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3 of 212 and 213 is the exception. In this case, the two degenerate chiral fermions belong to a single 4d IR.
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3 of 212 and 213 is the exception. In this case, the two degenerate chiral fermions belong to a single 4d IR.
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We have also examined the "physically irreducible" 2d representations, i.e., pairs of conjugate 1d representations degenerate by TRS. These are never compatible with the Weyl Hamiltonian.
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We have also examined the "physically irreducible" 2d representations, i.e., pairs of conjugate 1d representations degenerate by TRS. These are never compatible with the Weyl Hamiltonian.
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