GR metric gauge transformation, deduce 'generating' vector

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SUMMARY

The discussion focuses on the transformation of the metric tensor in the context of general relativity, specifically the equation ##g_{uv}'=g_{uv}+\nabla_v C_u+\nabla_u C_v##. The participants analyze the relationship between the transformed metric ##g_{uv}'##, represented as ##ds^2=dx^2+2\epsilon f'(y) dx dy + dy^2##, and the original metric ##g_{uv}##, which is ##ds^2=dx^2+dy^2##. The conclusion drawn is that the function ##C_u## can be expressed as ##C_u=2\epsilon(f(y),0)##, based on the conditions set by the flat space metric.

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binbagsss
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1. Problem

##g_{uv}'=g_{uv}+\nabla_v C_u+\nabla_u C_v##

If ##g_{uv}' ## is given by ##ds^2=dx^2+2\epsilon f'(y) dx dy + dy^2##
And ##g_{uv}## is given by ##ds^2=dx^2+dy^2##, Show that ## C_u=2\epsilon(f(y),0)##?

Homework Equations



Since we are in flatspace we have ##g_{uv}'=g_{uv}+\partial_v C_u+\partial_u C_v##

The Attempt at a Solution


[/B]
Since ##g_{xx}=g'_{xx}## and ##g_{yy}=g'_{yy}##

I get ##\partial_x C_x=\partial_y C_y=0##

##\implies C_x=c(y)##, ##c(y)## the constant of ##x## from integration, some function of ##y##
##C_y=k(x)## ##k(x)## some function of ##x##

From the cross term ##g_{xy}'=g_{yx}'=\epsilon f'(y)## I get:

## \epsilon f'(y)=\partial_x C_y + \partial_y C_x ##

So ## \epsilon f'(y)= k'(x) + c'(y) ##

I have no idea what to do now..

Many thanks in advance
 
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