Establish the physical adequacy of collisional cold-plasma modeling at low-density ICRF antenna edges

Establish whether macroscopic rectified sheaths in low-density ICRF antenna structures interact non-conservatively with electrons through Fermi acceleration or stochastic heating, thereby raising the electron temperature above its thermal-equilibrium value and making collisional cold-plasma, or even Maxwellian hot-plasma, descriptions inadequate.

Background

The paper shows that physical collisions regularize the lower-hybrid and resonance-cone singularities predicted by collisionless cold-plasma theory, but the resulting electric-field peaks remain confined to very short length scales. The authors emphasize that the neutral density controls these regularizing scales and that the neutral density in the antenna private scrape-off layer is poorly constrained.

A separate unresolved issue concerns the validity of the collisional cold-plasma description itself. At low density, rectified sheaths can become macroscopic and may interact non-conservatively with electrons, potentially causing stochastic heating or Fermi acceleration. If this raises the electron temperature substantially above its thermal-equilibrium value, both collisional cold-plasma and possibly Maxwellian hot-plasma models could become inappropriate for describing ICRF-frequency behavior inside antenna structures.

References

The physical adequacy of the collisional cold plasma description remains a separate question. In this low-density regime, the rectified sheaths become macroscopic, a point routinely neglected when modeling the sheath as a boundary condition. These wide sheaths may interact non-conservatively with electrons (``Fermi acceleration'' or stochastic heating) and may cause the electron temperature to rise well above its thermal equilibrium value, making collisional cold plasma (and possibly even Maxwellian hot plasma) an inadequate description. Whether this occurs at ICRF frequencies inside antenna structures is not established.