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TeX (original user input):

\begin{align}
  & R=\frac{1}{\sqrt{-g}}{{\left[ \sqrt{-g}\left( -{{g}^{\mu }}^{\nu }\Gamma _{\mu \nu }^{\alpha }+{{g}^{\mu }}^{\alpha }\Gamma _{\mu \nu }^{\nu } \right) \right]}_{,\alpha }}+{{L}_{E}}\left( g,\Gamma  \right) \\ 
 & {{L}_{E}}={{g}^{\mu }}^{\nu }\left( \Gamma _{\mu \nu }^{\alpha }\Gamma _{\alpha \beta }^{\beta }-\Gamma _{\mu \beta }^{\alpha }\Gamma _{\nu \alpha }^{\beta } \right) \\ 
 & {{S}_{EH}}=\int\limits_{{{V}_{4}}}{\left( {{L}_{E}}+2\kappa {{L}_{Mat}} \right)\sqrt{-g}{{d}^{4}}x}+\int\limits_{{{V}_{4}}}{\frac{1}{\sqrt{-g}}{{\left[ \sqrt{-g}\left( -{{g}^{\mu }}^{\nu }\Gamma _{\mu \nu }^{\alpha }+{{g}^{\mu }}^{\alpha }\Gamma _{\mu \nu }^{\nu } \right) \right]}_{,\alpha }}\sqrt{-g}{{d}^{4}}x} \\ 
\end{align}

TeX (checked):

{\begin{aligned}&R={\frac {1}{\sqrt {-g}}}{{\left[{\sqrt {-g}}\left(-{{g}^{\mu }}^{\nu }\Gamma _{\mu \nu }^{\alpha }+{{g}^{\mu }}^{\alpha }\Gamma _{\mu \nu }^{\nu }\right)\right]}_{,\alpha }}+{{L}_{E}}\left(g,\Gamma \right)\\&{{L}_{E}}={{g}^{\mu }}^{\nu }\left(\Gamma _{\mu \nu }^{\alpha }\Gamma _{\alpha \beta }^{\beta }-\Gamma _{\mu \beta }^{\alpha }\Gamma _{\nu \alpha }^{\beta }\right)\\&{{S}_{EH}}=\int \limits _{{V}_{4}}{\left({{L}_{E}}+2\kappa {{L}_{Mat}}\right){\sqrt {-g}}{{d}^{4}}x}+\int \limits _{{V}_{4}}{{\frac {1}{\sqrt {-g}}}{{\left[{\sqrt {-g}}\left(-{{g}^{\mu }}^{\nu }\Gamma _{\mu \nu }^{\alpha }+{{g}^{\mu }}^{\alpha }\Gamma _{\mu \nu }^{\nu }\right)\right]}_{,\alpha }}{\sqrt {-g}}{{d}^{4}}x}\\\end{aligned}}

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R=1g[g(gμνΓμνα+gμαΓμνν)],α+LE(g,Γ)LE=gμν(ΓμναΓαββΓμβαΓναβ)SEH=V4(LE+2κLMat)gd4x+V41g[g(gμνΓμνα+gμαΓμνν)],αgd4x
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  • R
  • g
  • g
  • g
  • μ
  • ν
  • Γ
  • μ
  • ν
  • α
  • g
  • μ
  • α
  • Γ
  • μ
  • ν
  • ν
  • α
  • LE
  • g
  • Γ
  • LE
  • g
  • μ
  • ν
  • Γ
  • μ
  • ν
  • α
  • Γ
  • α
  • β
  • β
  • Γ
  • μ
  • β
  • α
  • Γ
  • ν
  • α
  • β
  • SEH
  • V4
  • LE
  • κ
  • LMat
  • g
  • x
  • V4
  • g
  • g
  • g
  • μ
  • ν
  • Γ
  • μ
  • ν
  • α
  • g
  • μ
  • α
  • Γ
  • μ
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