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Display information for equation id:math.2685.27 on revision:2685

* Page found: Weitere Eigenschaften der Dirac-Gleichung (eq math.2685.27)

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\left( \mathfrak{i} {{\gamma }^{\nu }}{{\partial }_{\nu }}-m \right)\Psi =0\ \left( \text{in S} \right)\quad \left( \mathfrak{i} \gamma {{'}^{\nu }}\partial {{'}_{\nu }}-m' \right)\Psi '=0\ \left( \text{in S }\!\!'\!\!\text{ } \right)

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( 𝔦 γ ν ∂ ν - m ) Ψ = 0 ( in S )   ( 𝔦 γ ∂ ′ ν - ′ ν m ′ ) Ψ ′ = 0 ( in S  ′   ) fragments fragments ( i superscript 𝛾 𝜈 subscript 𝜈 m ) Ψ 0 fragments ( in S ) italic-  fragments ( i γ superscript superscript 𝜈 ′ superscript subscript 𝜈 ′ superscript 𝑚 ′ ) superscript Ψ ′ 0 fragments ( superscript in S  ′   ) {\displaystyle{\displaystyle\left(\mathfrak{i}{{\gamma}^{\nu}}{{\partial}_{\nu% }}-m\right)\Psi=0\ \left(\text{in S}\right)\quad\left(\mathfrak{i}\gamma{{{}^{% \prime}}^{\nu}}\partial{{{}^{\prime}}_{\nu}}-m^{\prime}\right)\Psi^{\prime}=0% \ \left(\text{in S }\!\!^{\prime}\!\!\text{ }\right)}} 
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MathML (experimentell; keine Bilder) rendering

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(iγν∂ν−m)Ψ=0(in S)(iγ'ν∂'ν−m′)Ψ′=0(in S ′ )
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