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Display information for equation id:math.1699.4 on revision:1699

* Page found: Dynamik des 2- Zustands- Systems (eq math.1699.4)

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Hash: 94ffae6def307d024070b3d4a98104c3

TeX (original user input): 

\hat{V}=-\frac{e\hbar }{2{{m}_{0}}}\hat{\bar{\sigma }}\cdot \bar{B}=-\frac{e\hbar B}{2{{m}_{0}}}{{\hat{\bar{\sigma }}}_{3}}=\hbar {{\omega }_{l}}{{\hat{\bar{\sigma }}}_{3}}

TeX (checked): 

{\hat {V}}=-{\frac {e\hbar }{2{{m}_{0}}}}{\hat {\bar {\sigma }}}\cdot {\bar {B}}=-{\frac {e\hbar B}{2{{m}_{0}}}}{{\hat {\bar {\sigma }}}_{3}}=\hbar {{\omega }_{l}}{{\hat {\bar {\sigma }}}_{3}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (13.391 KB / 1.936 KB) :

V ^ = - e ⁢ ℏ 2 ⁢ m 0 ⁢ σ ¯ ^ ⋅ B ¯ = - e ⁢ ℏ ⁢ B 2 ⁢ m 0 ⁢ σ ¯ ^ 3 = ℏ ⁢ ω l ⁢ σ ¯ ^ 3 ^ 𝑉 ⋅ 𝑒 Planck-constant-over-2-pi 2 subscript 𝑚 0 ^ ¯ 𝜎 ¯ 𝐵 𝑒 Planck-constant-over-2-pi 𝐵 2 subscript 𝑚 0 subscript ^ ¯ 𝜎 3 Planck-constant-over-2-pi subscript 𝜔 𝑙 subscript ^ ¯ 𝜎 3 {\displaystyle{\displaystyle\hat{V}=-\frac{e\hbar}{2{{m}_{0}}}\hat{\bar{\sigma% }}\cdot\bar{B}=-\frac{e\hbar B}{2{{m}_{0}}}{{\hat{\bar{\sigma}}}_{3}}=\hbar{{% \omega}_{l}}{{\hat{\bar{\sigma}}}_{3}}}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.979 KB / 342 B) :

V^=−eℏ2m0σ¯^⋅B¯=−eℏB2m0σ¯^3=ℏωlσ¯^3

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Calculated based on the variables occurring on the entire Dynamik des 2- Zustands- Systems page

Identifiers

  • V^
  • e
  • m0
  • σ¯^
  • B¯
  • e
  • B
  • m0
  • σ¯^3
  • ωl
  • σ¯^3

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