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Anisotropic superconductors between types I and II
Self-duality or matching between the magnetic and the condensate coherence lengths is a fundamental property
of isotropic superconductors at the critical Bogomolnyi point (B point). The self-dual state of the condensate
is infinitely degenerate, which is the core reason for the sharp transition between the superconductivity types in
the nearest vicinity of the critical temperature Tc. Below Tc nonlocal interactions in the condensate remove
the degeneracy, which leads to the appearance of a finite intertype (IT) domain between types I and II. This
domain exhibits the mixed state with exotic field-condensate configurations and nonstandard magnetic response,
which cannot be understood within the dichotomy of the conventional superconductivity types. At a first glance,
this picture does not apply to an anisotropic system because no spatial matching between the condensate and
magnetic field can be generally expected for direction-dependent characteristic lengths. However, contrary
to these expectations, here we demonstrate that anisotropic superconductors follow the same scenario of the
interchange between types I and II. In anisotropic materials the IT domain is governed by the B point of the
effective isotropic model obtained by the appropriate scaling transformation of the initial anisotropic formalism.
This transformation depends on the direction of the applied magnetic field, and thus the superconductivity type
of strongly anisotropic materials can be dependent on this direction.