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0 votes
0 answers
29 views

Is the tensor product involved in the metric a symmetric product?

The expression of the FRW metric in Cosmology in usually written as: $$ds^2=-dt^2+a^2(t)d\vec{x}^2$$ where $c=1$. However, $dt^2$ is a shortening of $dt\otimes dt$, that is, of the tensor product of $...
Wild Feather's user avatar
0 votes
1 answer
36 views

Question coming from Cosmological Perturbation

We consider the following scalar perturbation on the FRW metric: $$ ds^2 = -(1 + 2\phi)dt^2 +2a\partial_i B dx^i dt + a^2 \left( (1 - 2\psi)\delta_{ij} + 2\partial_{ij}E\right) dx^i dx^j $$ where $\...
Shivam Mishra's user avatar
0 votes
0 answers
86 views

Is there a metric, a solution to Einstein's field equations, for a single body in a space of uniform non-zero density?

The Swarzschild metric describes a single body in an empty space with zero density, while the FLRW metric is presumably for a space with uniform non-zero density but no single body. But is there a ...
John Hobson's user avatar
1 vote
2 answers
133 views

Is the FRW metric, based on spatial homogeneity and isotropy, rotationally and translationally invariant? If so, how?

The spatial part of the Minkowski metric, written in the Cartesian coordinates, $$d\vec{ x}^2=dx^2+dy^2+dz^2,$$ is invariant under spatial translations: $\vec{x}\to \vec{x}+\vec{a}$, where $\vec{a}$ ...
Solidification's user avatar
2 votes
1 answer
110 views

Saddle Shaped Universe

The universe, as described by FLRW metric, if $k = -1$ is clearly a 2 sheet 3-hyperboloid described by $x^2+y^2+z^2-w^2=-R^2$. So where does the more common saddle shaped picture of the open universe ...
Nayeem1's user avatar
  • 1,161
0 votes
2 answers
68 views

Homogeneous and Isotropic But not Maximally Symmetric Space

Is this statement correct: "In a homogeneous and Isotropic space the sectional curvature is constant, while in a maximally symmetric space the Riemann Curvature Tensor is covariantly constant in ...
Nayeem1's user avatar
  • 1,161
4 votes
3 answers
199 views

Change of variables from FRW metric to Newtonian gauge

My question arises from a physics paper, where they state that if we take the FRW metric as follows, where $t_c$ and $\vec{x}$ are the FRW comoving coordinates: $$ds^2=-dt_c^2+a^2(t_c)d\vec{x}_c^2$$ ...
Wild Feather's user avatar
0 votes
0 answers
27 views

A question about Friedmann cosmological expansion equation

A recent paper, arXiv:2403.01555, gives the equations for homogeneity and isotropy of an expanding 3-space as expressed in the following distance interval as $x^i = (t, \chi, \theta, \phi)$ and $x^i + ...
jim akerlund's user avatar
0 votes
1 answer
66 views

Name of metric used by Friedmann

In his original paper, Friedmann used the following dynamic and symmetrical metric: $$\mathrm{d}s^2=a(t)^2\left(\mathrm{d}\chi^2+\sin (\chi)^2\left(\mathrm{d}\theta^2+\sin (\theta)^2 \mathrm{d}\phi^2\...
Vincent ISOZ's user avatar
2 votes
0 answers
120 views

Transformation under coordinate transformation of scalar perurbation of FLRW metric

For the past few days I've been studying perturbation in cosmology. More specifically I am now busy with chapter 6 in Dodelson's Modern cosmology. In this book the perturbed FLRW metric which only ...
luki luk's user avatar
1 vote
0 answers
60 views

Robertson-Walker metric exercise [closed]

I'm trying to solve an exercise from my astrophysics and cosmology class, the request is the following, starting from the RW metric expression: $$ \begin{equation*} ds^2=c^2 dt^2 - a^2 \left ( \frac{...
Lip's user avatar
  • 41
1 vote
0 answers
88 views

Why is $h_{\mu\nu}$ not a tensor in the perturbed Universe in cosmological perturbation theory?

In the cosmological perturbation theory course per Hannu Kurki-Suonio (2022) : https://www.mv.helsinki.fi/home/hkurkisu/CosPer.pdf, there is a remark in the text page 5 that puzzles me. The text goes ...
Vincent's user avatar
  • 1,109
1 vote
1 answer
148 views

Deriving Klein-Gordon equation in curved spacetime [closed]

I try to drive The Klein-Gordon equation for a massless scalar field in case of FRW metric: $$ ds^2= a^2(t) [-dt^2 + dx^2] $$ So I start by: $$\left(\frac{1}{g^{1/2}}\partial_{\mu}(g^{1/2}g^{\mu\nu}\...
Dr. phy's user avatar
  • 395
4 votes
2 answers
170 views

Why isn't the curvature scale in Robertson-Walker metric dynamic?

$$ds^2=-c^2dt^2+a(t)^2 \left[ {dr^2\over1-k{r^2\over R_0^2}}+r^2d\Omega^2 \right]$$ This is the FRW metric, here k=0 for flat space, k=1 for spherical space, k=-1 for hyperbolic space. $R_0$ is the ...
Bababeluma's user avatar
0 votes
0 answers
230 views

Deriving the Ricci tensor on the flat FLRW metric

I am currently with a difficulty in deriving the space-space components of the Ricci tensor in the flat FLRW metric $$ds^2 = -c^2dt^2 + a^2(t)[dx^2 + dy^2 + dz^2],$$ to find: $$R_{ij} = \delta_{ij}[2\...
gabriel's user avatar
0 votes
1 answer
58 views

Making a scale factor invariant *density* in FRW spacetime

For a timelike observer in an FRW spacetime with a perfect fluid, the timelike energy density is given by $T_{\mu\nu}U^\mu U^\nu = \rho(t)$ for a comoving observer. I want to be able to track changes ...
perchlorious's user avatar
2 votes
1 answer
134 views

How do you relate $\Omega_{k}$, the curvature term in the FLRW metric, to the radius of curvature?

I have assumed, for reasons a bit too detailed to go into here, that if $\Omega_{k}$, the curvature term in the FLRW metric, is equal to 1, then the radius of curvature is equal to 13.8 billion light ...
John Hobson's user avatar
1 vote
2 answers
245 views

How is the interior Schwarzschild metric derived?

Where does the interior Schwarzschild metric come from? How is it derived and why does it have NOT a singularity? Would it mean that the singularity is only apparent and for those out of the black ...
Antoniou's user avatar
  • 495
2 votes
1 answer
78 views

Why must the components $g_{0i}$ of an isotropic, homogeneous spacetime metric vanish?

In Daniel Baumann's book on Cosmology, it says that the metric of an isotropic, homogeneous spacetime must have the form $$\mathrm{d}s^2=-\mathrm{d}t^2+a^2(t)\gamma_\mathrm{ij}(x)\mathrm{d}x^\mathrm{i}...
Thomas Wening's user avatar
1 vote
1 answer
69 views

Divergence of the time component of the stress-energy tensor in FLRW metric

I need some help with the divergence of the time component of the stress energy tensor for dust $\nabla_{\mu}T^{0\mu}$ given the stress energy tensor for dust is $$T^{\mu\nu}=(\rho+p)u^{\mu}u^{\nu} + ...
Eduardo V. Kuri's user avatar
0 votes
1 answer
52 views

Common choice in FLRW between dimensionless of scale factor (and coordinates of r lenght dimension) or the contrary

I have an old cosmology book in which the scale factor is expressed in the Roberston-Walker metric as: $\mathrm{d} s^2=c^2 \mathrm{~d} t^2-R(t)^2 \mathrm{~d} l^2$ with: $\mathrm{d} l^2=\dfrac{\mathrm{...
guizmo133's user avatar
0 votes
0 answers
62 views

Spacetimes where symmetries vary from place to place?

Are there spacetimes or metrics where symmetries (like Poincaré, Lorentz, diffeomorphism, translational... invariances) are only local and the symmetries of one local neighbourhood are not, a priori, ...
vengaq's user avatar
  • 2,462
2 votes
1 answer
196 views

What is the $r$ coordinate in a $\mathbb{S}^3$ FLRW spactime?

I'm having trouble understanding what the $r$ reduced-circumference coordinate really is in a 3-sphere $\mathbb{S}^3$ context. Let's start with the unit 3-sphere metric in hyperspherical $(\psi, \...
Johnny's user avatar
  • 163
0 votes
0 answers
86 views

Spacetimes, metrics and symmetries in the theory of relativity?

I was discussing this paper with a couple of physicists colleagues of mine (https://arxiv.org/abs/2011.12970) In the paper, the authors describe "spacetimes without symmetries". When I ...
vengaq's user avatar
  • 2,462
0 votes
1 answer
650 views

Klein-Gordon equation in FRW spacetime

The metric for FRW spacetime is $$ds^2=a(n)^2(dn^2 - dx^2)$$ where $dn$ is the conformal time differential form. The Klein Gordon equation in curved spacetime is $$\left(\frac{1}{g^{1/2}}\partial_{\mu}...
user avatar
1 vote
1 answer
123 views

What's the physical curvature scale $R_0$ in the FLRW metric?

I'm studing the FLRW metric using Daniel Baumann's book, Cosmology (2022), in this book the author derived the FRLW metric using the following equations: $$ dl^2 = \textbf{dx}^2 \pm du^2 $$ and $$ \...
Gustavo Henrique Magro's user avatar
0 votes
1 answer
98 views

Calculating distance from the FRW metric

My question arises from the book Cosmology by Daniel Baumann, specifically from equation (2.81), where I don't understand how the expression for the distance is calculated. I will start by providing ...
Wild Feather's user avatar
0 votes
2 answers
239 views

Christoffel symbol with conformal time not equal to with cosmic time one when making a change of coordinates for d'Alembertian

I think I am having a misunderstanding that would be nice to clear up. The covariant d'Alembertian $$ \Box \phi = g^{\mu\nu}\nabla_\mu\partial_\nu \phi= \left(\partial^2 + \Gamma^\mu_{\mu\lambda}\...
Ziltoid's user avatar
  • 23
0 votes
0 answers
73 views

Energy conservation, photon, distance

From Weinberg 1972 Gravitation and Cosmology Principles, when discussing the luminosity distance, he talked about due to light wavelength being stretched as well as time interval stretched, in the &...
ABC's user avatar
  • 161
1 vote
1 answer
105 views

Area of a sphere in curved 3D space

I'm having trouble finding any information on the derivation of the area of sphere in curved 3D space: $A = 4 \pi S^2_{\kappa}$, where $S_{\kappa} = R_o \sin(r/R_o)$. How did it come about from $ds^2 =...
ABC's user avatar
  • 161

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