({\frac {-{{\hbar }^{2}}}{2m}}\Delta +V({\bar {r}})\right)\Psi ({\bar {r}})=E\Psi ({\bar {r}})

LaTeXML (experimental; uses MathML) rendering

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( - 2 2 m Δ + V ( r ¯ ) ) Ψ ( r ¯ ) = E Ψ ( r ¯ ) superscript Planck-constant-over-2-pi 2 2 𝑚 Δ 𝑉 ¯ 𝑟 Ψ ¯ 𝑟 𝐸 Ψ ¯ 𝑟 {\displaystyle{\displaystyle\left(\frac{-{{\hbar}^{2}}}{2m}\Delta+V(\bar{r})% \right)\Psi(\bar{r})=E\Psi(\bar{r})}}
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SVG (MathML can be enabled via browser plugin) rendering

MathML (2.515 KB / 576 B) :

( 2 2 m Δ + V ( r ¯ ) ) Ψ ( r ¯ ) = E Ψ ( r ¯ ) {\displaystyle \left({\frac {-{{\hbar }^{2}}}{2m}}\Delta +V({\bar {r}})\right)\Psi ({\bar {r}})=E\Psi ({\bar {r}})}
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SVG (9.336 KB / 3.887 KB) :

{\displaystyle \left({\frac {-{{\hbar }^{2}}}{2m}}\Delta +V({\bar {r}})\right)\Psi ({\bar {r}})=E\Psi ({\bar {r}})}

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