Paper 2, Section II, D

General Relativity | Part II, 2016

The Kasner (vacuum) cosmological model is defined by the line element

ds2=c2dt2+t2p1dx2+t2p2dy2+t2p3dz2 with t>0d s^{2}=-c^{2} d t^{2}+t^{2 p_{1}} d x^{2}+t^{2 p_{2}} d y^{2}+t^{2 p_{3}} d z^{2} \quad \text { with } \quad t>0

where p1,p2,p3p_{1}, p_{2}, p_{3} are constants with p1+p2+p3=p12+p22+p32=1p_{1}+p_{2}+p_{3}=p_{1}^{2}+p_{2}^{2}+p_{3}^{2}=1 and 0<p1<10<p_{1}<1. Show that p2p3<0p_{2} p_{3}<0.

Write down four equations that determine the null geodesics of the Kasner model.

If kak^{a} is the tangent vector to the trajectory of a photon and uau^{a} is the four-velocity of a comoving observer (i.e., an observer at rest in the (t,x,y,z)(t, x, y, z) coordinate system above), what is the physical interpretation of kauak_{a} u^{a} ?

Let OO be a comoving observer at the origin, x=y=z=0x=y=z=0, and let SS be a comoving source of photons located on one of the spatial coordinate axes.

(i) Show that photons emitted by SS and observed by OO can be either redshifted or blue-shifted, depending on the location of SS.

(ii) Given any fixed time t=Tt=T, show that there are locations for SS on each coordinate axis from which no photons reach OO for tTt \leqslant T.

Now suppose that p1=1p_{1}=1 and p2=p3=0p_{2}=p_{3}=0. Does the property in (ii) still hold?

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