Variation of the kinetic term in scalar field theory

In summary, the variation of the kinetic term in scalar field theory involves analyzing how changes in the scalar field influence the action's kinetic component. This process typically entails calculating the functional derivatives of the kinetic term with respect to the field and its derivatives, leading to the equations of motion described by the Euler-Lagrange equations. The study of these variations reveals important physical implications, including the stability of the field configurations and the dynamics of scalar fields in different spacetime backgrounds. This analysis is crucial for understanding the behavior of scalar fields in various theoretical frameworks, including cosmology and particle physics.
  • #1
Baela
17
2
Varying ##\partial_\lambda\phi\,\partial^\lambda\phi## wrt the metric tensor ##g_{\mu\nu}## in two different ways gives me different results. Obviously I'm doing something wrong. Where am I going wrong?

Method 1: \begin{equation}
(\delta g_{\mu\nu})\,\partial^\mu\phi\,\partial^\nu\phi
\end{equation}

Method 2: \begin{align}&\quad\,\, (\delta g^{\mu\nu})\,\partial_\mu\phi\,\partial_\nu\phi \nonumber \\
&=(-g^{\mu\rho}g^{\nu\sigma}\delta g_{\rho\sigma})\,\partial_\mu\phi\,\partial_\nu\phi \quad (\because \delta g^{\mu\nu}=-g^{\mu\rho}g^{\nu\sigma}\delta g_{\rho\sigma} \,\,\text{as can be checked by varying the identity}\,\, g^{\mu\lambda}g_{\lambda\nu}=\delta^\mu_\nu) \nonumber\\
&=-(\delta g_{\rho\sigma})\,\partial^\rho\phi\,\partial^\sigma\phi
\end{align}
The second result differs from the first one by a minus sign. What's going wrong?
 
Last edited:
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  • #2
In Method 1 you are missing the variations of the metric inside the definitions ##\partial^\mu \phi = g^{\mu\nu}\partial_\nu \phi##.
 

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