Can Quantum Gravity Explain Inflation After the Big Bang?

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SUMMARY

This discussion centers on the potential role of quantum gravity, specifically Loop Quantum Gravity (LQG), in explaining cosmic inflation following the Big Bang. Key contributors, including Bojowald, Ashtekar, and Singh, have explored the implications of area and volume operators within LQG. While some believe that a brief inflationary period can arise naturally in LQG, it is widely accepted that additional mechanisms, such as the introduction of an inflaton field, are necessary to achieve the "60 e-folds" of expansion typically required for inflationary models. The necessity of such inflation in LQG remains a topic of debate, particularly concerning the horizon problem and the CMB temperature isotropy puzzle.

PREREQUISITES
  • Understanding of Loop Quantum Gravity (LQG)
  • Familiarity with inflationary cosmology concepts
  • Knowledge of eigenvalues and operators in quantum mechanics
  • Awareness of the cosmic microwave background (CMB) and its significance
NEXT STEPS
  • Research the implications of area and volume operators in Loop Quantum Gravity
  • Study the role of inflaton fields in inflationary models
  • Examine the papers by Bojowald, Ashtekar, and Singh on LQG and inflation
  • Investigate the horizon problem and its relevance to nonsingular models
USEFUL FOR

Astronomers, theoretical physicists, and cosmologists interested in the intersection of quantum gravity and cosmological inflation will benefit from this discussion.

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I wonder if quantum gravity effects can explain Inflation after the Big Bang? For example, in Loop Quantum Gravity, there are area and volume operators and eigenvalues, etc. Would there be jumps from one volume state to another with time? Thanks.
 
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friend said:
I wonder if quantum gravity effects can explain Inflation after the Big Bang? For example, in Loop Quantum Gravity, there are area and volume operators and eigenvalues, etc. Would there be jumps from one volume state to another with time? Thanks.

There have been papers on both sides of this issue. As a sample, here is a list of 48 papers:
http://arXiv.org/cits/gr-qc/0403106

These are the papers that cited an early work on this by Bojowald et al.
http://arXiv.org/abs/gr-qc/0403106

My personal opinion is that a brief inflationary period does arise in LQC---and is robust or generic. But this naturally arising brief inflation is not enough to produce the "60 e-folds" typically desired for inflation scenarios.

It seems that something must be put in by hand, to get the expansion by the factor e60 believed necessary to explain flatness and isotropy.

So what I see happening is that in recent LQC work by e.g. Ashtekar and Singh, they put in an inflaton field to get the conventional amount of inflation. The amount that is automatically occurring in the LQC models is not enough. This is just my personal view, I think opinions about it differ.
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A separate issue is whether, in LQC, you actually need e60-fold inflation. The "horizon problem" doesn't exist in a nonsingular model with a bounce because temperature equilibrium can have been achieved prior to bounce. A major motivation for inflation scenarios, namely the CMB temperature isotropy puzzle, is no longer so pressing. Whether and how much inflation is needed remains unresolved, as far as I know.
 
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