Covariant derivative acting on Dirac delta function in curved space

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The discussion centers on the computation of the covariant derivative of the Dirac delta function in curved space. The main question is whether the formula for the covariant derivative of a scalar density applies to the delta function, which is a scalar density of weight +1. The participants explore the expression for the covariant derivative, specifically focusing on how to express $$\nabla_\mu \delta(x-y)$$. Clarification is sought on the implications of using the given formula from the textbook in this context. Understanding this relationship is crucial for correctly applying functional derivatives in calculations involving curved spacetime.
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Homework Statement
$$\nabla_\beta \nabla_\nu \delta(x-y)=?$$
Relevant Equations
$$\nabla_\mu \phi=\partial_\mu \phi- w \Gamma^\nu_{\nu \mu} \phi$$
Pardon my naive computational question. In my calculations, I encounter the following expression:
$$
\frac{\delta}{\delta g^{\gamma \epsilon}(z)} \left( g_{\mu \alpha}(x) \nabla^x_\beta \nabla^x_\nu \delta(x-y)\right)
$$
To take the functional derivatives, we first need to determine what $$\nabla_\beta \nabla_\nu \delta(x-y)$$ is. Specifically, what is $$\nabla_\mu \delta(x-y)$$ ?

In the textbook it is written that the covariant derivative of a scalar density is given by:
$$
\nabla_\mu \phi=\partial_\mu \phi- w \Gamma^\nu_{\nu \mu} \phi
$$
Does this relation also hold for the delta function, given that the delta function is a scalar density of weight +1?
 
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