Undergrad Inflation resolves the horizon problem

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    Horizon Inflation
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SUMMARY

Inflation resolves the horizon problem in standard cosmology by proposing a rapid expansion phase that disconnects causally connected regions of the universe. This expansion can be modeled by the equation ~exp(βt), where the energy density remains constant, particularly in the context of vacuum energy. The discussion highlights that the universe, currently dominated by dark energy, transitions into an inflationary phase post dark energy-matter equality, with specific parameters such as Ωm=0.31 and ΩΛ=0.68 being critical for accurate cosmological modeling.

PREREQUISITES
  • Understanding of cosmological principles, particularly the horizon problem.
  • Familiarity with the concept of inflation in cosmology.
  • Knowledge of dark energy and its role in the universe's expansion.
  • Basic grasp of cosmological parameters like Ωm and ΩΛ.
NEXT STEPS
  • Study the mathematical framework of inflationary models in cosmology.
  • Explore the implications of dark energy on cosmic expansion and structure formation.
  • Investigate the relationship between redshift and cosmic evolution, particularly at z=16.54.
  • Learn about the role of dark matter in the current cosmological model.
USEFUL FOR

Astronomers, cosmologists, and physics students interested in understanding the dynamics of the universe's expansion and the implications of inflation on cosmological models.

Apashanka
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Can anyone please explain how inflation removes the horizon. problem of standard cosmology .
As much I know inflation is a period of accelerated expansion which can be approximated by ~exp(βt) which can be achieved if the energy density remains constt. throughout (e.g ≠ε(t)),which is the case for the vacuum energy (since P=-ρ)
 
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It expands a causally connected region to envelop the entire current horizon.
 
Orodruin said:
It expands a causally connected region to envelop the entire current horizon.
Will you please explain it in details...
Thank you
 
If I look to the left, the oldest light I can see has been traveling for 13.9bn years. If I look to the right, the oldest light I can see has been traveling for 13.9bn years. Yet the things I'm looking at appear to be at the same temperature. Why? It would only make sense if they were in causal contact and came into thermal equilibrium. But that would need at least 2×13.9bn years, so there isn't time.

Inflation solves the problem by having a rapid expansion phase that takes parts of the universe that were causally connected and disconnects them.
 
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Exactly what part of that is unclear?

If you expect answers tailored to your level you cannot just assume that people know where that is. You need to describe your current understanding and what part you find unclear.

You cannot expect people to write you a textbook excerpt. There are several good resources online. Have you read about it and in that case what was not clear?
 
Ibix said:
But that would need at least 2×13.9bn years
Quite a bit more due to expansion.
 
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We take our universe now to be dominated by the dark energy followed by matter and radiation ,and our universe is now in an accelerating phase (since present value of q <0(-1.52)) and it has to be since dark energy provides exponential growth.
It is therefore after the time of dark energy matter equality ,inflationary (accelerated) phase starts which is ε(t)m=ε(t)d
ε0m/a30d
,a30m0dm0d0=0.04/0.23
a(t)=.057
z=1/a-1=16.54
Can we say that at this redshift inflationary (accelerated phase/dark energy) phase starts??
Since for the matter and radiation dominated phase d2a(t)/dt2<0.
 
Apashanka said:
We take our universe now to be dominated by the dark energy followed by matter and radiation ,and our universe is now in an accelerating phase (since present value of q <0(-1.52)) and it has to be since dark energy provides exponential growth.
It is therefore after the time of dark energy matter equality ,inflationary (accelerated) phase starts which is ε(t)m=ε(t)d
ε0m/a30d
,a30m0dm0d0=0.04/0.23
a(t)=.057
z=1/a-1=16.54
Can we say that at this redshift inflationary (accelerated phase/dark energy) phase starts??
Since for the matter and radiation dominated phase d2a(t)/dt2<0.
Why did you take ##\Omega_m=0.04## and ##\Omega_{\Lambda}=0.23## ? Thats wrong. You should also take the dark matter account hence ##\Omega_m=0.31## and ##\Omega_{\Lambda}=0.68##
 

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