9 large dimensions, No curled up ones?

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SUMMARY

This discussion focuses on the exploration of models that incorporate large extra dimensions without relying on small curled-up dimensions. It highlights the challenges posed by large dimensions, particularly in terms of phenomenological issues regarding their visibility. Sean Carroll's proposal of injecting a generic field with a vacuum expectation value (vev) into the fifth dimension is presented as a potential solution. The discussion also references the modification of momentum dispersion relations in Kaluza-Klein (KK) theory due to the presence of a Lorentz-violating field.

PREREQUISITES
  • Understanding of Kaluza-Klein (KK) theory
  • Familiarity with vacuum expectation values (vev) in field theory
  • Knowledge of Lorentz invariance and its violations
  • Basic grasp of phenomenological implications in theoretical physics
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  • Research Sean Carroll's model on large extra dimensions and vacuum expectation values
  • Study the implications of Lorentz-violating fields in particle physics
  • Explore the mathematical framework of Kaluza-Klein theory
  • Investigate phenomenological models addressing the visibility of extra dimensions
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Theoretical physicists, cosmologists, and researchers interested in advanced models of extra dimensions and their implications in fundamental physics.

KeithClemens
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Any models worth checking out that do not rely on small curled up dimensions? And by large dimensions I don't mean 1mm, I mean all dimensions equally large.
 
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Not that I know of. Even large (mm size) extra dimensions is kind of pushing it in the context of replacing one heirachy with another. You see, if the extra dimensions are large then we are immediately faced with phenomenological issues, i.e. where are they?

There are ways to 'hide' large extra dimensions. Sean Carroll came up with an interesting twist recently. http://arxiv.org/abs/0802.0521

The idea is to inject some generic field with a vev into the 5th dimension into a model.

In KK theory the momentum required to probe the extra dims is on the order of:

k\propto\frac{1}{r}

However, the existence of this lorentz violating field modifies the dispersion relations of say some scalar field and the momentum now reads:

k\propto\frac{(1+\alpha_\phi^2)}{r}

where \alpha_\phi is the ratio of the vev of the field to its coupling parameter.
 

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