  Mirror modes in collisionless high-temperature plasmas represent macroscopic
high-temperature quasi-superconductors with bouncing electrons in
discrete-particle resonance with thermal ion-sound noise contributing to the
ion-mode growth beyond quasilinear stability. In the semi-classical GL
approximation the conditions for phase transition are given. The
quasi-superconducting state is of second kind causing a magnetically perforated
plasma texture. Focussing on the interaction of mirror bubbles we apply
semi-classical Josephson conditions and show that a mirror perforated plasma
emits weak electromagnetic radiation which in the magnetosheath is in the
sub-millimeter respectively infrared range.
