It is demonstrated that the known for a long time transition between
the gap and the gapless states in the Abrikosov-Gor’kov theory of a
superconductor with paramagnetic impurities is of the Lifshitz type,
i.e. of the 2\frac12212
order phase transition. We reveal the emergence of a cuspidal edge at
the density of states surface N(\omega,\Delta_0)N(ω,Δ0)
(\Delta_0Δ0
is the value of the superconducting order parameter in the absence of
magnetic impurities) and the occurrence of the catastrophe phenomenon at
the transition point. We study the stability of such a transition with
respect to the spatial fluctuations of the magnetic impurities critical
concentration n_sns
and show that the requirement for validity of its mean field description
is unobtrusive: \nabla \left( {\ln{n_s}} \right) \ll \xi^{-1}∇(lnns)≪ξ−1 (here \xiξ
is the superconducting coherence length). Finally, we show that,
similarly to the Lifshitz transition, the transition between gap and
gapless states should be accompanied by the corresponding singularities.
For instance, the superconducting thermoelectric effect has a giant peak
exceeding the normal value of the Seebeck coefficient by the ratio of
the Fermi energy and the superconducting gap. The concept of the
experiment for the confirmation of 2\frac12212
order transition nature is proposed. The obtained theoretical results
can be applied for the explanation of recent experiments with
lightwave-driven gapless superconductivity, for the new interpretation
of the disorder induced transition s_{\pm}s±-s_{++}s++
states via gapless state in multi-band superconductors, for better
understanding of the gapless color superconductivity in quantum
chromodynamics, the string theory.