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Phases and phase-transitions in quasisymmetric configuration space

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arxiv 2202.01194 v1 pith:FGHTL4A3 submitted 2022-02-02 physics.plasm-ph

classification physics.plasm-ph
keywords configurationsquasisymmetricspacephasesclosedconfigurationcurvesgeneral
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We explore the structure of the space of quasisymmetric configurations identifying them by their magnetic axes, described as 3D closed curves. We demonstrate that this topological perspective divides the space of all configurations into well-separated quasisymmetric phases. Each phase is characterized by the self-linking number (a topological invariant), defining different symmetry configurations (quasi-axisymmetry or quasi-helical symmetry). The phase-transition manifolds correspond to quasi-isodynamic configurations. By considering some models for closed curves (most notably torus unknots), general features associated with these phases are explored. Some general criteria are also built and leveraged to provide a simple way to describe existing quasisymmetric designs. This constitutes the first step in a program to identify quasisymmetric configurations with a reduced set of functions and parameters, to deepen understanding of configuration space, and offer an alternative approach to stellarator optimization that begins with the magnetic axis and builds outward.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Extending near-axis equilibria in DESC

    physics.plasm-ph 2025-06 conditional novelty 7.0 of 10

    The paper derives linear Fourier-Zernike constraints that make global DESC equilibria match a prescribed near-axis expansion through second order in the flux-surface radius.

  2. Periodic Korteweg-de Vries soliton potentials generate quasisymmetric magnetic field strength in a finite plasma-beta equilibrium

    physics.plasm-ph 2025-07 conditional novelty 6.0 of 10

    Quasisymmetric stellarator field strengths satisfy a cubic or quartic relation between (dB/dℓ)^2 and B, determined by three or four flux functions, even at finite beta.

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