We analytically evaluate the entanglement spectra of the superconductivitystates in graphene, primarily focusing on the s-wave and chiral $d_{x^{2}-y^{2}}+id_{xy} $ superconductivity states. We demonstrate that thetopology of the entanglement Hamiltonian can differ from that of the subsystemHamiltonian. In particular, the topological properties of the entanglementHamiltonian of the chiral $ d_{x^{2}-y^{2}}+id_{xy} $ superconductivity stateobtained by tracing out one spin direction clearly differ from those of thetime-reversal invariant Hamiltonian of noninteracting fermions on the honeycomblattice.
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