By substituting the right-hand side of (34) in (29), we get

(29a)

$$ \frac{1}{\sqrt{-g}} \frac{\partial \sqrt{-g}}{\partial x_{\sigma}} =

\begin{Bmatrix}\mu \sigma\\\mu\end{Bmatrix} $$

_Divergence of the contravariant four-vector._

Let us multiply (26) with the contravariant fundamental tensor _g_^{μν}

(inner multiplication), then by a transformation of the first member,

the right-hand side takes the form

(A)

$$ \frac{\partial}{\partial x_{\nu}} (g^{\mu\nu} A_{\mu}) - A_{\mu}

\frac{\partial g^{\mu\nu}}{\partial x_{\nu}} - \frac{1}{2}

g^{\tau\alpha} (\frac{\partial g_{\mu\alpha}}{\partial x_{\nu}} +

\frac{\partial g_{ u\alpha}}{\partial x_{\mu}} - \frac{\partial

g_{\mu\nu}}{\partial x_{\alpha}}) g^{\mu\nu} A_{\tau} $$

The Principle of Relativity · 第 139 / 203 题