Magnetized Transport and Stability era
In magnetized plasma transport and stability (1958-1980), Hideaki Hasegawa and Kazuo Mima introduced the drift-wave paradigm with the Hasegawa-Mima equation, providing a concise reduced model for cross-field transport and turbulence in strong magnetic fields. The resistive instability framework of Furth, Killeen, and Rosenbluth established the foundational theory of tearing modes in tokamaks, linking finite resistivity to magnetic island formation and confinement limits. P. H. Rutherford advanced nonlinear tearing-mode theory, describing the growth and saturation of magnetic islands and the resulting macroscopic relaxation processes that shaped toroidal confinement. Boris Kadomtsev and collaborators extended stability and reconnection theory to finite-beta plasmas, connecting magnetic geometry, boundary-layer physics, and topological relaxation to confinement outcomes.