Theory for Intrinsic Magnetic Field in Chiral Superconductor Measured by \muSR: Case of Sr_2RuO_4

Abstract

The local magnetic field induced by $μ^{+}$ trapped at an interstitial site in a chiral superconductor with $p$-wave symmetry, such as Sr$_2$RuO$_4$, is discussed by solving the Bogoliubov-de Gennes equation on the two-dimensional square lattice. In the model Hamiltonian, the effect of the trapped $μ^{+}$ extracting the electrons at surrounding Ru sites is phenomenologically taken into account as a non-magnetic impurity potential which locally destroys the chiral superconducting order with $p$-wave symmetry giving rise to local circulating current around $μ^{+}$ site. It is shown that the size of the induced local magnetic field in the case with periodic boundary condition is far smaller compared to the case with open boundary condition without $μ^{+}$, in which the surface current induced by destruction of superconducting order at the surface boundary gives contribution corresponding to the intrinsic angular momentum of the order of $\hbar N_{\rm s}/2$, with $N_{\rm s}$ being the number of superconducting electrons. This result qualitatively explains why the magnetic field $\simeq0.5$G measured by $μ$SR in Sr$_2$RuO$_4$ is far smaller than the expected intrinsic magnetic field $\simeq 50$G which is nearly the same as the lower critical field $H_{{\rm c}1}\simeq 50$G.