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Display information for equation id:math.1821.31 on revision:1821

* Page found: Der nichtrelativistische Grenzfall (eq math.1821.31)

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Hash: ba841d6da76a5e7603b5bc8ef2c59751

TeX (original user input): 

\frac{1}{2{{m}_{0}}}e\hbar \bar{\sigma }=\frac{e}{{{m}_{0}}}\frac{\hbar }{2}\bar{\sigma }=g\frac{e}{{{m}_{0}}}\bar{S}

TeX (checked): 

{\frac {1}{2{{m}_{0}}}}e\hbar {\bar {\sigma }}={\frac {e}{{m}_{0}}}{\frac {\hbar }{2}}{\bar {\sigma }}=g{\frac {e}{{m}_{0}}}{\bar {S}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (8.596 KB / 1.385 KB) :

1 2 ⁢ m 0 ⁢ e ⁢ ℏ ⁢ σ ¯ = e m 0 ⁢ ℏ 2 ⁢ σ ¯ = g ⁢ e m 0 ⁢ S ¯ 1 2 subscript 𝑚 0 𝑒 Planck-constant-over-2-pi ¯ 𝜎 𝑒 subscript 𝑚 0 Planck-constant-over-2-pi 2 ¯ 𝜎 𝑔 𝑒 subscript 𝑚 0 ¯ 𝑆 {\displaystyle{\displaystyle\frac{1}{2{{m}_{0}}}e\hbar\bar{\sigma}=\frac{e}{{{% m}_{0}}}\frac{\hbar}{2}\bar{\sigma}=g\frac{e}{{{m}_{0}}}\bar{S}}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.402 KB / 296 B) :

12m0eℏσ¯=em0ℏ2σ¯=gem0S¯

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Calculated based on the variables occurring on the entire Der nichtrelativistische Grenzfall page

Identifiers

  • m0
  • e
  • σ¯
  • e
  • m0
  • σ¯
  • g
  • e
  • m0
  • S¯

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