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Display information for equation id:math.1619.86 on revision:1619

* Page found: Zustandsvektoren im Hilbertraum (eq math.1619.86)

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TeX (original user input): 

\int_{{{R}^{3}}}^{{}}{{{d}^{3}}p\left| {\bar{p}} \right\rangle \left\langle  {\bar{p}} \right|}=\int_{{{R}^{3}}}^{{}}{{{d}^{3}}r\left| {\bar{r}} \right\rangle }\left\langle  {\bar{r}} \right|=1

TeX (checked): 

\int _{{R}^{3}}^{}{{{d}^{3}}p\left|{\bar {p}}\right\rangle \left\langle {\bar {p}}\right|}=\int _{{R}^{3}}^{}{{{d}^{3}}r\left|{\bar {r}}\right\rangle }\left\langle {\bar {r}}\right|=1

LaTeXML (experimentell; verwendet MathML) rendering

MathML (10.303 KB / 1.479 KB) :

∫ R 3 d 3 ⁢ p ⁢ | p ¯ ⟩ ⁢ ⟨ p ¯ | = ∫ R 3 d 3 ⁢ r ⁢ | r ¯ ⟩ ⁢ ⟨ r ¯ | = 1 subscript superscript 𝑅 3 superscript 𝑑 3 𝑝 ket ¯ 𝑝 bra ¯ 𝑝 subscript superscript 𝑅 3 superscript 𝑑 3 𝑟 ket ¯ 𝑟 bra ¯ 𝑟 1 {\displaystyle{\displaystyle\int_{{{R}^{3}}}{{{d}^{3}}p\left|{\bar{p}}\right% \rangle\left\langle{\bar{p}}\right|}=\int_{{{R}^{3}}}{{{d}^{3}}r\left|{\bar{r}% }\right\rangle}\left\langle{\bar{r}}\right|=1}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.806 KB / 331 B) :

∫R3d3p|p¯⟩⟨p¯|=∫R3d3r|r¯⟩⟨r¯|=1

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Identifiers

  • R
  • p
  • p¯
  • p¯
  • R
  • r
  • r¯
  • r¯

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