Physlib.StringTheory.FTheory.SU5.Charges.OfRationalSection
7 declarations
Codimension-one configurations of sections and in F-theory
#CodimensionOneConfigThis inductive type represents the set of distinct geometric configurations of the zero-section relative to the additional rational section within the codimension-one fiber (specifically an fiber) of an F-theory model. These configurations characterize how sections intersect the fiber components and are used to determine the allowed charges for matter fields in the and representations.
Decidability of equality for codimension-one configurations
#instDecidableEqCodimensionOneConfigThis instance provides a procedure to determine whether two codimension-one configurations of sections and in an F-theory model are identical. Specifically, for any two configurations , it is decidable whether .
Finiteness of codimension-one configurations
#instFintypeThe set of distinct geometric configurations of the zero-section and the additional rational section in the codimension-one fiber of an F-theory model, represented by the type , is finite. This finite set is explicitly given by the collection of configurations .
Allowed charges for the representation given a codimension-one configuration
#allowedBarFiveChargesThis function assigns a finite set of integers representing the allowed charges for matter fields in the representation of F-theory, based on the codimension-one configuration of the sections and . For a given configuration , the set of allowed charges is defined as: - If is `same`, the set is . - If is `nearestNeighbor`, the set is . - If is `nextToNearestNeighbor`, the set is .
Allowed charges for the representation of
#allowedTenChargesGiven a codimension-one configuration of the sections and in an F-theory model, this function returns the finite set of allowed charges for matter fields in the representation. The sets are defined based on the configuration as follows: - If , the set of allowed charges is . - If , the set of allowed charges is . - If , the set of allowed charges is .
Finiteness of allowed charges for the representation
#instFintypeSubtypeIntMemFinsetAllowedBarFiveChargesFor any codimension-one configuration of the sections and in an F-theory model, the set of allowed charges for matter fields in the representation is finite.
Finiteness of allowed charges for the representation of
#instFintypeSubtypeIntMemFinsetAllowedTenChargesFor any codimension-one configuration of the sections and in an F-theory model, the set of allowed charges for matter fields in the representation is finite.
