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[edit] Summary
| Description |
Euclidean embedding of a part of the Lambda-CDM spacetime geometry, showing the Milky Way (brown), a quasar at redshift z = 6.4 (yellow), light from the quasar reaching the Earth after approximately 12 billion years (red), and the present-era metric distance to the quasar of approximately 28 billion light years (orange). Lines of latitude (purple) are lines of constant cosmological time, spaced by 1 billion years; lines of longitude (cyan) are worldlines of objects moving with the Hubble flow, spaced by 1 billion light years in the present era (less in the past and more in the future).
|
| Source |
Own work (see mathematical details below)
|
| Date |
2008 March 18
|
| Author |
Ben Rudiak-Gould
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Permission
(Reusing this image) |
Public domain (an attribution would be appreciated but isn't required)
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| Other versions |
Image:Embedded LambdaCDM geometry (alt view).png |
[edit] Mathematical details
The FLRW metric with two spatial dimensions suppressed is
- ds2 = c2dt2 − a(t)2dx2
where a(tnow) = 1. If we flip the sign of the dx term, making the metric Euclidean, it can be embedded isometrically in Euclidean 3-space with cylindrical coordinates (r,φ,z) by

where R is a free parameter. z is only defined when
, and a'(t) goes to infinity for both small and large t in ΛCDM, so a smaller R allows us to embed a larger fraction of the universe's history. On the other hand, with a large R we can embed larger spatial distances, since the embedding curves around on itself at a comoving distance of 2πR.
Ignoring the effects of radiation in the early universe and assuming k = 0 and w = −1, the ΛCDM scale factor is
![a(t) = \left[ \frac{\Omega_m}{\Omega_v} \sinh^2 \left( \frac32 \sqrt{\Omega_v} H_0 t \right) \right]^{\frac13}](http://upload.wikimedia.org/math/4/4/9/449b7a513befd46828e7962a87be66f0.png)
and the WMAP five-year report gives

(Mpc = megaparsec, Gyr = gigayear). For the embedding above I chose
and a time range of 0.7 Gyr to 18 Gyr. I deliberately cut off the embedding short of a full circle to emphasize that space does not loop back on itself (or, if it does, not at a distance governed by the arbitrary parameter R).
The path of the light ray satisfies dx / dt = c / a(t).
File history
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| Date/Time | Dimensions | User | Comment |
| current | 21:09, 18 March 2008 | 640×544 (30 KB) | BenRG | |
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