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END USER LICENCE AGREEMENTEnd User License Agreement • August 22nd, 2018
We can make our theory topological by redefining these algebraic relations, which gives us a way of preserving only states which are not subject to spacetime transformations. Topological twisting [69, 95] is a redefinition of the stress energy tensor by the U(1) cur- rent which leaves only the topologically invariant states. There are two types of twist, A and B, but we only need to look at the B-twist in order to understand the correspondence with topological states in LG models. The surviving states are the chiral primary states discussed above. First we make the B-twist transformations
END USER LICENCE AGREEMENTEnd User License Agreement • August 22nd, 2018
We can make our theory topological by redefining these algebraic relations, which gives us a way of preserving only states which are not subject to spacetime transformations. Topological twisting [69, 95] is a redefinition of the stress energy tensor by the U(1) cur- rent which leaves only the topologically invariant states. There are two types of twist, A and B, but we only need to look at the B-twist in order to understand the correspondence with topological states in LG models. The surviving states are the chiral primary states discussed above. First we make the B-twist transformations
