How Does WMAP Data Influence Our Understanding of Inflationary Potential?

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Discussion Overview

The discussion revolves around the influence of WMAP data on understanding inflationary potential within the context of effective field theory and string theory. Participants explore the implications of mass scales in inflationary models and the dynamics of string theory, as well as the nature of quantum fluctuations during inflation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant references a paper discussing the inflationary potential and its relation to WMAP data, suggesting a need for comments on the findings.
  • Another participant quotes a conclusion from the paper, emphasizing the necessity of specific mass scales for string theory to accurately describe inflationary cosmology and questions how M-theory might address this issue.
  • A different participant argues that string theory dynamics must account for the inflaton mass scale, noting the existence of numerous models in the literature that propose various GUT scales, while also highlighting the challenges in selecting the simplest model due to constraints from experimental data.
  • A participant asks about the standard nature of SUSY scale matching with GUT scales, indicating a desire for clarification on this aspect of the discussion.
  • Another participant raises a question about the horizon crossed by quantum vacuum fluctuations during inflation, specifically inquiring whether it refers to the sound horizon.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between string theory, mass scales, and inflationary models. The discussion remains unresolved, with no consensus reached on the correct model or interpretation of the data.

Contextual Notes

Participants note the complexity of selecting models that fit experimental bounds and the ongoing work in the field, indicating that many assumptions and definitions are still under debate.

Kea
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This looks interesting.

Clarifying Inflation Models: The precise Inflationary Potential
from effective field theory and the WMAP data
D. Cirigliano, H.J. de Vega, N.G. Sanchez
http://arxiv.org/PS_cache/astro-ph/pdf/0412/0412634.pdf

Any comments?
 
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To quote from the conclusion:

"Without the presence of the mass scales [itex]m[/itex] and [itex]M_{\textrm{GUT}}[/itex], there is no hope in String theory to get a correct inflationary cosmology describing the observed CMB fluctuations."

That's not to say that M-theory can't do it. But how?

Here, [itex]m[/itex] is the inflaton mass scale, and it is argued that it satisfies the relation

[tex]m \simeq \frac{M_{\textrm{GUT}}^{2}}{M_{\textrm{pl}}} [/itex][/tex]
 
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It just means the dynamics of String theory must account for that scale, which is well known to be what probably happens. Currently, your guess is as good as any phenomenological experts in that field though as to what *the* correct model is, there are literally dozens across the literature that output 1 or more GUT scales. If you add extra constraints (like getting the proper fcnc suppression, and Cabibo fermion matrices) they all flunk at some point or another. But that's WIP, a lot of people suspect there is enough freedom to output many models that fit all experimental bounds, then its just a question of choosing the simplest (least amount of exotics, etc).
 
hi

Thank you, Haelfix.

What about the SUSY scale mathching [itex]M_{\textrm{GUT}}[/itex] ?
Is this also standard stuff?

Regards
Kea
 
During inflation quantum vacuum fluctuations are generated with physical wavelengths that grow faster than the Hubble radius, when the wavelengths of these perturbations cross the horizon they freeze out and decouple

What horizon is this crossed by the wavelengths? Is possible that is the so-called sound horizon?
 
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