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Parity and Spin CFT with boundaries and defects
by Ingo Runkel, Lóránt Szegedy, Gérard M. T. Watts
This Submission thread is now published as
Submission summary
Authors (as registered SciPost users):  Lóránt Szegedy · Gerard Watts 
Submission information  

Preprint Link:  https://arxiv.org/abs/2210.01057v2 (pdf) 
Date accepted:  20230915 
Date submitted:  20230719 08:05 
Submitted by:  Szegedy, Lóránt 
Submitted to:  SciPost Physics 
Ontological classification  

Academic field:  Physics 
Specialties: 

Abstract
This paper is a followup to [arXiv:2001.05055] in which twodimensional conformal field theories in the presence of spin structures are studied. In the present paper we define four types of CFTs, distinguished by whether they need a spin structure or not in order to be welldefined, and whether their fields have parity or not. The cases of spin dependence without parity, and of parity without the need of a spin structure, have not, to our knowledge, been investigated in detail so far. We analyse these theories by extending the description of CFT correlators via threedimensional topological field theory developed in [arXiv:hepth/0204148] to include parity and spin. In each of the four cases, the defining data are a special Frobenius algebra $F$ in a suitable ribbon fusion category, such that the Nakayama automorphism of $F$ is the identity (oriented case) or squares to the identity (spin case). We use the TFT to define correlators in terms of $F$ and we show that these satisfy the relevant factorisation and singlevaluedness conditions. We allow for world sheets with boundaries and topological line defects, and we specify the categories of boundary labels and the fusion categories of line defect labels for each of the four types. The construction can be understood in terms of topological line defects as gauging a possibly noninvertible symmetry. We analyse the case of a $\mathbb{Z}_2$symmetry in some detail and provide examples of all four types of CFT, with BershadskyPolyakov models illustrating the two new types.
Published as SciPost Phys. 15, 207 (2023)
Author comments upon resubmission
{\bf Report 1 and reply}
The authors discuss the structures of RCFTs graded by parity and in the presence of spin structures. The paper builds upon previous work by the authors and incorporates the most general RCFT observables that involve defects and boundaries. The exposition is comprehensive, clear and skillfully illustrated. It clarifies various subtleties in the literature on such RCFTs. This will be a very useful reference to learn about these RCFTs and certainly deserves to be published.
Some minor comments:
 While the authors focus on RCFT in this paper, it maybe worthwhile to briefly comment on how some of the constructions can be generalized to general 2d CFT which may not be rational (e.g. gauging a special Frobenius algebra F which does not rely on starting with an underlying modular tensor category) .
Reply:
We have added some comments at the end of section 1.5
 The authors mention in the abstract that the construction (gauging F) is like "as gauging a possibly noninvertible symmetry". This was not mentioned in the main text. It would be good to mention and clarify this point (e.g. when and how it becomes noninvertible).
Reply:
We have explained the relation to gauging symmetries and added an example of a noninvertible symmetry and its gauging in section 1.5. In any given CFT, a symmetry (in the sense of an indecomposable topological defect) is either invertible or noninvertible. A symmetry may become noninvertible after gauging a different symmetry, but we do not need this in our construction and would prefer not to comment on it.
 The main general construction of type 4 spin CFT comes from gauging F in a type 2 CFT as stated in Sec 1.5. This is related but different from the usual fermionization construction (which starts from type 1). Just for clarity, in discussing the Ising example (similarly for the other examples), it may be good to fill in the empty boxes in the table (7.12) below (7.11).
Reply:
There are two related constructions in this paper which both actually start with a type 1 CFT and which result in a theory without parity (bosonic theory'') using the algebra $A_+$, and a theory with parity (
fermionic theory'') using the algebra $A_$.
Depending on the details of the theory, using $A_+$ will result in a theory of type 3 or of type 1 (which is a type 3 theory which is actually insensitive to the spin structure), and using $A_$ will result in a theory of type 4 or of type 2 (which is a type 4 theory which is actually insensitive to the spin structure). The examples in section 7 cover all four of these cases.
The construction of a theory of type 4 starts with a theory of type 1 which is extended to a theory of type 2 and then gauged to get the desired theory of type 4. This is indeed different to the ``usual" fermionisation procedure which starts with the a theory of 1, tensors with Arf to get a trivial tensor product theory of type 4 and then gauges to get the desired theory of type 4.
We have attempted to make this clearer by
\begin{itemize}
\item adding text on how the different types relate in more detail and how the spin theories of types 3 and 4 are constructed at the end of sections 1.2 and 1.3,
\item adding a discussion of how the Arf 2d TFT fits into the our construction in section 7.1,
\item adding a discussion on how our results relate to these in [HNT] in the case of $c=4/5$ minimal models in section 7.4.4.
\end{itemize}
In the Ising example, the table (7.11) is intended to show which two theories can be constructed by $A_\pm$, and since only two are possible, this is why only two boxes are filled. In the same way, the tables in sections 7.4.1 (now numbered (7.22)) and at the end of section 7.5.1 (now numbered (7.46)) also show only two boxes filled, as these are the two theories that can be constructed using $A_\pm$.
We think it would actually be confusing to include the intermediate stage CFTs in these boxes, when applicable.
 Usual fermionization map from bosonic to fermionic (spin) CFT comes with a choice (e.g. by stacking with fermionic SPT). It would be good to mention where that choice is contained in the construction here (e.g. in the F algebra).
Reply:
There are indeed choices made in this paper.
The first choice is in the construction of the fermionic CFT from the category $\hat\Cc$. We have to make a choice of how to construct a spin theory from $\hat\Cc$ and a Frobenius algebra $A$. Thereafter, all the choices lie in the choice of $A$. We have chosen what seemed the most natural construction. Other choices of construction are also possible, but are equivalent to changing the choice of algebra, so we have not elaborated on this in the paper.
The second choice is the choice of Frobenius algebra $A$  we give examples of algebras which lead to particular CFTs. Morita equivalent algebras lead to the same CFTs, but there can be more than one Morita equivalence class, and so more than one CFT that can be defined from a given $\hat\Cc$  indeed, when the Ramond parityswap leads to an inequivalent theory, there will be two inequivalent Frobenius algebras which give the two theories related by parityswapping the Ramond sector. Not surprisingly since the Arf theory is given by the choice of the Clifford algebra as the Frobenius algebra, the Ramondparity swap operation is given by tensoring the Frobenius algebra with the Clifford algebra. We have included an explicit comparison to other constructions in the new section 7.4.4, although we defer the details of the Ramond parityswap to a later paper.
{\bf Report 2 and reply}
This work gives a detailed discussion of four types of 2d CFTs depending on whether they have spin structure and/or parity dependence on the local fields. Following the notations of eq.(1.2), the diagonal cases 1 and 4 are better understood, and the offdiagonal cases 2 and 3 are new to this work. The presentation are clear, rigorous, and contains enough details. This result is definitely worth to be published, and the referee recommends so.
It would be nice if the authors can clarify further on the following points:
 In the case of Z2 symmetry, the authors clarified in Sec. 7.1 that the CFTs of offdiagonal types, i.e. 2 and 3, are nonunitary, while the diagonal types 1 and 4 are unitary.
Reply:
We have moved section 7.1 to 7.2 and added a comment on the unitarity of the various theories, to the effect that for the examples considered there types 2 and 3 are necessarily nonunitary but 1 and 4 can be either, depending on the details of the model.
 It is known, e.g. in [KTT] and [HNT] as cited in the current work, that starting with 1, gauging Z2 while introducing the spin structure dependence (via including an Arf term), leads to 4. This is known as the fermionisation map and is indeed described in Sec.7.2. However, in the introduction Sec.1.5, the authors commented that starting with 2 and performing a (possibly different) gauging of topological symmetry, one leads to 4. It would be useful if the authors could clarify the difference between the normal fermionisation map 1$\to$4 and the “new gauging” 2$\to$4. In particular, how to understand a nonunitary theory 2 is mapped to a unitary theory 4? This would help the readers to understand the relations between four types of CFTs better.
Reply:
Our procedure is to start with type 1, allow for defects with parity, resulting in a theory of type 2 (but the bulk theory is still type 1  so no contradiction with unitarity), and then gauging a defect to arrive at type 4. This is now explained in more detail at the end of section 1.3. We have added section 7.4.4 to explain in an example how our construction produces the different theories in [HNT].
List of changes
See in author comments.
Submission & Refereeing History
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