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Display information for equation id:math.3923.12 on revision:3923

* Page found: Zustände mit Bahn- und Spinvariablen (eq math.3923.12)

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Hash: 9ffd24bb747a37c79c7ec8209eb5d74b

TeX (original user input): 

\int_{{}}^{{}}{{{d}^{3}}r\left\{ \left| \bar{r}\uparrow \right\rangle \left\langle \bar{r}\uparrow \right|+\left| \bar{r}\downarrow \right\rangle \left\langle \bar{r}\downarrow \right| \right\}}=1\quad \in {{H}_{B}}\times {{H}_{S}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (7.866 KB / 1.435 KB) :

∫ d 3 r { | r ¯ ↑ ⟩ ⟨ r ¯ ↑ | + | r ¯ ↓ ⟩ ⟨ r ¯ ↓ | } = 1   ∈ H B × H S fragments superscript 𝑑 3 r fragments { | ¯ 𝑟 ↑ ⟩ fragments ⟨ ¯ 𝑟 ↑ | | ¯ 𝑟 ↓ ⟩ fragments ⟨ ¯ 𝑟 ↓ | } 1 italic-  subscript 𝐻 𝐵 subscript 𝐻 𝑆 {\displaystyle{\displaystyle\int{{{d}^{3}}r\left\{\left|\bar{r}\uparrow\right% \rangle\left\langle\bar{r}\uparrow\right|+\left|\bar{r}\downarrow\right\rangle% \left\langle\bar{r}\downarrow\right|\right\}}=1\quad\in{{H}_{B}}\times{{H}_{S}% }}} 
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MathML (1.748 KB / 380 B) :

∫d3r{|r¯↑⟩⟨r¯↑|+|r¯↓⟩⟨r¯↓|}=1∈HB×HS
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