No. | Reporting period | Objectives | Activities | Results |
---|---|---|---|---|
1 | 3.11.2008 -- 15.12.2008 | Study supersymmetric solutions |
|
arXiv: 0812.2172 |
2 | 16.12.2008 - 15.06.2009 | Study of supersymmetric solutions |
|
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3 | 16.06.2009 - 15.12.2009 |
| Heterotic Compactifications on SU(2)-structure backgrounds - published in JHEP 1001 (2010) 011 |
1st reporting period
For the initial stage of the project a simple model was considered. This consists of N=1 supergravity coupled to a "visible" sector made of a E6 gauge theory with one chiral field in the 27 and one singlet field (the Kaehler modulus). The possible supersymmetric solutions with gauge group which is large enough to contain the Standard Model were classified and moduli stabilisation discussed for these cases. It has been shown that for this simple models there are no proper supersymmetric solutions. It has also been argued that the absence of solutions can be traced back to the fact that in the absence of matter fields no solutions for this model can be found either. This study helps to identify the probelms which one encounters in finding vacua of these models. In particular it is clear that one needs more complicated models which will be considered in the following stages of the project.2nd and 3rd reporting period
In a second stage of the project a more complete analysis of the supersymmetric solutions was done. It has been argued that in a Minkowski supersymmetric E6 preserving ground state, pairs of matter fields get large masses along with pairs of moduli (both Kaehler and complex structure). Integrating out these massive fields leads to simpler models which can be analysed in detail. We have argued that such models do not have viable solutions mainly due to the fact that the superpoential is large. This prevents using the gaugino condensates to stabilise the dilaton field which is actually the only method which is available in such models. Therefore we were looking for different solutions which may allow for small values for the superpotential. If the gauge group is broken, the small values for the matter fields may lead to a small value for the superpotential. However, such solutions always have a non-vanishing flux superpotential - which is large - at least in the regime where the approximations used in order to derive these models hold.