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Display information for equation id:math.2685.33 on revision:2685

* Page found: Weitere Eigenschaften der Dirac-Gleichung (eq math.2685.33)

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TeX (original user input): 

\left( \mathfrak{i} \gamma {{'}^{\nu }}\partial {{'}_{\nu }}-m' \right)\Psi '=0\Rightarrow \left( \mathfrak{i} {{\gamma }^{\nu }}{{\left( {{L}^{-1}} \right)}^{\mu }}_{\nu }{{\partial }_{\mu }}-m \right)S\Psi =0

LaTeXML (experimentell; verwendet MathML) rendering

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( 𝔦 γ ∂ ′ ν - ′ ν m ′ ) Ψ ′ = 0 ⇒ ( 𝔦 γ ν ( L - 1 ) μ ν ∂ μ - m ) S Ψ = 0 fragments fragments ( i γ superscript superscript 𝜈 ′ superscript subscript 𝜈 ′ superscript 𝑚 ′ ) superscript Ψ ′ 0 ⇒ fragments ( i superscript 𝛾 𝜈 subscript superscript fragments ( superscript 𝐿 1 ) 𝜇 𝜈 subscript 𝜇 m ) S Ψ 0 {\displaystyle{\displaystyle\left(\mathfrak{i}\gamma{{{}^{\prime}}^{\nu}}% \partial{{{}^{\prime}}_{\nu}}-m^{\prime}\right)\Psi^{\prime}=0\Rightarrow\left% (\mathfrak{i}{{\gamma}^{\nu}}{{\left({{L}^{-1}}\right)}^{\mu}}_{\nu}{{\partial% }_{\mu}}-m\right)S\Psi=0}} 
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(iγ'ν∂'ν−m′)Ψ′=0⇒(iγν(L−1)μν∂μ−m)SΨ=0
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