F-theory with a SU(5) gauge group #
This module contains the details of F-theory with a SU(5) gauge group, with possible additional charges. This should be compared to the directory:
PhysLean.Particles.SuperSymmetry.SU5
which contains the details of the SUSY SU(5) gauge group not in F-theory. Many of the results here use results from that directory.
Data structures #
The main data structures part of this theory are:
PotentialTerm
: An inductive type containing the terms in the super and Kahler potential of the theory. This can be found inPhysLean.Particles.SuperSymmetry.SU5.Potential
, as not specific to F-theory.Fluxes
: Contains the fluxes associated with each representation present in the theory.Charges
: Contains the charges associated with each representation present in the theory. This can be found inPhysLean.Particles.SuperSymmetry.SU5.Potential
, as not specific to F-theory.Quanta
: Contains the fluxes and charges of each representation present in the theory.
Propositions #
There are a number of important propositions in the theory.
Charges.AllowsTerm
: For a given potential term, determines whether an element ofCharges
allows that term.Charges.IsPhenoConstrained
: Is true when the charges permit a term that is phenomenologically constrained, such as the four-dimension proton decay coupling.Fluxes.NoExotics
: Is true when the fluxes lead to no exotic particles.Quanta.IsViable
: Is true when the quanta is phenomenologically viable, meaning it satisfies a number of conditions, such as anomaly cancellation, no exotic particles, and allowing the top Yukawa coupling.
The charges are additionally constrained by the configuration CodimensionOneConfig
,
of the zero-section (σ₀
) and the additional rational section (σ₁
).
This is detailed in the paper arxiv:1504.05593
. In implemented here using
Charges.ofFinset S5 S10
: which gives the finite set of charges where the 5-bar charges must live in the setS5
and the 10-bar charges must live in the setS10
.
Important results #
isViable_iff_mem_viableElems
: Enumerates all the viableQuanta
for a givenCodimensionOneConfig
.
References #
This theory is looked at in the following paper:
- arXiv:1507.05961.