Theoretically predicted by Alexei Abrikosov in 1957 based on Ginzburg-Landau theory, Type II superconductors are characterized by two critical magnetic fields, \(H_{c1}\) and \(H_{c2}\). Between these fields, they enter a mixed or “vortex” state, allowing partial magnetic field penetration through quantized flux tubes called Abrikosov vortices. This allows them to remain superconducting in much higher magnetic fields than Type I superconductors.





