Force balance and quasi-symmetry of Boozer realizations

Determine whether magnetic fields realizing a prescribed Boozer-coordinate magnitude satisfy force-balance relations such as the magnetohydrostatic equation, characterize the relationship between the two free single-variable functions in the local realizability theorem and the usual free functions in magnetohydrostatic solutions with nested flux surfaces, and determine the consequences of additionally requiring quasi-symmetry.

Background

The local realizability theorem allows an arbitrary positive analytic field-strength function in Boozer coordinates, together with admissible analytic flux-function coefficients. This freedom is geometric and does not impose the magnetohydrostatic force-balance equation.

The paper proves a separate characterization showing that admitting Boozer coordinates alone is weaker than satisfying force balance. It also notes that quasi-symmetric field-strength functions are locally realizable, while the resulting flux-surface geometries may nevertheless be constrained. The compatibility of realizability with magnetohydrostatic balance and quasi-symmetry remains unresolved.

References

Do the magnetic fields realizing a particular magnitude $B$ satisfy force-balance relations, such as the MHS equation eq:#1{MHS}? What is the relationship between the two free single-variable functions in thm:#1{FTSD} and the usual free functions encountered in the theory of MHS solutions with nested flux surfaces? What if one also demands that $\bm{B}$ is quasi-symmetric?

— All field strengths are possible locally in Boozer coordinates  (2609.09517 - Klotz et al., 8 Sep 2026) in Conclusions, question (3)

Finally, a related open question is the existence of non-axisymmetric equilibria satisfying exact quasisymmetry.

— Analytic toroidal 3D MHD equilibria and steady Euler flows with invariant surfaces  (2609.26742 - Landreman, 22 Sep 2026) in Discussion and conclusions