First-order chiral to non-chiral transition in the angular dependence of the upper critical induction of the Scharnberg-Klemm $p$-wave pair state

We calculate the temperature $T$ and angular $(θ,ϕ)$ dependence of the upper critical induction $B_{c2}(θ,ϕ,T)$ for parallel-spin superconductors with an axially symmetric $p$-wave pairing interaction pinned to the lattice and a dominant ellipsoidal Fermi surface (FS). For all FS anisotropies, the chiral Scharnberg-Klemm state $B_{c2}(θ,ϕ,T)$ exceeds that of the chiral Anderson-Brinkman-Morel state, and exhibits a kink at $θ=θ^{*}(T,ϕ)$, indicative of a first-order transition from its chiral, nodal-direction behavior to its non-chiral, antinodal-direction behavior. Applicability to Sr$_2$RuO$_4$, UCoGe, and topological superconductors such as Cu$_x$Bi$_2$Se$_3$ is discussed.

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