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Display information for equation id:math.1599.24 on revision:1599

* Page found: Zeitunabhängige Schrödinger- Gleichung und stationäre Zustände (eq math.1599.24)

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Hash: 838a7b191dac3f422ffeb7b65eba18ac

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*

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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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MathML (experimentell; keine Bilder) rendering

MathML (1.279 KB / 329 B) :

∫R3(H^Ψ)*Ψd3r=∫R3(EΨ)*Ψd3r=E*
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