Killing vectors in KS coordinates

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SUMMARY

The discussion centers on proving the vector components \(\xi^u = \frac{v}{2 r_s}\) and \(\xi^v = \frac{u}{2 r_s}\) as a Killing vector in the KS space-time, defined by the line element \(\frac{4 r_s^3}{r} e^{-\frac{r}{r_s}} (du^2 - dv^2) + r^2 (d\theta^2 + \sin^2 \theta d\phi^2)\). The user encounters difficulties with the GrTensor tool while attempting to incorporate constraints, specifically the equation \(\left( \frac{r}{r_s} - 1 \right) e^{\frac{r}{r_s}} = u^2 - v^2\). The discussion concludes that the Lie derivative of \(g_{\mu\nu}\) with respect to \(\xi_{\mu}\) must be shown to be zero to confirm the Killing vector property.

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pervect
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I want to prove (or disprove) that the vector with components
\xi^u = \frac{v}{2 r_s}\hspace{5 mm} \xi^v = \frac{u}{2 r_s}

is a Killing vector of the KS space-time with line element

\frac{4 r_s^3}{r} e^{-\frac{r}{r_s}} \left( du^2 -dv^2\right) + r^2 \left( d\theta^2 + sin^2 \theta d\phi^2\right)

Here r is an implicit function of u,v, which is handled by a constraint equation.

However, I seem to be having a hard time getting GRT to handle the contraints. I try

\left( \frac{r}{r_s} - 1 \right) e^{\frac{r}{r_s}} = u^2 - v^2 directly, but it doesn't simplify.

I try to feed it the following
<br /> <br /> {\frac {\partial }{\partial u}}r \left( u,v \right) =2\,{{\it r\_s}}^{<br /> 2}u \left( r \left( u,v \right) \right) ^{-1} \left( {e^{{\frac {r<br /> \left( u,v \right) }{{\it r\_s}}}}} \right) ^{-1}<br /> <br />

but it complains about "illegal use of object as a name", I can't see what it's objecting to.

So a) -does this look like the right expression for the Killing Vector? And b) - how does one successfully get the constraints into GrTensor?
 
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Don't need any complicated algebra, it's true almost by inspection. Just show directly that the Lie derivative of gμν with respect to ξμ is zero. The coordinate transformation is u → u + εv, v → v + εu. Then u2 - v2 → u2 - v2 so it obeys the constraint, and du2 - dv2 → du2 - dv2 so it's an isometry, and that's really all there is to it!
 
I set r_s to 1, and renamed r to rr,and finally got GRT to crunch through it,but your way is both much easier and more insightful. Thanks!
 

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