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1 2⊃′ becomes real, the Hamiltonian becomes symmetric under 12⊃′ and one can use the same solution as in Ref.. That is why we call this solution "symmetric."
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1 2 ⊃′ becomes real, the Hamiltonian becomes symmetric under 1 ↔ 2 ⊃′ and one can use the same solution as in Ref.. That is why we call this solution "symmetric."
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