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Display information for equation id:math.2685.29 on revision:2685

* Page found: Weitere Eigenschaften der Dirac-Gleichung (eq math.2685.29)

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TeX (original user input): 

\partial {{'}_{\mu }}=\frac{\partial }{\partial x{{'}^{\mu }}}=\frac{\partial x{{'}^{\nu }}}{\partial {{x}^{\mu }}}\frac{\partial }{\partial {{x}^{\nu }}}={{\left( {{L}^{-1}} \right)}^{\nu }}_{\mu }{{\partial }_{\nu }}

TeX (checked): 

\partial {{'}_{\mu }}={\frac {\partial }{\partial x{{'}^{\mu }}}}={\frac {\partial x{{'}^{\nu }}}{\partial {{x}^{\mu }}}}{\frac {\partial }{\partial {{x}^{\nu }}}}={{\left({{L}^{-1}}\right)}^{\nu }}_{\mu }{{\partial }_{\nu }}

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MathML (11.643 KB / 1.754 KB) :

∂ = ′ μ ∂ ∂ x μ ′ = ∂ x ν ′ ∂ ⁡ x μ ∂ ∂ ⁡ x ν = ( L - 1 ) ν μ ∂ ν fragments superscript subscript 𝜇 ′ fragments x superscript superscript absent 𝜇 ′ fragments x superscript superscript absent 𝜈 ′ superscript 𝑥 𝜇 superscript 𝑥 𝜈 subscript superscript fragments ( superscript 𝐿 1 ) 𝜈 𝜇 subscript 𝜈 {\displaystyle{\displaystyle\partial{{{}^{\prime}}_{\mu}}=\frac{\partial}{% \partial x{{{}^{\prime}}^{\mu}}}=\frac{\partial x{{{}^{\prime}}^{\nu}}}{% \partial{{x}^{\mu}}}\frac{\partial}{\partial{{x}^{\nu}}}={{\left({{L}^{-1}}% \right)}^{\nu}}_{\mu}{{\partial}_{\nu}}}}

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MathML (1.663 KB / 333 B) :

∂'μ=∂∂x'μ=∂x'ν∂xμ∂∂xν=(L−1)νμ∂ν

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  • ν
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  • ν
  • L
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