Existence and stability of nonzero auxiliary-coset branches

Determine whether nonzero branches of the auxiliary coset connection \(X\), including branches disconnected from the regular \(X=0\) branch, exist and are stable while satisfying both the algebraic coset-connection equation and the remaining connection equation of the exactly orbit-constrained projected Yang–Mills theory.

Background

In the exactly constrained theory with positive Higgs kinetic coefficient, the coset connection XX is auxiliary. On the regular weak-curvature branch, its algebraic equation eliminates it through the solution X=0X=0, reducing the theory locally to SU(n)SU(n) Yang–Mills theory.

The algebraic equation is nonlinear because the projected curvature contains the term su(X∧X){}_{su}(X\wedge X). The paper develops eigenvalue, Cartan-root, fixed-point, and bifurcation criteria for possible nonzero solutions, but emphasizes that solving the pointwise algebraic equation is insufficient: a candidate branch must also satisfy the coupled equation for the remaining connection BB. The existence and stability of such branches, especially those not connected to X=0X=0, are therefore left unresolved.

References

The existence and stability of nonzero branches, including those disconnected from $X=0$, remain open.

— Projected Yang-Mills Theory and the MacDowell-Mansouri Analogy  (2610.08566 - Alvarez, 6 Oct 2026) in Section 7, Summary and Discussion; see also Section 4.6, “Nontrivial branches of the auxiliary coset connection”