The observable and non-observable parts of the Universe

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Discussion Overview

The discussion centers on the nature of the observable and non-observable universe, particularly in relation to the Big Bang. Participants explore whether the Big Bang was responsible solely for the observable universe or if it also pertains to the unobservable universe, delving into theoretical implications and interpretations of various sources.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants propose that the Big Bang only gave rise to the observable universe, suggesting that the unobservable universe exists outside of this initial event.
  • Others argue that the universe is spatially infinite, and while the observable universe was smaller in the past, the entire universe remains infinite regardless of the observable portion's size.
  • A later reply questions the interpretation of sources, suggesting that the observable universe's size can shrink to zero at the singularity, which raises issues about the nature of infinity and the Big Bang.
  • Some participants highlight the distinction between the observable universe and the entirety of the universe, emphasizing that the observable universe is just a finite part of a potentially infinite whole.
  • There are references to various models, including inflation, which some believe may provide a better understanding of the universe's origins than traditional interpretations of the Big Bang singularity.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between the Big Bang and the observable versus unobservable universe. The discussion remains unresolved, with no consensus on the interpretations of the sources or the implications of the Big Bang.

Contextual Notes

Participants note limitations in understanding due to the complexities of infinity and the nature of singularities, as well as the potential for misinterpretation of popular science sources.

  • #31
PeroK said:
Mathematically that doesn't imply what you might intuitively want it to imply.

For example, let's assume your ##t=0## scenario is valid. You claim to have a set of infinite extent. But, you are unable to find any two points whose distance is non-zero. This is a contradiction.

The mathematical answer is probably that in the limit you no longer have a valid manifold. You can't talk about distances unless you have a valid metric. And, in the limit, you no longer have a valid metric.
I’m actually not suggesting those satements to imply anything other than what they say. Just that those statements are important to understand and somewhat counterintuitive. Formulating them as Ned did, I agree is not mathematically valid, but I believe he really meant these underlying statements and improperly simplified them for a nontechnical article.
 
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  • #32
PeroK said:
You claim to have a set of infinite extent.

No, that's not what he claimed. The limiting procedure @PAllen described does not construct a set and say that it is "a spacelike slice at time ##t = 0##". It only constructs a number and says that it has the same value (infinity) at ##t = 0## as it has for all ##t > 0##. Of course this is a sloppy heuristic description, but it can be made precise without having to make any claims about an infinite set of points existing at ##t = 0##.

That said, there is also a different way of proceeding, which is to use the method used to construct Penrose diagrams to add a "boundary" corresponding to ##t = 0## to the FRW spacetime manifold. This procedure does in fact lead to a boundary with an infinite set of distinct points in it, each one corresponding to a particular 3-tuple of comoving coordinates, i.e., to a distinct "spatial point" in each spacelike slice in the region ##t > 0##. Physically, this corresponds to the fact that, in the limit ##t \rightarrow 0##, every single spatial point in the FRW universe becomes causally disconnected from every other. We can then use the induced metric (if it can be called that--see further comments below) on the boundary to compute zero spatial volume for this infinite set of points (because, as I noted earlier, the sum of an infinite set of zeroes is still zero).

PeroK said:
You claim to have a set of infinite extent. But, you are unable to find any two points whose distance is non-zero. This is a contradiction.

No, it isn't. It simply says that this...

PeroK said:
You can't talk about distances unless you have a valid metric. And, in the limit, you no longer have a valid metric.

...is correct in the sense that there is no valid Riemannian metric on the infinite set of points at ##t = 0## constructed by the method I described above. But you do have a valid manifold, because having a valid manifold does not require having a valid Riemannian metric. And you do have a perfectly well-defined mathematical formula that assigns the value zero to the integral ##\int \int \int a(t = 0) dx dy dz## over this manifold. And this formula is derived from a thingie that looks like a metric, just not a Riemannian one.

So at this point we have a situation which, although describable consistently using math, has no description in ordinary language that really does justice to it.
 
  • #33
PeterDonis said:
But you do have a valid manifold, because having a valid manifold does not require having a valid Riemannian metric. And you do have a perfectly well-defined mathematical formula that assigns the value zero to the integral ##\int \int \int a(t = 0) dx dy dz## over this manifold. And this formula is derived from a thingie that looks like a metric, just not a Riemannian one.

What is the definition of this metric "thingie"?
 
  • #34
PeroK said:
What is the definition of this metric "thingie"?

##a(t) \left( dx^2 + dy^2 + dz^2 \right)## for ##t = 0##
 
  • #35
PeterDonis said:
##a(t) \left( dx^2 + dy^2 + dz^2 \right)## for ##t = 0##

But ##a(0) = 0##?
 
  • #36
PeroK said:
But ##a(0) = 0##?

Yes, that's why the thingie I wrote is not a valid Riemannian metric for ##t = 0##. But it's still a perfectly well-defined mathematical formula.
 
  • #37
Most FLRW cosmologies have an irremovable singularity in that not only is there geodesic incompleteness, but curvature invariants become infinite, which prevents an extension of the manifold to remove geodesic incompleteness. However, the special case of a(t)=t, the Milne cosmology is interesting in relation to what @PeterDonis is discussing. Here, geodesic incompleteness is removable because curvature is identically zero everywhere, and a coordinate transform takes you to Minkowski coordinates. Here, the limiting t=0 surface (not considered part of the Milne model) is simply the light cone from t=0, spatial origin. This is topologically R3, because it is S2XR plus the central point. However, metrically, any way of computing its volume is zero because one component of the volume element must be light like. Here we are using the Minkowski metric which is perfectly well defined, and is a true (pseudoriemannian) metric.
 
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  • #38
Thank you all of you!

I see that post #13, #14, #15 were more direct replies to my post. I appreciate and value your advice, and could see your point. There were many points about the big bang which had bothered me for years but I'm glad that I have the basic answers and can picture it better.

There is no doubt that a book should be the primary source of learning, and it gives you a detailed and coherent view of a subject. At the same you need to devote more time to go through a book which some of us find it hard for several reasons.

I have another question cosmic microwave background radiation, CMBR, which is closely related to the observable universe. Could I ask it here or start a new thread?

Thank you!
 
  • #39
PainterGuy said:
Thank you all of you!

I see that post #13, #14, #15 were more direct replies to my post. I appreciate and value your advice, and could see your point. There were many points about the big bang which had bothered me for years but I'm glad that I have the basic answers and can picture it better.

There is no doubt that a book should be the primary source of learning, and it gives you a detailed and coherent view of a subject. At the same you need to devote more time to go through a book which some of us find it hard for several reasons.

I have another question cosmic microwave background radiation, CMBR, which is closely related to the observable universe. Could I ask it here or start a new thread?

Thank you!
Start a new thread.
 
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