Quanta of 5-d representations #
The 5-bar representations of the SU(5)รU(1)
carry
the quantum numbers of their U(1) charges and their fluxes.
In this module we define the data structure for these quanta and properties thereof.
##ย Key definitions
FiveQuanta
is the type of quanta of 5-bar representations.FiveQuanta.toFluxesFive
is the underlyingFluxesFive
of aFiveQuanta
.FiveQuanta.toCharges
is the underlying Multiset charges of aFiveQuanta
.FiveQuanta.reduce
is the reduction of aFiveQuanta
which adds together all the fluxes corresponding to the same charge (i.e. representation).FiveQuanta.anomalyCoefficent
is the anomaly coefficent associated with aFiveQuanta
.FiveQuanta.ofChargesExpand
is theFiveQuanta
with fluxes{(1, -1), (1, -1), (1, -1), (0, 1), (0, 1), (0, 1)}
and finite set of charges equal to a givenc
.
Key theorems #
mem_ofChargesExpand_map_reduce_iff
states that aFiveQuanta
is in the image ofofChargesExpand c
underreduce
if and only if it is aFiveQuanta
with charges equal toc
and fluxes which have no exotics or zero.
The quanta of 5-bar representations corresponding to a multiset of
(q, M, N)
for each partcile. (M, N)
are defined in the FluxesFive
module.
Instances For
Reduce #
The reduce
of FiveQuanta
is a new FiveQuanta
with all the fluxes
corresponding to the same charge (i.e. represenation) added together.
Equations
Instances For
Anomaly cancellation #
The anomaly coefficent of a FiveQuanta
is given by the pair of integers:
(โแตข qแตข Nแตข, โแตข qแตขยฒ Nแตข)
.
The first components is for the mixed U(1)-MSSM, see equation (22) of arXiv:1401.5084. The second component is for the mixed U(1)Y-U(1)-U(1) gauge anomaly, see equation (23) of arXiv:1401.5084.
Equations
Instances For
ofChargesExpand #
Given a finite set of charges c
the FiveQuanta
with fluxes {(1, -1), (1, -1), (1, -1), (0, 1), (0, 1), (0, 1)}
and finite set of charges equal to c
.
Equations
- One or more equations did not get rendered due to their size.