On the chirality of the SM and the fermion content of GUTs

Renato M. Fonseca

doi:10.1016/j.nuclphysb.2015.06.012

paper

On the chirality of the SM and the fermion content of GUTs

arXiv:1504.03695 · doi:10.1016/j.nuclphysb.2015.06.012

Abstract

The Standard Model (SM) is a chiral theory, where right- and left-handed fermion fields transform differently under the gauge group. Extra fermions, if they do exist, need to be heavy otherwise they would have already been observed. With no complex mechanisms at work, such as confining interactions or extra-dimensions, this can only be achieved if every extra right-handed fermion comes paired with a left-handed one transforming in the same way under the Standard Model gauge group, otherwise the new states would only get a mass after electroweak symmetry breaking, which would necessarily be small ( $\sim 100 GeV$ ). Such a simple requirement severely constrains the fermion content of Grand Unified Theories (GUTs). It is known for example that three copies of the representations $5 + 10$ of $S U (5)$ or three copies of the $16$ of $S O (10)$ can reproduce the Standard Model's chirality, but how unique are these arrangements? In a systematic way, this paper looks at the possibility of having non-standard mixtures of fermion GUT representations yielding the correct Standard Model chirality. Family unification is possible with large special unitary groups --- for example, the $171$ representation of $S U (19)$ may decompose as $3 (16) + 120 + 3 (1)$ under $S O (10)$ .

arXiv commentMinor changes; matches publication in Nuclear Physics B

On the chirality of the SM and the fermion content of GUTs

Abstract

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