Large Chern Number and Edge Currents in Sr2RuO4

We show from a weak coupling microscopic calculation that the most favored chiral superconducting order parameter in Sr2RuO4 has Chern number |C|=7. The two dominant components of this order parameter are given by sin(3 kx) + i sin(3 ky) and sin(kx) cos(ky) + i sin(ky) cos(kx) and lie in the same irreducible representation Eu of the tetragonal point group as the usually assumed gap function sin(kx) + i sin(ky). While the latter gap function leads to C=1, the two former lead to C=-7, which is also allowed for an Eu gap function since the tetragonal symmetry only fixes C modulo 4. Since it was shown that the edge currents of a |C|>1 superconductor vanish exactly in the continuum limit, and can be strongly reduced on the lattice, this form of order parameter could help resolve the conflict between experimental observation of time-reversal symmetry breaking and yet the absence of observed edge currents in Sr2RuO4.

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