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Display information for equation id:math.1619.92 on revision:1619

* Page found: Zustandsvektoren im Hilbertraum (eq math.1619.92)

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H=L{}^\text{2}({{R}^{3}})=\left\{ \Psi :{{R}^{3}}\to C\left| {} \right.\left[ \int_{{{R}^{3}}}^{{}}{{{d}^{3}}r{{\left| \Psi (\bar{r}) \right|}^{2}}<\infty } \right] \right\}

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MathML (9.257 KB / 1.677 KB) :

H = L ( R 3 ) 2 = { Ψ : R 3 → C | [ ∫ R 3 d 3 r | Ψ ( r ¯ ) | 2 < ∞ ] } fragments H L superscript fragments ( superscript 𝑅 3 ) 2 fragments { Ψ : superscript 𝑅 3 → C | fragments [ subscript superscript 𝑅 3 superscript 𝑑 3 r | Ψ fragments ( ¯ 𝑟 ) superscript | 2 ] } {\displaystyle{\displaystyle H=L{}^{\text{2}}({{R}^{3}})=\left\{\Psi:{{R}^{3}}% \to C\left|{}\right.\left[\int_{{{R}^{3}}}{{{d}^{3}}r{{\left|\Psi(\bar{r})% \right|}^{2}}<\infty}\right]\right\}}} 
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H=L2(R3)={Ψ:R3→C|[∫R3d3r|Ψ(r¯)|2<∞]}
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