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Gauge theory

The global group matters

From local Lie algebra data to allowed matter and line operators.

Start with the mathematical object

A gauge Lie algebra determines the local commutation relations. A connected group with that algebra also requires a global form. For compact simple Lie algebra, write G = G̃/Γ, with G̃ simply connected and Γ a subgroup of its center.

G=G~/Γ,Γ⊆Z(G~)G=\widetilde G/\Gamma,\qquad \Gamma\subseteq Z(\widetilde G)

Test the matter representation

An irreducible representation of G̃ is an ordinary representation of G precisely when Γ acts trivially. For SU(2) → SO(3), this selects integer spin. For SU(3) → PSU(3), it selects zero triality. The workbench preserves a chosen highest weight when you change the global form, so an obstruction remains visible.

R descends to G⟺R(γ)=1for every γ∈ΓR\text{ descends to }G\quad\Longleftrightarrow\quad R(\gamma)=\mathbf1\quad\text{for every }\gamma\in\Gamma

Reverse the question

Given several matter multiplets, take the intersection of their kernels in the center. Any subgroup of that intersection defines a compatible central quotient. This constrains the gauge group without selecting one quotient uniquely.

K=⋂iker⁡ ⁣(Ri∣Z(G~)),Γ⊆KK=\bigcap_i\ker\!\left(R_i\big|_{Z(\widetilde G)}\right),\qquad \Gamma\subseteq K

Specify the physical theory

The gauge group and the matter content are parts of the theory data. Choices of magnetic and dyonic lines and discrete theta parameters can carry additional information. A group page supplies mathematical data. The current saved physical-setup format records fields, a gauge quotient and a polynomial counting question; line spectra and theta choices require additional theory data outside that format.

Try a calculation

Select PSU(3) and enter (p,q) = (3,0). This ten-dimensional representation descends, but is of complex type. Zero center charge and reality type are independent questions.

λ=(3,0),dim⁡R=10,3+2⋅0≡0(mod3)\lambda=(3,0),\qquad \dim R=10,\qquad 3+2\cdot0\equiv0\pmod3

Specify matter and the quotient

Read gauge symmetry and matter representations, then work through the Standard Model setup. Saved polynomial setups retain the selected group and matter; line-operator spectra and theta choices remain outside that format.

Sources and further reading

This guide connects sourced reference material with supported calculations. Source curation and automated checks do not constitute completed independent expert review. Read the editorial method.