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A theory that describes how matter interacts dynamically with the geometry of space and time. It was first published by Einstein in 1915 and is currently used to study the structure and evolution of the universe, as well as having practical applications like GPS.

1 vote
1 answer
123 views

Has this metric (which seems like flat space but isn't) been studied before

I am investigating the metric $ds^2 = -dt^2 + (1+C)dr^2 + r^2 d\theta^2 + r^2 \sin^2\theta d\phi^2, $ where $C$ is a constant. This intuitively seems like flat space but actually has a non-zero Kret …
supercoolphysicist's user avatar
0 votes
1 answer
420 views

What is this spacetime metric?

Does anyone know whether this metric has been studied before or if it has a proper name? $$ds^2 = -dt^2 + e^{2At} dx^2 + e^{2Bt} dy^2 + e^{2Ct} dz^2$$ i.e. a de Sitter metric which has a different e …
supercoolphysicist's user avatar
0 votes
0 answers
142 views

What is the physical reasoning for the weak-field approximation to gravity having a curvatur...

The metric for the weak field approximation to gravity is given by $ds^2 = -(1-\Phi(r))dt^2 + (1+\Psi(r))\left(dr^2 + r^2d\theta^2 + r^2\sin^2\theta d\phi^2\right)$ When $\Phi(r)=\Psi(r)$, e.g. when …
supercoolphysicist's user avatar
1 vote
0 answers
72 views

Do negative residues in any decomposition of the graviton propagator lead to ghosts?

When looking at the linearised graviton propagator around a background, one can use several decompositions, e.g. decomposing the perturbation to the background metric $g_{\mu\nu}$ into $h_{\mu\nu} = …
supercoolphysicist's user avatar
0 votes
1 answer
109 views

Plane wave propagating in de Sitter spactime

Around a flat background, a plane wave propagating in the $z$ direction is given by $h_{\mu\nu} = \epsilon_{\mu\nu} \cos(\omega t -kz)$. What is the generalisation of this to a de Sitter background …
supercoolphysicist's user avatar
0 votes

Plane wave propagating in de Sitter spactime

To lowest order in $\Lambda$, i.e. taking the metric to be Minkowski plus a perturbation from $\Lambda$, plus a perturbation from the plane wave, the plane wave is given in the following papers The …
supercoolphysicist's user avatar
2 votes
1 answer
98 views

2nd order perturbation of a charged rotating body

What is the 2nd order perturbation to the flat Minkowski metric $\eta_{ab}$ caused by a charged, rotating body? In particular, if we take a metric $\eta_{ab} + h_{ab} $, what $h_{ab}$ satisfies the Ei …
supercoolphysicist's user avatar
3 votes
0 answers
154 views

Difficult coordinate transformation

I am trying to introduce a tortoise coordinate for a modified Schwarzschild metric $$\mathrm{d}s^2=\left(1-\frac{2M\mathop{}\!\mathrm{erf}(r)}{r}\right) \mathrm{d}t^2 + \left(1-\frac{2M\mathop{}\!\ma …
supercoolphysicist's user avatar
8 votes
1 answer
2k views

Fourier transform in curved spacetimes

When in a flat spacetime, one can use the identity $$\int^\infty_{-\infty} d^3k~ e^{i \bf{ k \cdot r}} f(k)=\int^\infty_{-\infty} dk ~ k f(k)\sin(kr) $$ Does this generalise to curved spacetimes, f …
supercoolphysicist's user avatar
1 vote

Tensor Index Notation Manipulation

You raise tensors using your metric tensor. For flat spacetime, this is the Minkowski metric $\eta_{\mu\nu}$. You must contract the Minkowski metric with one of the indices of your tensor in order to …
supercoolphysicist's user avatar
1 vote
1 answer
429 views

Quadrupole moment of Kerr spacetime

In this paper, the Kerr black hole is described as having quadrupole moment of $q=J^2/M$ (which means $q=a^2M$ using $J=aM$) whereas in this paper it says in the abstract that the limiting case of Ker …
supercoolphysicist's user avatar
0 votes
1 answer
574 views

Deriving the Schwarzschild metric in the weak-field regime

I am trying to derive the weak-field Schwarzschild metric, but starting from the same form as Schwarzschild: $ds^2=-(1+2\Phi(r))dt^2+(1-2\Psi(r))dr^2 +r^2 d\Omega^2$ which has $R=-2\partial_r^2 \Phi …
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1 vote

Deriving a Schwarzschild radius using relativistic mass

John Rennie, I think we should clarify that when you go from the second metric to the first, you first perform the transformation $dx^2+dy^2 + dz^2=dr^2 + r^2 d\theta^2+r^2\sin^2\theta d\phi^2$, which …
supercoolphysicist's user avatar
3 votes
1 answer
715 views

Commutation relations for inverse d'Alembertian operator

Is there a commutation relation for the inverse d'Alembertian operator in general relativity? i.e. if we define $\Box = g^{\mu\nu}\nabla_\mu\nabla_\nu$ and $\Box \Box^{-1}X_{\alpha_1,\alpha_2...}=X_{\ …
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