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We revisit the problem of boundary excitations at a topological boundary or junction defects between topological boundaries in non-chiral bosonic topological orders in 2+1 dimensions.
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Note1, this should be contrasted with the W W matrix discussed for example in [ 2 ] , in which the x x indices contain only “unconfined” sectors
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Note2, from the examples we have worked with, it appears that M c M_{c} is proportional to δ i j \delta_{ij} , which is explicit in the examples built from gauge theories. We also expect that to be a natural result as we break an anyon line into two at the boundary
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