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Display information for equation id:math.1597.24 on revision:1597

* Page found: Zeitunabhängige Schrödinger- Gleichung und stationäre Zustände (eq math.1597.24)

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Hash: 2d99a2197014db64f692b0d4da09dad1

TeX (original user input): 

\int\limits_{{{R}^{3}}}^{{}}{{}}\left( \hat{H}\Psi  \right)*\Psi {{d}^{3}}r=\int\limits_{{{R}^{3}}}^{{}}{{}}\left( E\Psi  \right)*\Psi {{d}^{3}}r=E*

TeX (checked): 

\int \limits _{{R}^{3}}^{}{}\left({\hat {H}}\Psi \right)*\Psi {{d}^{3}}r=\int \limits _{{R}^{3}}^{}{}\left(E\Psi \right)*\Psi {{d}^{3}}r=E*

LaTeXML (experimentell; verwendet MathML) rendering

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∫ R 3 ( H ^ Ψ ) * Ψ d 3 r = ∫ R 3 ( E Ψ ) * Ψ d 3 r = E * fragments subscript superscript 𝑅 3 fragments ( ^ 𝐻 Ψ ) Ψ superscript 𝑑 3 r subscript superscript 𝑅 3 fragments ( E Ψ ) Ψ superscript 𝑑 3 r E {\displaystyle{\displaystyle\int\limits_{{{R}^{3}}}{{}}\left(\hat{H}\Psi\right% )*\Psi{{d}^{3}}r=\int\limits_{{{R}^{3}}}{{}}\left(E\Psi\right)*\Psi{{d}^{3}}r=% E*}} 
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SVG (0 B / 8 B) :


SVG (MathML kann über ein Browser-Plugin aktiviert werden) rendering

MathML (2.985 KB / 561 B) :

∫ R 3 ( H ^ Ψ ) ∗ Ψ d 3 r = ∫ R 3 ( E Ψ ) ∗ Ψ d 3 r = E ∗ {\displaystyle \int \limits _{{R}^{3}}^{}{}\left({\hat {H}}\Psi \right)*\Psi {{d}^{3}}r=\int \limits _{{R}^{3}}^{}{}\left(E\Psi \right)*\Psi {{d}^{3}}r=E*} 
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SVG (10.871 KB / 4.558 KB) :

{\displaystyle \int \limits _{{R}^{3}}^{}{}\left({\hat {H}}\Psi \right)*\Psi {{d}^{3}}r=\int \limits _{{R}^{3}}^{}{}\left(E\Psi \right)*\Psi {{d}^{3}}r=E*}

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