- #1
latentcorpse
- 1,444
- 0
In question 4 of this paper, I am trying to find the sign of [itex]\Lambda[/itex]
Since we have the vacuum einstein eqns [itex]G_{\mu \nu}=-\Lambda g_{\mu \nu}[/itex]
we can just contract to get [itex]R-\frac{4}{2} R=-4\Lambda \Rightarrow \Lambda=\frac{R}{4}[/itex]
So [itex]\Lambda[/itex] will have the same sign as [itex]R[/itex]
Now given the components of [itex]R[/itex] in the question, we compute [itex]R=3 \frac{\ddot{a}}{a} + ( a \ddot{a} + 2 \dot{a}^2 +2 ) ( 1 + \sin^2{\chi} + \sin^2{\chi} \sin^2{\theta})[/itex]
Now the second bracket is clearly positive.
I'm not sure about the rest of the expression though because, how do we know the signs of [itex]a , \dot{a} , \ddot{a}[/itex]? We aren't told whether the universe is accelerating or not?
Secondly, in the next bit of the question, we have to obtain the scale factor.
I have solved the continuity equation [itex]\dot{\rho} + 3\gamma \frac{\dot{a}}{a} \rho=0[/itex]
However, [itex]\gamma=0[/itex] when we have a cosmological constant fluid.
This means [itex]\dot{\rho}=0 \Rightarrow \rho = k[/itex] where [itex]k[/itex] is constant.
This would meant that the Friedmann equation will read [itex]\left( \frac{\dot{a}}{a} \right)^2 = \frac{8 \pi G k}{3} + \frac{\Lambda}{3}[/itex]
But then I don't see how to solve for [itex]a[/itex]? Also I think I may have made a mistake or missed something as I don't see how that time symmetry and rescaling stuff is going to help.
I think we are trying to get to a de Sitter spacetime ultimately!
Cheers.
Since we have the vacuum einstein eqns [itex]G_{\mu \nu}=-\Lambda g_{\mu \nu}[/itex]
we can just contract to get [itex]R-\frac{4}{2} R=-4\Lambda \Rightarrow \Lambda=\frac{R}{4}[/itex]
So [itex]\Lambda[/itex] will have the same sign as [itex]R[/itex]
Now given the components of [itex]R[/itex] in the question, we compute [itex]R=3 \frac{\ddot{a}}{a} + ( a \ddot{a} + 2 \dot{a}^2 +2 ) ( 1 + \sin^2{\chi} + \sin^2{\chi} \sin^2{\theta})[/itex]
Now the second bracket is clearly positive.
I'm not sure about the rest of the expression though because, how do we know the signs of [itex]a , \dot{a} , \ddot{a}[/itex]? We aren't told whether the universe is accelerating or not?
Secondly, in the next bit of the question, we have to obtain the scale factor.
I have solved the continuity equation [itex]\dot{\rho} + 3\gamma \frac{\dot{a}}{a} \rho=0[/itex]
However, [itex]\gamma=0[/itex] when we have a cosmological constant fluid.
This means [itex]\dot{\rho}=0 \Rightarrow \rho = k[/itex] where [itex]k[/itex] is constant.
This would meant that the Friedmann equation will read [itex]\left( \frac{\dot{a}}{a} \right)^2 = \frac{8 \pi G k}{3} + \frac{\Lambda}{3}[/itex]
But then I don't see how to solve for [itex]a[/itex]? Also I think I may have made a mistake or missed something as I don't see how that time symmetry and rescaling stuff is going to help.
I think we are trying to get to a de Sitter spacetime ultimately!
Cheers.