Abstract

For a single free scalar field in d ≥ 2 dimensions, almost all the unitary conformal defects must be ‘trivial’ in the sense that they cannot hold interesting dynamics. The only possible exceptions are monodromy defects in d ≥ 4 and co-dimension three defects in d ≥ 5. As an intermediate result we show that the n-point correlation functions of a conformal theory with a generalized free spectrum must be those of the generalized free theory.

Highlights

  • The rationale for this pattern is as follows

  • On the defect the local operators are organized in representations of so(p + 1, 1) × so(q), with the first factor acting as the usual conformal algebra in p dimensions and the latter as a usual global symmetry — neither of these symmetries is generated by a local current on the defect

  • This work contains some more general results, our main outcome is that most defects in the free scalar theory are ‘trivial’ in the sense that there is no room for any interesting dynamics on the defect: up to potentially an undetermined one-point function, all the n-point correlation functions of the bulk field φ are completely fixed

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Summary

Summary

An expansion like equation (1.3) completely fixes the two-point function of the bulk field φ, but more work is required to constrain the higher-point functions: we have to learn about the defect OPE of the operators ψs(+) themselves.

The two-point function of the free scalar
General form of the two-point functions
Two-point functions of the free scalar
Constraining defect interactions
Bulk-defect-defect three-point functions
Constraints from analyticity
Reconstructing the bulk
The defect-channel expansion
Consistency with the bulk OPE
Triviality of defects of dimension 2 and higher
Triviality of line defects
Analytic continuation to line defects
Line defects and generalized free field theories
Tests in conformal perturbation theory
Coupling the trivial defect to lower-dimensional matter
A nearly marginal deformation in free theory
A monodromy defect in free theory
Applications
A Details of the scalar bulk-to-defect OPE
C Three-point functions from the bulk-to-defect OPE
Full Text
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