2017
DOI: 10.1007/jhep08(2017)077
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Counting and construction of holomorphic primary fields in free CFT4 from rings of functions on Calabi-Yau orbifolds

Abstract: Counting formulae for general primary fields in free four dimensional conformal field theories of scalars, vectors and matrices are derived. These are specialised to count primaries which obey extremality conditions defined in terms of the dimensions and left or right spins (i.e. in terms of relations between the charges under the Cartan subgroup of SO(4, 2)). The construction of primary fields for scalar field theory is mapped to a problem of determining multi-variable polynomials subject to a system of symme… Show more

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Cited by 21 publications
(34 citation statements)
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“…28 On the other hand parity odd S-matrices are even function of the ⊥ i (and hence of α i ) when D is odd, but an odd function of both ⊥ i and α i when D is even. 29 We have already explained (see around (2.21) ) that it is convenient to regard parity odd S-matrices as functions of ε D−3 (see (2.19) 27 We can also see this in another way. It follows from (2.12) that |αi| 2 is completely physical, so permutations act on |αi| 2 in the usual way; once again we see that the ambiguity is in the sign.…”
Section: Jhep02(2020)114mentioning
confidence: 97%
“…28 On the other hand parity odd S-matrices are even function of the ⊥ i (and hence of α i ) when D is odd, but an odd function of both ⊥ i and α i when D is even. 29 We have already explained (see around (2.21) ) that it is convenient to regard parity odd S-matrices as functions of ε D−3 (see (2.19) 27 We can also see this in another way. It follows from (2.12) that |αi| 2 is completely physical, so permutations act on |αi| 2 in the usual way; once again we see that the ambiguity is in the sign.…”
Section: Jhep02(2020)114mentioning
confidence: 97%
“…Previous studies [7] have explained how to map the algebraic problem of constructing primary fields in the quantum field theory of a free scalar field φ in four dimensions to one of finding polynomial functions on (R 4 ) n that are harmonic, translation invariant and which are in the trivial representation of S n . In this article, we have extended this construction to describe primary fields in the free quantum field theory of a single Weyl fermion.…”
Section: Discussionmentioning
confidence: 99%
“…The above formula produces an expression of the form in i P i (Z) wheren i are unit vectors inside the carrier space of V ⊗k H and P i (Z) are the polynomials that correspond to primary operators. To translate polynomials into momenta, the formula [7] z k ↔ (−1) k P k 2 k k! , (3.39) that we derived above, is very useful.…”
Section: )mentioning
confidence: 99%
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