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Dagger nn-categories

Giovanni Ferrer, Brett Hungar, Theo Johnson-Freyd, Cameron Krulewski, Lukas Müller, Nivedita, David Penneys, David Reutter, Claudia Scheimbauer, Luuk Stehouwer, Chetan Vuppulury
Abstract.

We present a coherent definition of dagger (,n)(\infty,n)-category in terms of equivariance data trivialized on parts of the category. Our main example is the bordism higher category 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X}. This allows us to define a reflection-positive topological quantum field theory to be a higher dagger functor from 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} to some target higher dagger category 𝒞\mathcal{C}. Our definitions have a tunable parameter: a group GG acting on the (,1)(\infty,1)-category 𝐂𝐚𝐭(,n)\mathbf{Cat}_{(\infty,n)} of (,n)(\infty,n)-categories. Different choices for GG accommodate different flavours of higher dagger structure; the universal choice is G=Aut(𝐂𝐚𝐭(,n))=(/2)nG=\operatorname{Aut}(\mathbf{Cat}_{(\infty,n)})=(\mathbb{Z}/2\mathbb{Z})^{n}, which implements dagger involutions on all levels of morphisms.

The Stratified Cobordism Hypothesis suggests that there should be a map PL(n)Aut(𝐀𝐝𝐣𝐂𝐚𝐭(,n))\mathrm{PL}(n)\to\operatorname{Aut}(\mathbf{AdjCat}_{(\infty,n)}), where PL(n)\mathrm{PL}(n) is the group of piecewise-linear automorphisms of n\mathbb{R}^{n} and 𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)} the (,1)(\infty,1)-category of (,n)(\infty,n)-categories with all adjoints; we conjecture more strongly that Aut(𝐀𝐝𝐣𝐂𝐚𝐭(,n))PL(n)\operatorname{Aut}(\mathbf{AdjCat}_{(\infty,n)})\cong\mathrm{PL}(n). Based on this conjecture we propose a notion of dagger (,n)(\infty,n)-category with unitary duality or PL(n)\mathrm{PL}(n)-dagger category. We outline how to construct a PL(n)\mathrm{PL}(n)-dagger structure on the fully-extended bordism (,n)(\infty,n)-category 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} for any stable tangential structure XX; our outline restricts to a rigorous construction of a coherent dagger structure on the unextended bordism (,1)(\infty,1)-category 𝐁𝐨𝐫𝐝n,n1X\mathbf{Bord}_{n,n-1}^{X}. The article is a report on the results of a workshop held in Summer 2023, and is intended as a sketch of the big picture and an invitation for more thorough development.

In June 2023, we gathered for an online workshop on “Dagger Higher Categories”The workshop schedule and participant list can be found at http://categorified.net/dagger2023.html.. The goal of the workshop was the following. Many of us had some thoughts and ideas on what a “dagger higher category” should be, but there was no proposal for a full definition. Through compiling and comparing ideas, we hoped to emerge with a complete consensus definition, including nontrivial examples. This goal was met with great success. In this article, we will elaborate on our findings. Our discussion will focus on the essential ideas and will be short on technical details and essentially devoid of proofs; for this reason, we will refer to “statements” rather than “lemmas” or “theorems,” and strictly speaking all statements herein (other than those cited to the published literature) carry the ontological status of conjectures. We also list some true “conjectures,” of whose veracity we are less confident. Our goal is to sketch the big picture, and we hope that our article can serve as a blueprint for a more thorough development of the subject.

1. Dagger 1-categories

Categories with an (anti-)involution have been studied since the early days of category theory [ML61, Pup62]. A familiar example is the category of Hilbert spaces and bounded linear maps, with an involution ()(-)^{\dagger} given by the usual notion of adjoint map. The notion of a complex *-category and notions of C\rm C^{*}- and W\rm W^{*}-category in the complex linear setting were introduced in [GLR85] and have been studied extensively in the C\rm C^{*} tensor setting [FK93, DR89, LR97, Wen98, M0̈3, Yam04].

Roughly, an involution ()(-)^{\dagger} should reverse the direction of morphisms in a compatible way. In [Sel07], the following notion was introduced in the non-linear setting. A category 𝒞\mathcal{C} is a dagger category if it is equipped with a bijection ():hom(x,y)hom(y,x)(-)^{\dagger}:\hom(x,y)\to\hom(y,x) for each pair (x,y)(x,y) of objects, such that (f)=f(f^{\dagger})^{\dagger}=f and (fg)=gf(f\circ g)^{\dagger}=g^{\dagger}\circ f^{\dagger} for all composable morphisms f,gf,g. In other words, ()(-)^{\dagger} is a functor 𝒞𝒞op\mathcal{C}\to\mathcal{C}^{\mathrm{op}} which is involutive and the identity on (the set of) objects.

This definition is evil in the following sense [Hen15]: since it explicitly references the set of objects in 𝒞\mathcal{C}, dagger structures cannot be readily transported along general equivalences of categories. In detail: given a dagger category (𝒞,())(\mathcal{C},(-)^{\dagger}) and an equivalence F:𝒞𝒟F:\mathcal{C}\simeq\mathcal{D} with (weak) inverse F1F^{-1}, the transported “dagger” functorA different formula for the transported structure supplies a dagger structure on 𝒟\mathcal{D} such that F1F^{-1} is a dagger functor [Kar18, Lemma 2.1.16], but then FF will typically not only fail to be a dagger equivalence, it will fail to be compatible with the dagger structures at all. F()F1:𝒟𝒟opF\circ(-)^{\dagger}\circ F^{-1}:\mathcal{D}\to\mathcal{D}^{\mathrm{op}} is naturally part of a weak involution in the sense that its square is coherently-isomorphic to id𝒟\mathrm{id}_{\mathcal{D}}, but it will almost never be an identity on objects. We violated the general rule of thumb: from a category, one can coherently extract its groupoid of objects up to isomorphism, but not its set of objects. Non-evil notions refer only to coherently-extractable data.

Nevertheless, there is a well-developed “dagger category theory” that parallels the usual theory of categories, with dagger versions of functor, natural transformation, and the like [GLR85, LR97, Yam04, HP17, JP17, Kar18, HK16, HK19, Sri21]. From the perspective of dagger category theory, the coherently-extractable space of objects is the groupoid of objects and unitary isomorphism.

With this in mind, [SS23] developed the following ideas. Consider the (2,1)(2,1)-category 𝐂𝐚𝐭\mathbf{Cat} of 11-categories, functors and natural isomorphisms. This (2,1)(2,1)-category carries a /2\mathbb{Z}/2\mathbb{Z}-action which sends 𝒞𝒞op\mathcal{C}\mapsto\mathcal{C}^{\mathrm{op}}. An anti-involutive category is a homotopy fixed point for this action: explicitly, it consists of a category 𝒞\mathcal{C}, a categorical equivalence :𝒞𝒞op\dagger:\mathcal{C}\overset{\sim}{\to}\mathcal{C}^{\mathrm{op}}, and a natural isomorphism η:opid𝒞\eta:\dagger^{\mathrm{op}}\circ\dagger\overset{\sim}{\Rightarrow}\mathrm{id}_{\mathcal{C}}, such that for each object x𝒞x\in\mathcal{C}, ηx1=(ηx)\eta_{x^{\dagger}}^{-1}=(\eta_{x})^{\dagger}.

If 𝒢\mathcal{G} is a groupoid, then 𝒢\mathcal{G} and 𝒢op\mathcal{G}^{\mathrm{op}} are canonically equivalent via the functor that is the identity on objects and sends morphisms to their inverses. In other words, the /2\mathbb{Z}/2\mathbb{Z}-action 𝒞𝒞op\mathcal{C}\mapsto\mathcal{C}^{\mathrm{op}} on 𝐂𝐚𝐭\mathbf{Cat} trivializes when restricted to the full sub-(2,1)(2,1)-category 𝐆𝐩𝐝𝐂𝐚𝐭\mathbf{Gpd}\subset\mathbf{Cat} of groupoids. In particular, given an anti-involutive category 𝒞\mathcal{C}, the groupoid ι0𝒞\iota_{0}\mathcal{C} of objects of 𝒞\mathcal{C} inherits a coherent action by /2\mathbb{Z}/2\mathbb{Z}. Let (ι0𝒞)/2(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} denote the groupoid of homotopy fixed points for this action.

As a motivating example, consider 𝒞=𝐕𝐞𝐜fd\mathcal{C}=\mathbf{Vec}^{\mathrm{fd}}_{\mathbb{C}} the category of finite-dimensional vector spaces, and :VV¯\dagger:V\mapsto\overline{V}^{\vee} the functor that assigns the complex-conjugate dual of a vector space. Then (ι0𝒞)/2(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} is the groupoid of finite-dimensional Hermitian vector spaces, i.e. vector spaces equipped with a nondegenerate conjugate-symmetric sesquilinear form which might not be positive-definite, and “unitary” isomorphisms thereof. In order to encode the theory of Hilbert spaces, we must specify extra data: we must mark some of the Hermitian spaces as preferred, and leave out the others. This marking restricts the set of objects of (ι0𝒞)/2(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}, but keeps all unitary isomorphisms between them; in other words, the marked subspace 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\subset(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} should be a full subgroupoid. If there were a vector space that did not admit a Hilbert structure, then we should have already excised it from 𝒞\mathcal{C}; in other words, the composition 𝒞0(ι0𝒞)/2𝒞\mathcal{C}_{0}\subset(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}\to\mathcal{C} should be essentially surjective.

Definition 1.1.

A coherent dagger 1-category is an anti-involutive category (𝒞,)(\mathcal{C},\dagger) together with a fully faithful subgroupoid 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\hookrightarrow(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} such that the induced map 𝒞0(ι0𝒞)/2ι0𝒞\mathcal{C}_{0}\hookrightarrow(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}\to\iota_{0}\mathcal{C} is essentially surjective. A morphism between coherent dagger 1-categories is a functor respecting the anti-involutions and the subgroupoids.

Coherent dagger structures are non-evil: if 𝒞\mathcal{C} is a dagger category and 𝒞𝒟\mathcal{C}\cong\mathcal{D} an equivalence with an ordinary category, then 𝒟\mathcal{D} acquires a natural coherent dagger structure. The main theorem of [SS23] says that coherent dagger categories are equivalent in the appropriate sense to dagger categories as traditionally defined. Namely, coherent dagger categories can be strictified to dagger categories as traditionally defined:

Theorem 1.2 ([SS23]).

Any dagger category 𝒞\mathcal{C} defines a coherent dagger category by keeping 𝒞\mathcal{C} and \dagger as-is, and setting 𝒞0\mathcal{C}_{0} to be the groupoid of objects in 𝒞\mathcal{C} and unitary morphisms between them. The so-defined functor from the (2,1)(2,1)-category of dagger categories, dagger functors, and unitary natural isomorphisms to the (2,1)(2,1)-category of coherent dagger categories is an equivalence.

Its inverse assigns to a coherent dagger category (𝒞,,𝒞0(ι0𝒞)/2)(\mathcal{C},\dagger,\mathcal{C}_{0}\hookrightarrow(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}) the category whose objects are the objects of 𝒞0\mathcal{C}_{0} and whose morphisms are the morphisms in 𝒞\mathcal{C} between the images of objects; this new category is equivalent to 𝒞\mathcal{C} because of the essential surjectivity axiom, and its anti-involution is strictly trivial on the set of objects.

Definition 1.1 immediately generalizes to the (,1)(\infty,1)-world, where it was independently proposed by [Hen22]. An (,1)(\infty,1)-category is a homotopically-coherent version of “category enriched in spaces.” As is standard in higher category theory, we will interchangeably use the word \infty-groupoid and space for “nice topological space considered up to homotopy.” Then an (,1)(\infty,1)-category has not a set of morphisms between any two objects, but rather a space of morphisms; composition is associative up to parameterized homotopy; this homotopy itself satisfies higher and higher homotopies relating different parenthesizations. There are many ways of axiomatizing the notion of “(,1)(\infty,1)-category,” and we refer the reader to [Ber10, AC16] for nice surveys.

Ignoring size issues, there is an (,1)(\infty,1)-category 𝐂𝐚𝐭(,1)\mathbf{Cat}_{(\infty,1)} whose objects are (,1)(\infty,1)-categories and whose morphisms are (,1)(\infty,1)-functors. There is a functor ι0:𝐂𝐚𝐭(,1)𝐒𝐩𝐚𝐜𝐞\iota_{0}\colon\mathbf{Cat}_{(\infty,1)}\to\mathbf{Space}, corepresented by the terminal (,1)(\infty,1)-category {pt}\{\mathrm{pt}\}, which assigns to each (,1)(\infty,1)-category its space of objects. Moreover, 𝐂𝐚𝐭(,1)\mathbf{Cat}_{(\infty,1)} carries a canonical /2\mathbb{Z}/2\mathbb{Z}-action sending 𝒞𝒞op\mathcal{C}\mapsto\mathcal{C}^{\mathrm{op}} [Toë05]. An anti-involutive (,1)(\infty,1)-category is a (homotopy) fixed point for this action.

As in the 1-categorical case, the /2\mathbb{Z}/2\mathbb{Z}-action on 𝐂𝐚𝐭(,1)\mathbf{Cat}_{(\infty,1)} trivializes on the full subcategory 𝐒𝐩𝐚𝐜𝐞𝐂𝐚𝐭(,1)\mathbf{Space}\subseteq\mathbf{Cat}_{(\infty,1)}. Hence, the space of objects ι0𝒞\iota_{0}\mathcal{C} of any anti-involutive (,1)(\infty,1)-category 𝒞\mathcal{C} inherits a coherent /2\mathbb{Z}/2\mathbb{Z} action, whose homotopy fixed points we continue to denote by (ι0𝒞)/2.(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}.

Definition 1.3.

A dagger (,1)(\infty,1)-category is an anti-involutive (,1)(\infty,1)-category, together with a full sub-\infty-groupoid 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\hookrightarrow(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} such that the induced map 𝒞0(ι0𝒞)/2𝒞\mathcal{C}_{0}\hookrightarrow(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}\to\mathcal{C} is essentially surjective.

Anticipating our nn-dimensional generalization, let us note that part of the data of a dagger (,1)(\infty,1)-category is the space 𝒞0\mathcal{C}_{0}, the (,1)(\infty,1)-category 𝒞\mathcal{C}, and the essential surjection 𝒞0ι0𝒞\mathcal{C}_{0}\to\iota_{0}\mathcal{C}. This structure is called a flagged (,1)(\infty,1)-category. Any specific 11-category 𝒞\mathcal{C} in the traditional sense supplies a flagged (,1)(\infty,1)-category: one takes 𝒞0\mathcal{C}_{0} to be the actual set of objects, whereas ι0𝒞\iota_{0}\mathcal{C} is the groupoid of objects and isomorphisms. In other words, flaggings are a way of remembering “sets” of objects in a way that nevertheless transports coherently. The requirement that 𝒞0ι0𝒞\mathcal{C}_{0}\to\iota_{0}\mathcal{C} be essentially surjective simply means that the data of the homomorphisms between elements of 𝒞0\mathcal{C}_{0} suffices to recover all of 𝒞\mathcal{C} up to categorical equivalence. A flagging is called univalent§§§This is reminiscent of the completeness condition of Segal spaces. if it does not in fact remember any further data: if the map 𝒞0ι0𝒞\mathcal{C}_{0}\to\iota_{0}\mathcal{C} is not just essentially surjective but also fully faithful.

By analogy, in a dagger (,1)(\infty,1)-category, the requirement that 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} be fully faithful will be called the univalence axiom, even though it does not force any map to be an equivalence. And by analogy, dropping the univalence axiom leads to a useful weakening of Definition 1.3.

Definition 1.4.

A flagged dagger (,1)(\infty,1)-category is an anti-involutive (,1)(\infty,1)-category 𝒞\mathcal{C} equipped with a map of spaces 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} such that the induced map 𝒞0(ι0𝒞)/2𝒞\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}\to\mathcal{C} is essentially surjective.

Our motivating example of a flagged dagger (,1)(\infty,1)-category is the higher category of bordisms, which we discuss in Example 6.7.

Whether univalent or not, the flagging should be thought of as recording the “identity on objects” condition in the traditional definition of dagger category. In a flagged dagger category which is not univalent, the groupoid 𝒞0\mathcal{C}_{0} selects a notion of equivalence between objects that is finer than unitary equivalence.

Write 𝐅𝐥𝐂𝐚𝐭(,1)\mathbf{Fl{\dagger}Cat}_{(\infty,1)} for the (,1)(\infty,1)-category of flagged dagger (,1)(\infty,1)-categories: the homomorphisms are the obvious ones which preserve the equivariance and the flaggings. Write 𝐂𝐚𝐭(,1){\dagger}\mathbf{Cat}_{(\infty,1)} for the full subcategory of 𝐅𝐥𝐂𝐚𝐭(,1)\mathbf{Fl}{\dagger}\mathbf{Cat}_{(\infty,1)} on the univalent ones.

Statement 1.5.

The inclusion

𝐂𝐚𝐭(,1)𝐅𝐥𝐂𝐚𝐭(,1){\dagger}\mathbf{Cat}_{(\infty,1)}\hookrightarrow\mathbf{Fl{\dagger}Cat}_{(\infty,1)}

admits a left adjoint, which replaces 𝒞0\mathcal{C}_{0} with the full subgroupoid inside (ι0𝒞)/2(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} on the essential image of 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}.

One benefit of Statement 1.5 is that it can be easier to present flagged dagger categories than their univalentizations. Indeed, most (,1)(\infty,1)-categories 𝒞\mathcal{C} of interest (for example the bordism categories discussed in Section 6) come with distinguished flaggings 𝒞0𝒞\mathcal{C}_{0}\to\mathcal{C}, and sometimes this flagged category is naturally anti-involutive in the sense that 𝒞\mathcal{C} is anti-involutive and 𝒞0ι0𝒞\mathcal{C}_{0}\to\iota_{0}\mathcal{C} is /2\mathbb{Z}/2\mathbb{Z}-equivariant. To promote this to a flagged dagger structure then merely requires a trivialization of the /2\mathbb{Z}/2\mathbb{Z}-action on 𝒞0\mathcal{C}_{0}. Speaking very approximately, it can be easier to do this when 𝒞0\mathcal{C}_{0} has very few morphisms requiring trivialization data.

Instead of dropping the univalence axiom, we could instead drop the essential surjectivity condition:

Definition 1.6.

A coflagged dagger (,1)(\infty,1)-category is an anti-involutive (,1)(\infty,1)-category 𝒞\mathcal{C} equipped with a fully faithful inclusion of spaces 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\hookrightarrow(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}.

Comparing to Definition 1.1, a coflagged dagger (,1)(\infty,1)-category can be thought of as an anti-involutive (,1)(\infty,1)-category equipped with the data of Hermitian pairings on some but not necessarily all objects.

Statement 1.7.

Writing 𝐜𝐨𝐅𝐥𝐂𝐚𝐭(,1)\mathbf{coFl{\dagger}Cat}_{(\infty,1)} for the (,1)(\infty,1)-category of coflagged dagger (,1)(\infty,1)-categories, the inclusion

𝐂𝐚𝐭(,1)𝐜𝐨𝐅𝐥𝐂𝐚𝐭(,1){\dagger}\mathbf{Cat}_{(\infty,1)}\hookrightarrow\mathbf{coFl{\dagger}Cat}_{(\infty,1)}

admits a right adjoint, which replaces 𝒞\mathcal{C} with its full subcategory on the image of 𝒞0(ι0𝒞)/2𝒞\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}\to\mathcal{C}.

Note that every anti-involutive (,1)(\infty,1)-category is naturally a coflagged dagger (,1)(\infty,1)-category with 𝒞0=(ι0𝒞)/2\mathcal{C}_{0}=(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}. Through this observation, Statement 1.7 specializes to a higher version of the “Hermitian completion” functor of [SS23].

2. Dagger nn-categories via flaggings

The notion of (,n)(\infty,n)-category is designed to formalize categories with an nn-fold hierarchy of directions of composition. As with the (,1)(\infty,1)-case, there are many models, some of which are surveyed in [BR13, BR20, BSP21]. Informally, an (,n)(\infty,n)-category has a space of objects; for each pair of objects, a space of 11-morphisms between them and a coherently-associative and coherently-unital composition law; for each pair of parallel 11-morphisms, a space of 22-morphisms between them, and two (coherently-associative and coherently-unital) composition laws, one of which lifts the composition law of 11-morphisms and the other of which is in the new second dimension; and so on up to dimension nn.

In this informal description of (,n)(\infty,n)-categories in the previous paragraph, we did not specify which maps between them should be considered equivalences. There is a most natural guess if one explained the idea without supplying the name “category”: a homomorphism could be declared an equivalence when it induces equivalences on all spaces of kk-morphisms, including on the space of objects. Comparing with the traditional notion of strict 1-category, this choice would select the strict isomorphisms and not the categorical equivalences. In contrast, categorical equivalence does not remember any specific sets or spaces of kk-morphisms, but merely the higher groupoids thereof. As in the (,1)(\infty,1)-case, the extra data of spaces of morphisms in a presentation of an (,n)(\infty,n)-category is called a flagging of that (,n)(\infty,n)-category [AF18]. Given a correct theory of (,n)(\infty,n)-categories, the notion of flagged (,n)(\infty,n)-category can be defined as follows:

Definition 2.1.

A flagged (,n)(\infty,n)-category is a chain

𝒞0𝒞1𝒞n\mathcal{C}_{0}\to\mathcal{C}_{1}\to\dots\to\mathcal{C}_{n}

where each 𝒞k\mathcal{C}_{k} is an (,k)(\infty,k)-category, and the map 𝒞k𝒞k+1\mathcal{C}_{k}\to\mathcal{C}_{k+1} is essentially surjective on (k)(\leq k)-morphismsA functor F:𝒞𝒟F\colon\mathcal{C}\to\mathcal{D} of (,n)(\infty,n)-categories is essentially surjective on (k)(\leq k)-morphisms if it is essentially surjective on objects and, for every 0j<k0\leq j<k and every pair of jj-morphisms ff and gg with the same source and target, the functor Ff,g:hom𝒞(f,g)hom𝒟(Ff,Fg)F_{f,g}\colon\hom_{\mathcal{C}}(f,g)\to\hom_{\mathcal{D}}(Ff,Fg) of (,nj1)(\infty,n-j-1)-categories is essentially surjective.. The flagging is univalent if 𝒞kιk𝒞k+1\mathcal{C}_{k}\to\iota_{k}\mathcal{C}_{k+1} is an equivalence for each kk, where ιk:𝐂𝐚𝐭(,k+1)𝐂𝐚𝐭(,k)\iota_{k}\colon\mathbf{Cat}_{(\infty,k+1)}\to\mathbf{Cat}_{(\infty,k)} is the right-adjoint to the inclusion 𝐂𝐚𝐭(,k)𝐂𝐚𝐭(,k+1)\mathbf{Cat}_{(\infty,k)}\hookrightarrow\mathbf{Cat}_{(\infty,k+1)}, which takes an (,k+1)(\infty,k+1)-category and forms an (,k)(\infty,k)-category by forgetting the non-invertible (k+1)(k+1)-morphisms.

The definition of dagger (,1)(\infty,1)-category used as an essential ingredient the fact that every (,1)(\infty,1)-category 𝒞\mathcal{C} has an opposite 𝒞op\mathcal{C}^{\mathrm{op}} that reverses the direction of composition. Similarly, given an (,n)(\infty,n)-category 𝒞\mathcal{C}, one can produce new (,n)(\infty,n)-categories by reversing any of the nn directions of composition. This supplies an action of (/2)n(\mathbb{Z}/2\mathbb{Z})^{n} on 𝐂𝐚𝐭(,n)\mathbf{Cat}_{(\infty,n)}, the (,1)(\infty,1)-category of (,n)(\infty,n)-categories. In fact, this action is completely canonical: one of the theorems of [BSP21], generalizing [Toë05], says that this map

(1) (/2)nAut(𝐂𝐚𝐭(,n))(\mathbb{Z}/2\mathbb{Z})^{n}\to\operatorname{Aut}(\mathbf{Cat}_{(\infty,n)})

is an isomorphism of (higher) groups. Given 1kn1\leq k\leq n, we will occasionally write (/2)k(/2)n(\mathbb{Z}/2\mathbb{Z})_{k}\subset(\mathbb{Z}/2\mathbb{Z})^{n} for the kkth coordinate /2\mathbb{Z}/2\mathbb{Z}, which acts on (,n)(\infty,n)-categories by reversing the composition of kk-morphisms; we will write that action as 𝒞𝒞kop\mathcal{C}\mapsto\mathcal{C}^{k\mathrm{op}}.

Definition 2.2.

Given a group homomorphism G(/2)nG\to(\mathbb{Z}/2\mathbb{Z})^{n}, an (,n)(\infty,n)-category 𝒞𝐂𝐚𝐭(,n)\mathcal{C}\in\mathbf{Cat}_{(\infty,n)} is GG-volutiveFrom the Latin volvere, “to roll,” and involvere, “to roll inwards.” when it is equipped with the data making it into a fixed point for the action of GG on Aut(𝐂𝐚𝐭(,n))\operatorname{Aut}(\mathbf{Cat}_{(\infty,n)}) via (1). In the special case when G(/2)nG\to(\mathbb{Z}/2\mathbb{Z})^{n} is the identity, we will say 𝒞\mathcal{C} is fully-volutive. When G=(/2)(/2)nG=(\mathbb{Z}/2\mathbb{Z})\to(\mathbb{Z}/2\mathbb{Z})^{n} selects the last involution, we will say 𝒞\mathcal{C} is top-volutive.

As in the 1-category case, volutive structures do not capture the theory of daggers: they do not include an analogue of the requirement that “dagger is the identity on objects.” To encode the latter, we use flaggings. To set up the definition, we note the following. Every (,k)(\infty,k)-category is in particular an (,k+1)(\infty,k+1)-category, and the inclusion 𝐂𝐚𝐭(,k)𝐂𝐚𝐭(,k+1)\mathbf{Cat}_{(\infty,k)}\hookrightarrow\mathbf{Cat}_{(\infty,k+1)} is stable under the ambient (/2)k+1(\mathbb{Z}/2\mathbb{Z})^{k+1}-action. Indeed, the first kk involutions (/2)k(/2)k+1(\mathbb{Z}/2\mathbb{Z})^{k}\subset(\mathbb{Z}/2\mathbb{Z})^{k+1} act on 𝐂𝐚𝐭(,k)\mathbf{Cat}_{(\infty,k)} via the canonical action, and the last involution (/2)k+1(\mathbb{Z}/2\mathbb{Z})_{k+1} has a canonical trivialization. Recall that a fixed point for the trivial action of a group GG on a category 𝒳\mathcal{X} is precisely an action of GG on some object X𝒳X\in\mathcal{X}. Thus if 𝒞\mathcal{C} is an (,k)(\infty,k)-category thought of as an (,k+1)(\infty,k+1)-category, then a fully-volutive structure in the (,k+1)(\infty,k+1)-sense is precisely a fully-volutive structure in the (,k)(\infty,k)-sense together with a coherently-compatible /2\mathbb{Z}/2\mathbb{Z}-action. In particular, by picking the trivial /2\mathbb{Z}/2\mathbb{Z}-action, any fully-volutive (,k)(\infty,k)-category can be thought of as a fully-volutive (,k+1)(\infty,k+1)-category.

Definition 2.3.

A flagged fully-dagger (,n)(\infty,n)-category is a flagged (,n)(\infty,n)-category

𝒞0𝒞1𝒞n\mathcal{C}_{0}\to\mathcal{C}_{1}\to\dots\to\mathcal{C}_{n}

such that each 𝒞k\mathcal{C}_{k} is a fully-volutive (,k)(\infty,k)-category, and the map 𝒞k𝒞k+1\mathcal{C}_{k}\to\mathcal{C}_{k+1} is a map of fully-volutive (,k+1)(\infty,k+1)-categories, where 𝒞k\mathcal{C}_{k} is given the trivial (k+1)(k+1)th anti-involution. Equivalently, 𝒞k𝒞k+1\mathcal{C}_{k}\to\mathcal{C}_{k+1} is factored through a map 𝒞k(ιk𝒞k+1)(/2)k+1\mathcal{C}_{k}\to(\iota_{k}\mathcal{C}_{k+1})^{(\mathbb{Z}/2\mathbb{Z})_{k+1}} of fully-volutive (,k)(\infty,k)-categories.

We remind the reader that, in the higher-categorical world, requesting that “this is a map of these things” is requesting for extra structure on the map. In the case at hand, this structure can be unpacked as follows. A map 𝒞k𝒞k+1\mathcal{C}_{k}\to\mathcal{C}_{k+1} is the same as a map 𝒞kιk𝒞k+1\mathcal{C}_{k}\to\iota_{k}\mathcal{C}_{k+1}. The fully-volutive structure on 𝒞k+1\mathcal{C}_{k+1} induces a fully-volutive structure on ιk𝒞k+1\iota_{k}\mathcal{C}_{k+1} in the (,k)(\infty,k)-sense together with a typically-nontrivial action of /2\mathbb{Z}/2\mathbb{Z}. The requested structure unpacks to a map of fully-volutive (,k)(\infty,k)-categories 𝒞k(ιk𝒞k+1)/2\mathcal{C}_{k}\to(\iota_{k}\mathcal{C}_{k+1})^{\mathbb{Z}/2\mathbb{Z}}. Comparing with Definitions 1.1 and 1.3, we exactly recover the “flagged dagger categories”; in particular, the “essential surjectivity” axiom is enforced by asking that 𝒞0𝒞1𝒞n\mathcal{C}_{0}\to\mathcal{C}_{1}\to\dots\to\mathcal{C}_{n} be a flagged (,n)(\infty,n)-category independent of the volutive, but we do not have any univalence axiom. We add that univalence axiom now.

Definition 2.4.

A flagged fully-dagger (,n)(\infty,n)-category is univalent if the maps 𝒞k(ιk𝒞k+1)/2\mathcal{C}_{k}\to(\iota_{k}\mathcal{C}_{k+1})^{\mathbb{Z}/2\mathbb{Z}} are fully-faithful on (k+1)(\geq k+1)-morphisms******A functor F:𝒞𝒟F\colon\mathcal{C}\to\mathcal{D} is fully-faithful on (k+1)(\geq k+1)-morphisms if, for every pair of kk-morphisms ff and gg with the same source and target, the functor Ff,g:𝒞(f,g)𝒟(F(f),F(g))F_{f,g}\colon\mathcal{C}(f,g)\to\mathcal{D}(F(f),F(g)) is an equivalence.. A fully-dagger (,n)(\infty,n)-category is a univalent flagged fully-dagger (,n)(\infty,n)-category. We will write 𝐂𝐚𝐭(,n){\dagger}\mathbf{Cat}_{(\infty,n)} for the (,1)(\infty,1)-category of fully-dagger (,n)(\infty,n)-categories.

Beware that a fully-dagger (,n)(\infty,n)-category is not the same as a flagged fully-dagger (,n)(\infty,n)-category of which the underlying flagging is univalent.

Definitions 2.3 and 2.4 refer only to the successive inclusions 𝒞k(ιk𝒞k+1)/2𝒞k+1\mathcal{C}_{k}\to(\iota_{k}\mathcal{C}_{k+1})^{\mathbb{Z}/2\mathbb{Z}}\to\mathcal{C}_{k+1}. But they imply more general conditions, and these more general conditions will be needed when studying groups GG other than (/2)n(\mathbb{Z}/2\mathbb{Z})^{n}.

Statement 2.5.

In a flagged fully-dagger (,n)(\infty,n)-category 𝒞\mathcal{C}, the map 𝒞k𝒞l\mathcal{C}_{k}\to\mathcal{C}_{l} is essentially surjective on (k)(\leq k)-morphisms for every 0kln0\leq k\leq l\leq n. This map factors through (ιk𝒞l)(/2)k+1××(/2)l(\iota_{k}\mathcal{C}_{l})^{(\mathbb{Z}/2\mathbb{Z})_{k+1}\times\dots\times(\mathbb{Z}/2\mathbb{Z})_{l}}. If 𝒞\mathcal{C} is univalent, then 𝒞k(ιk𝒞l)(/2)k+1××(/2)l\mathcal{C}_{k}\to(\iota_{k}\mathcal{C}_{l})^{(\mathbb{Z}/2\mathbb{Z})_{k+1}\times\dots\times(\mathbb{Z}/2\mathbb{Z})_{l}} is fully faithful on (l)(\geq l)-morphisms.

Definition 2.6.

Let G(/2)nG\subset(\mathbb{Z}/2\mathbb{Z})^{n} be a subgroup. For any subinterval {k+1,,l}{1,,n}\{k+1,\dots,l\}\subset\{1,\dots,n\}, define G({k+1,,l})=G(/2)nj=k+1l(/2)jG(\{k+1,\dots,l\})=G\cap_{(\mathbb{Z}/2\mathbb{Z})^{n}}\prod_{j=k+1}^{l}(\mathbb{Z}/2\mathbb{Z})_{j}. A flagged GG-dagger (,n)(\infty,n)-category is a flagged (,n)(\infty,n)-category 𝒞\mathcal{C} together with, for each kk, a G({1,,k})G(\{1,\dots,k\})-volutive structure on 𝒞k\mathcal{C}_{k} and, for each 0k<ln0\leq k<l\leq n, and a factorization of 𝒞k𝒞l\mathcal{C}_{k}\to\mathcal{C}_{l} through a map 𝒞k(ιk𝒞l)G({k+1,,l})\mathcal{C}_{k}\to(\iota_{k}\mathcal{C}_{l})^{G(\{k+1,\dots,l\})} of G({1,,k})G(\{1,\dots,k\})-volutive (,k)(\infty,k)-categories. A flagged GG-dagger (,n)(\infty,n)-category is univalent when the maps 𝒞k(ιk𝒞l)G({k+1,,l})\mathcal{C}_{k}\to(\iota_{k}\mathcal{C}_{l})^{G(\{k+1,\dots,l\})} are all fully faithful on (l)(\geq l)-morphisms, in which case the flagged GG-dagger (,n)(\infty,n)-category is a GG-dagger (,n)(\infty,n)-category.

We will write G𝐂𝐚𝐭(,n)G{\dagger}\mathbf{Cat}_{(\infty,n)} for the (,1)(\infty,1)-category of GG-dagger (,n)(\infty,n)-categories. The most interesting case for examples is when G=(/2)nG=(\mathbb{Z}/2\mathbb{Z})_{n}, in which case we will also refer to (/2)n(\mathbb{Z}/2\mathbb{Z})_{n}-dagger (,n)(\infty,n)-categories as top-dagger. More generally, the cases that arise in examples are when G(/2)nG\subset(\mathbb{Z}/2\mathbb{Z})^{n} is a product of some of the coordinate (/2)k(\mathbb{Z}/2\mathbb{Z})_{k}s. For such a GG, Definition 2.6 simplifies: since in this case the maps j=k+1lG({j})G({k+1,,l})\prod_{j={k+1}}^{l}G(\{j\})\to G(\{k+1,\dots,l\}) are all isomorphisms, one can restrict to just the successive inclusions 𝒞k𝒞k+1\mathcal{C}_{k}\to\mathcal{C}_{k+1} in the definition and invoke a GG-version of Statement 2.5. We have suggested a more general definition in anticipation of our discussion of unitary duality in Section 5.

3. Dagger nn-categories via enrichment

Let 𝒱\mathcal{V} be a symmetric monoidal (,1)(\infty,1)-category, with monoidal structure 𝒱:𝒱×𝒱𝒱\otimes_{\mathcal{V}}\colon\mathcal{V}\times\mathcal{V}\to\mathcal{V} and monoidal unit 1𝒱𝒱1_{\mathcal{V}}\in\mathcal{V}. There is a notion of 𝒱\mathcal{V}-enriched (,1)(\infty,1)-category, which we will abbreviate as 𝒱\mathcal{V}-category. A full definition is provided by [GH15]; we will recall the main ingredients. A flagged 𝒱\mathcal{V}-category 𝒞\mathcal{C} consists of a space 𝒞0\mathcal{C}_{0} of objects and, for each x,y𝒞0x,y\in\mathcal{C}_{0}, an object hom(x,y)𝒱\hom(x,y)\in\mathcal{V}, together with a coherently-associative and coherently-unital composition law hom(y,z)𝒱hom(x,y)hom(x,z)\hom(y,z)\otimes_{\mathcal{V}}\hom(x,y)\to\hom(x,z). The global sections functor Γ:=hom(1𝒱,):𝒱𝐒𝐩𝐚𝐜𝐞\Gamma:=\hom(1_{\mathcal{V}},-)\colon\mathcal{V}\to\mathbf{Space} is lax-symmetric-monoidal, and so 𝒞\mathcal{C} induces a flagged plain (,1)(\infty,1)-category Γ𝒞\Gamma\mathcal{C} with the same space 𝒞0\mathcal{C}_{0} of objects, and with spaces of morphisms given by Γhom(,)\Gamma\hom(-,-). The flagged 𝒱\mathcal{V}-category 𝒞\mathcal{C} is called univalent if Γ𝒞\Gamma\mathcal{C} is univalent. By definition, a 𝒱\mathcal{V}-category is a univalent flagged 𝒱\mathcal{V}-category. We will write 𝐂𝐚𝐭[𝒱]\mathbf{Cat}[\mathcal{V}] for the (,1)(\infty,1)-category of 𝒱\mathcal{V}-categories. The primordial example: 𝐂𝐚𝐭[𝐂𝐚𝐭(,n1)]𝐂𝐚𝐭(,n)\mathbf{Cat}[\mathbf{Cat}_{(\infty,n-1)}]\cong\mathbf{Cat}_{(\infty,n)}.

Using the symmetry on 𝒱\mathcal{V}, for each 𝒱\mathcal{V}-category 𝒞\mathcal{C} it should be possible to define an opposite 𝒱\mathcal{V}-category 𝒞op\mathcal{C}^{\mathrm{op}} with the same objects and morphisms but the opposite order of composition. This supplies an involution /2Aut(𝐂𝐚𝐭[𝒱])\mathbb{Z}/2\mathbb{Z}\to\operatorname{Aut}(\mathbf{Cat}[\mathcal{V}]). We can immediately generalize Definition 1.3:

Definition 3.1.

Let 𝒞\mathcal{C} be a 𝒱\mathcal{V}-category, with space of objects ι0𝒞\iota_{0}\mathcal{C}. A flagged dagger structure on 𝒞\mathcal{C} is a fixed-point structure on 𝒞\mathcal{C} for the /2\mathbb{Z}/2\mathbb{Z}-action on 𝐂𝐚𝐭[𝒱]\mathbf{Cat}[\mathcal{V}] together with a map of spaces 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} such that the induced map 𝒞0(ι0𝒞)/2ι0𝒞\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}}\to\iota_{0}\mathcal{C} is essentially surjective. A flagged dagger structure is univalent when 𝒞0(ι0𝒞)/2\mathcal{C}_{0}\to(\iota_{0}\mathcal{C})^{\mathbb{Z}/2\mathbb{Z}} is fully faithful. A dagger 𝒱\mathcal{V}-category is a 𝒱\mathcal{V}-category with a univalent flagged dagger structure.

We will write 𝐂𝐚𝐭[𝒱]{\dagger}\mathbf{Cat}[\mathcal{V}] for the (,1)(\infty,1)-category of dagger 𝒱\mathcal{V}-categories. We expect that the equivalence 𝐂𝐚𝐭[𝐂𝐚𝐭(,n1)]𝐂𝐚𝐭(,n)\mathbf{Cat}[\mathbf{Cat}_{(\infty,n-1)}]\cong\mathbf{Cat}_{(\infty,n)} generalizes to dagger categories:

Statement 3.2.

There is an equivalence of (,1)(\infty,1)-categories

𝐂𝐚𝐭[𝐂𝐚𝐭(,n1)]𝐂𝐚𝐭(,n).{\dagger}\mathbf{Cat}[{\dagger}\mathbf{Cat}_{(\infty,n-1)}]\cong{\dagger}\mathbf{Cat}_{(\infty,n)}.

In particular, by iterating Statement 3.2, one arrives at an alternative model of fully-dagger (,n)(\infty,n)-category than the one given in Definition 2.4. Mixing 𝐂𝐚𝐭[]\mathbf{Cat}[-] and 𝐂𝐚𝐭[]{\dagger}\mathbf{Cat}[-] provides alternative models of the versions with dagger structures on only some levels:

Statement 3.3.

There are equivalences of (,1)(\infty,1)-categories

𝐂𝐚𝐭[𝐂𝐚𝐭(,n1)](/2)1𝐂𝐚𝐭(,n)\displaystyle{\dagger}\mathbf{Cat}[\mathbf{Cat}_{(\infty,n-1)}]\cong(\mathbb{Z}/2\mathbb{Z})_{1}{\dagger}\mathbf{Cat}_{(\infty,n)}
𝐂𝐚𝐭[G𝐂𝐚𝐭(,n1)](×G)𝐂𝐚𝐭(,n)\displaystyle\mathbf{Cat}[G{\dagger}\mathbf{Cat}_{(\infty,n-1)}]\cong(*\times G){\dagger}\mathbf{Cat}_{(\infty,n)}

For example, iterating the second of these equivalences supplies an alternative model for top-dagger (,n)(\infty,n)-categories.

4. Dagger bicategories

In this section, we will elaborate on how Definitions 2.4 and 2.6 play out in the case of bicategories. Our goal is to outline a strictification for coherent dagger bicategories analogous to Statement 1.2 for 11-categories. Even though our definition of a fully-dagger bicategory unpacks to something complicated, it can be strictified to a “more traditionally defined” fully-dagger bicategory involving less data (but more “evil”):

Definition 4.1.

A bi-involutive bicategory is a bicategory \mathcal{B} equipped with two functors

1:1op,2:2op\displaystyle\dagger_{1}:\mathcal{B}\to\mathcal{B}^{1\mathrm{op}},\quad\dagger_{2}:\mathcal{B}\to\mathcal{B}^{2\mathrm{op}}

such that

  1. (a)

    2\dagger_{2} is the identity on objects and 11-morphisms and strictly squares to the identity;

  2. (b)

    1\dagger_{1} is the identity on objects (but not necessarily on 11-morphisms) and weakly squares to the identity in the sense that it comes equipped with a natural isomorphism ϕ:12id\phi:\dagger_{1}^{2}\to\mathrm{id}_{\mathcal{B}}, which is the identity on objects (but not necessarily on 11-morphisms).

There is a further condition, left to the reader, comparing the two ways to trivialize 13\dagger_{1}^{3}. Additionally, the two daggers strongly commute:

21op1=12op2.\dagger_{2}^{1\mathrm{op}}\circ\dagger_{1}=\dagger_{1}^{2\mathrm{op}}\circ\dagger_{2}.

This equality should be compatible with the isomorphism ϕ:12id\phi:\dagger_{1}^{2}\to\mathrm{id}_{\mathcal{B}}, i.e. ϕ\phi is unitary with respect to 2\dagger_{2}.

Unpacking Definition 4.1, it is an enriched-type definition in the sense of Section 3, so that Statement 3.2 for n=2n=2 gives a justification for the hope that bi-involutive bicategories are a model for fully dagger bicategories. In other words, similarly to how a bicategory is a category weakly enriched in categories, a bi-involutive bicategory is a \dagger-category (1\dagger_{1}) weakly enriched in \dagger-categories (2\dagger_{2}).

We decided on the name “bi-involutive bicategory” because it generalizes the notion of a bi-involutive tensor category of [HP17] to a bicategory with more than one object.

Remark 4.2.

There are at least two other structures one might call \dagger-bicategories, which are both GG-dagger categories in the sense of 2.6: they correspond to considering the two canonical /2\mathbb{Z}/2\mathbb{Z}-subgroups of /2×/2\mathbb{Z}/2\mathbb{Z}\times\mathbb{Z}/2\mathbb{Z}.††††††It could be interesting to consider the diagonal subgroup. The first one leads to a 2\dagger_{2} which is the identity on objects and 1-morphisms as above, giving a category weakly enriched in dagger categories as a special case of Statement 3.3. The other structure leads to a 1\dagger_{1} which is the identity on objects as above, a dagger category weakly enriched in categories.

Example 4.3.

A natural example of a bi-involutive bicategory is the bicategory of von Neumann algebras, Hilbert space bimodules equipped with commuting normal actions and bounded bimodule homomorphisms [Sau83, BDH88, Con94, BDH14, CHPJP22]. The daggers are given by

  • 1{\dagger}_{1}

    For a Hilbert space bimodule HNM{}_{M}H_{N} for M,NM,N von Neumann algebras, H1H^{{\dagger}_{1}} is defined to be H¯MN{}_{N}\overline{H}_{M} where H¯\overline{H} is the complex conjugate Hilbert space and the actions are given by bξ¯a=aξb¯b\cdot\overline{\xi}\cdot a=\overline{a^{*}\xi b^{*}}

  • 2{\dagger}_{2}

    For 2-morphisms (Hilbert space bimodule homomorphisms), the dagger is simply given by the adjoint as maps between Hilbert spaces.

We note that there is actually an involution on objects (which we may call 0{\dagger}_{0}) given by taking the opposite algebra (or equivalently, the complex conjugate algebra). One reason for this additional object-level involution in monoidal bicategories is due to the extra /2\mathbb{Z}/2\mathbb{Z} action given by reversing the monoidal product.

Example 4.4.

Consider the case in which \mathcal{B} has one object so that \mathcal{B} is the delooping of a monoidal category 𝒞\mathcal{C}. Having only a top-dagger 2\dagger_{2} on \mathcal{B} is the same as having a monoidal dagger structure on 𝒞\mathcal{C}. On the other hand, having only a 1\dagger_{1} on \mathcal{B} is the same as having a weak covariant involution (.)¯\overline{(.)} on 𝒞\mathcal{C} that is op-monoidal in the sense that xy¯y¯x¯.\overline{x\otimes y}\cong\overline{y}\otimes\overline{x}. Such structures have been considered in the context of dagger categories in [Egg11].

In the rest of this section, we provide some ideas for a proof of the following strictification result, which is a bicategorical analogue of the main theorem of [SS23].

Statement 4.5.

The (3,1)(3,1)-category of bi-involutive bicategories is equivalent to the (3,1)(3,1)-category of fully-dagger bicategories.

Firstly, a fully-volutive structure on a bicategory \mathcal{B} consists of a pair of equivalences ψ1:1op\psi_{1}\colon\mathcal{B}\to\mathcal{B}^{1\mathrm{op}} and ψ2:2op\psi_{2}\colon\mathcal{B}\to\mathcal{B}^{2\mathrm{op}}, together with natural isomorphisms Ω1:ψ11opψ1id\Omega_{1}\colon\psi_{1}^{1\mathrm{op}}\circ\psi_{1}\to\mathrm{id}_{\mathcal{B}}, Ω2:ψ22opψ2id\Omega_{2}\colon\psi_{2}^{2\mathrm{op}}\circ\psi_{2}\to\mathrm{id}_{\mathcal{B}}, and Ω12:ψ21opψ1ψ12opψ2\Omega_{12}\colon\psi_{2}^{1\mathrm{op}}\circ\psi_{1}\to\psi_{1}^{2\mathrm{op}}\circ\psi_{2}, and various modifications which satisfy various coherence conditions. To provide a fully-dagger structure on this volutive bicategory, we need to understand the relevant fixed point categories and specify our flaggings.

The bigroupoid (ι0)/2×/2(\iota_{0}\mathcal{B})^{\mathbb{Z}/2\mathbb{Z}\times\mathbb{Z}/2\mathbb{Z}} has objects consisting of an element of \mathcal{B} equipped with fixed point data for both ψ1\psi_{1} and ψ2\psi_{2} together with compatibility data between them, satisfying various coherence conditions. Similarly to the 11-categorical case, this in particular consists of isomorphisms hb1:ψ1(b)bh_{b}^{1}\colon\psi_{1}(b)\to b and hb2:ψ2(b)bh_{b}^{2}\colon\psi_{2}(b)\to b. The space 0\mathcal{B}_{0} in the definition of a dagger bicategory can be identified with a subspace of (ι0)/2×/2(\iota_{0}\mathcal{B})^{\mathbb{Z}/2\mathbb{Z}\times\mathbb{Z}/2\mathbb{Z}} such that the map to \mathcal{B} is essentially surjective. This picks out at least one preferred /2×/2\mathbb{Z}/2\mathbb{Z}\times\mathbb{Z}/2\mathbb{Z}-fixed point structure for every object bb\in\mathcal{B}.

The bicategory ι1/2\iota_{1}\mathcal{B}^{\mathbb{Z}/2\mathbb{Z}} has objects given by an element of \mathcal{B} equipped with fixed point data for ψ2\psi_{2}. The 1-morphisms consist of pairs of a 1-morphism f:bbf\colon b\to b^{\prime} in \mathcal{B} and 2-isomorphisms

(2) ψ2(b){\psi_{2}(b)}b{b}ψ2(b){\psi_{2}(b^{\prime})}b{b^{\prime}}hb2\scriptstyle{h_{b}^{2}}ψ2(f)\scriptstyle{\psi_{2}(f)}f\scriptstyle{f}hb2\scriptstyle{h_{b^{\prime}}^{2}}

satisfying a natural coherence condition. One can think of this 22-morphism as the data specifying how ff is a unitary 11-morphism. The bicategory 1\mathcal{B}_{1} is equivalent to a subcategory of ι1/2\iota_{1}\mathcal{B}^{\mathbb{Z}/2\mathbb{Z}}, whose objects can be identified with those of 0\mathcal{B}_{0}, since 01\mathcal{B}_{0}\to\mathcal{B}_{1} is essentially surjective. The 1-morphisms pick out at least one preferred /2\mathbb{Z}/2\mathbb{Z}-fixed point structure on every 1-morphism. The 2-morphisms are fixed by the condition that the map to ι1/2\iota_{1}\mathcal{B}^{\mathbb{Z}/2\mathbb{Z}} is fully faithful on 2-morphisms. Note how this additionally fixes the 1-morphisms of 0\mathcal{B}_{0}: they are exactly those whose fixed point structure restricts to one of the chosen fixed point structures in 1\mathcal{B}_{1}. In summary, the structure of a dagger bicategory is equivalent to a fully-volutive bicategory \mathcal{B} together with a choice of at least one /2×/2\mathbb{Z}/2\mathbb{Z}\times\mathbb{Z}/2\mathbb{Z}-fixed point on every object bb\in\mathcal{B} and at least one compatible /2\mathbb{Z}/2\mathbb{Z}-fixed point on every 1-morphism.

From this data we can construct a bi-involutive bicategory (analogous to the construction in [SS23]) as follows. Consider the bicategory \mathcal{B}^{\prime} of which the objects are the objects of 0\mathcal{B}_{0} and 1-morphisms the 1-morphisms of 1\mathcal{B}_{1}. The 2-morphisms are those of \mathcal{B}, requiring no compatibility with the fixed point data. By construction, there is a forgetful functor \mathcal{B}^{\prime}\to\mathcal{B}, which is an equivalence of bicategories. The anti-involutions ψ1\psi_{1} and ψ2\psi_{2} induce compatible anti-involutions on \mathcal{B}^{\prime}.‡‡‡‡‡‡We expect the equivalence \mathcal{B}^{\prime}\to\mathcal{B} to come equipped with a canonical datum saying it preserves the fully-volutive structures. Namely, 1\dagger_{1} is defined by the same formula as in the 11-categorical case:

f:bb\displaystyle f\colon b\to b^{\prime} hb1ψ1(f)(hb1)1.\displaystyle\longmapsto h_{b}^{1}\circ\psi_{1}(f)\circ(h_{b^{\prime}}^{1})^{-1}.

We do not spell out the fixed point structure (2) on the 11-morphism f1f^{\dagger_{1}} here. There is a natural isomorphism ϕ:12id\phi:\dagger_{1}^{2}\to\mathrm{id}_{\mathcal{B}^{\prime}} which is the identity on objects and uses the fixed point data on bb and bb^{\prime} to get a 22-isomorphism f11ff^{\dagger_{1}\dagger_{1}}\cong f for a 11-morphism f:bbf:b\to b^{\prime}. The top-dagger 2:2op\dagger_{2}\colon\mathcal{B}^{\prime}\longrightarrow\mathcal{B}^{\prime 2\mathrm{op}} is the identity on objects and 1-morphisms. It sends a 2-morphism ϑ:fg\vartheta\colon f\Rightarrow g to a version of ψ2(ϑ)\psi_{2}(\vartheta), where we identify its domain and target with gg and ff respectively using their fixed point data. The functor 2\dagger_{2} strictly squares to the identity. The two daggers commute strictly, and ϕ\phi is 2\dagger_{2}-unitary. We have thus constructed a canonical bi-involutive bicategory \mathcal{B}^{\prime} from the coherent full \dagger bicategory \mathcal{B}.

5. Dagger nn-categories with unitary duals

An (,n)(\infty,n)-category 𝒞\mathcal{C} is said to have adjoints, if for each 1kn11\leq k\leq n-1 and each kk-morphism f:xyf:x\to y (between parallel (k1)(k-1)-morphisms x,yx,y), there exist kk-morphisms fR,fL:yxf^{R},f^{L}:y\to x and (k+1)(k+1)-morphisms ηR:idxfRf\eta^{R}\colon\mathrm{id}_{x}\to f^{R}\circ f, ϵR:ffRidy\epsilon^{R}\colon f\circ f^{R}\to\mathrm{id}_{y}, ηL:idyffL\eta^{L}\colon\mathrm{id}_{y}\to f\circ f^{L}, ϵL:fLfidx\epsilon^{L}\colon f^{L}\circ f\to\mathrm{id}_{x} such that the zig-zag compositions, which after suppressing coherence (e.g. unitor and associator) information become

ffηRffRfϵRff,\displaystyle f\overset{f\eta^{R}}{\longrightarrow}ff^{R}f\overset{\epsilon^{R}f}{\longrightarrow}f, fRηRfRfRffRfRϵRfR,\displaystyle f^{R}\overset{\eta^{R}f^{R}}{\longrightarrow}f^{R}ff^{R}\overset{f^{R}\epsilon^{R}}{\longrightarrow}f^{R},
fηLfffLffϵLf,\displaystyle f\overset{\eta^{L}f}{\longrightarrow}ff^{L}f\overset{f\epsilon^{L}}{\longrightarrow}f, fLfLηLfLffLϵLfLfL,\displaystyle f^{L}\overset{f^{L}\eta^{L}}{\longrightarrow}f^{L}ff^{L}\overset{\epsilon^{L}f^{L}}{\longrightarrow}f^{L},

are equivalent to identities. Let 𝐀𝐝𝐣𝐂𝐚𝐭(,n)𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)}\subset\mathbf{Cat}_{(\infty,n)} denote the full sub-(,1)(\infty,1)-category on the (,n)(\infty,n)-categories with adjoints.

The theory of (,n)(\infty,n)-categories with adjoints has been well-studied, but there are many questions remaining. The most famous work pertains to the symmetric monoidal case, in which case dualizability is also imposed on objects. We will call a symmetric monoidal category rigid if it has adjoints and also admits duals for objects. The Cobordism Hypothesis of [BD95, Lur09b] asserts that the free rigid symmetric monoidal (,n)(\infty,n)-category generated by a single object is the (,n)(\infty,n)-category 𝐁𝐨𝐫𝐝nfr\mathbf{Bord}_{n}^{\mathrm{fr}} of framed nn-dimensional bordisms — a framing τ\tau on a smooth nn-manifold MM is a trivialization of its tangent bundle τ:TMn\tau:\mathrm{T}_{M}\cong\mathbb{R}^{n}. In other words, if 𝒞\mathcal{C} is a rigid symmetric-monoidal (,n)(\infty,n)-category, with space of objects ι0𝒞\iota_{0}\mathcal{C}, then there is a canonical equivalence

ι0𝒞homsym(𝐁𝐨𝐫𝐝nfr,𝒞).\iota_{0}\mathcal{C}\cong\hom_{\mathrm{sym\otimes}}(\mathbf{Bord}_{n}^{\mathrm{fr}},\mathcal{C}).

The group O(n)\mathrm{O}(n) obviously acts on the framings on a given nn-manifold, by rotating the trivialization, and so acts on the (,n)(\infty,n)-category 𝐁𝐨𝐫𝐝nfr\mathbf{Bord}_{n}^{\mathrm{fr}}. This in turn supplies a famous action of O(n)\mathrm{O}(n) on ι0𝒞\iota_{0}\mathcal{C} for any rigid symmetric monoidal (,n)(\infty,n)-category 𝒞\mathcal{C}.

In fact, there is a larger group that acts, as explained in [Lur09b, Remark 2.4.30]. It makes sense to talk about a “tangent bundle” of a piecewise linear (a.k.a. PL) manifold, but it is not a vector bundle: whereas the tangent bundle of a smooth nn-manifold MM is classified by a map TM:MBO(n)BDiff(n)\mathrm{T}_{M}:M\to\mathrm{B}\mathrm{O}(n)\simeq\mathrm{B}\mathrm{Diff}(n), a tangent bundle of a PL manifold is classified by a map TM:MBPL(n)\mathrm{T}_{M}:M\to\mathrm{B}\mathrm{PL}(n). In particular, it makes sense to talk about framed PL manifolds: they are PL manifolds equipped with a trivialization of TM:MBPL(n)\mathrm{T}_{M}:M\to\mathrm{B}\mathrm{PL}(n). By construction, any smoothing of a PL manifold lifts TM:MBPL(n)\mathrm{T}_{M}:M\to\mathrm{B}\mathrm{PL}(n) through BDiff(n)BO(n)\mathrm{B}\mathrm{Diff}(n)\simeq\mathrm{B}\mathrm{O}(n). We now quote a nontrivial fact of differential topology, called the Main Theorem of Smoothing Theory:

Theorem 5.1 ([KS77, Essay IV]).

Let MM be a piecewise-linear manifold. Then the space of lifts of TM:MBPL(n)\mathrm{T}_{M}:M\to\mathrm{B}\mathrm{PL}(n) through BO(n)\mathrm{B}\mathrm{O}(n) is homotopy equivalent to the space of smoothings of MM.

An immediate corollary is that a framed PL manifold has a unique (up to a contractible space) smoothing that is compatible with the framing. In particular, the framed bordism categories built from smooth or from PL manifolds are equivalent. But PL(n)\mathrm{PL}(n) acts by rotating the framings of nn-dimensional PL-manifolds, and so acts on the PL version of 𝐁𝐨𝐫𝐝nfr\mathbf{Bord}^{\mathrm{fr}}_{n}, and so acts on the space ι0𝒞\iota_{0}\mathcal{C}. This is the largest group that acts universally on the objects of rigid (,n)(\infty,n)-categories:

Statement 5.2 ([Lur09b, Remark 2.4.30]).

Assuming the Cobordism Hypothesis, the rotate-the-framing map PL(n)Autsym(𝐁𝐨𝐫𝐝nfr)\mathrm{PL}(n)\to\operatorname{Aut}_{\mathrm{sym\otimes}}(\mathbf{Bord}_{n}^{\mathrm{fr}}) is an equivalence when n4n\neq 4. The case n=4n=4 is equivalent to the 4-dimensional piecewise-linear Schoenflies conjecture (which remains open).

The proof of Statement 5.2 has circulated among experts, but is not available in print.

The story in the absence of symmetric monoidal structures is less well-studied. The Tangle Hypothesis and Cobordism Hypothesis with Singularities amount to the existence of a graphical calculus for (,n)(\infty,n)-categories with adjoints, generalizing the graphical calculi described for example in [Sel11]. The precise details of this graphical calculus have not been worked out in the literature. Roughly, the main ingredients are the following:

  1. (a)

    The diagrams in the graphical calculus are drawn on networks of submanifolds of the standard n\mathbb{R}^{n}.

  2. (b)

    Strata of codimension kk are labeled by kk-morphisms.

  3. (c)

    Strata are normally framed: if XnX\subset\mathbb{R}^{n} is a codimension-kk submanifold, then it comes with a trivialization ν:NXk\nu:\mathrm{N}_{X}\cong\mathbb{R}^{k} of its normal bundle. More generally, substrata of strata are relatively normally framed. This normal framing encodes source and target information (and so must be consistent with the labelings).

  4. (d)

    Strata are tangentially framed: if XnX\subset\mathbb{R}^{n} is a codimension-kk submanifold, then it comes with a trivialization τ:TXnk\tau:\mathrm{T}_{X}\cong\mathbb{R}^{n-k} of its tangent bundle. This tangential framing encodes the direction of composition internal to the morphism.

  5. (e)

    The various framing data are compatible. For example, if XnX\subset\mathbb{R}^{n} is a non-sub stratum, it must come equipped with a nullhomotopy of the composite isomorphism

    n=Tn=NXTXντknk=n,\mathbb{R}^{n}=\mathrm{T}_{\mathbb{R}^{n}}=\mathrm{N}_{X}\oplus\mathrm{T}_{X}\xrightarrow{\nu\oplus\tau}\mathbb{R}^{k}\oplus\mathbb{R}^{n-k}=\mathbb{R}^{n},

    where the left-hand equality simply uses that XX is a submanifold of the standard n\mathbb{R}^{n}. For substrata YXnY\subset\dots\subset X\subset\mathbb{R}^{n}, there are similar but more complicated compatibility conditions.

When n=2n=2, one finds the well known calculus of “string diagrams.” The framing-compatibility is probably the least familiar component of this calculus. Along a 1-dimensional stratum, it is a nullhomotopy of an element of O(2)\mathrm{O}(2). That element is nullhomotopic only when it lives in SO(2)\mathrm{SO}(2). This forces the normal and tangential framings to determine each other. But there is more to a nullhomotopy than just its existence: an element of SO(2)\mathrm{SO}(2) has a \mathbb{Z}-torsor of nullhomotopies. Explicitly, the framing compatibility consists of a “winding number” carried by each wire. This axiom prevents closed circles; it is what allows the string diagram calculus to apply to non-pivotal 2-categories.

To say that (,n)(\infty,n)-categories with adjoints admit some graphical calculus is to say that (,n)(\infty,n)-categories with adjoints are precisely “interpreters” for such a graphical calculus. Suppose we are given such an interpreter. Here is another interpreter: precompose your interpreter with some element of O(n)\mathrm{O}(n) acting on all input diagrams. Thus, assuming that there is indeed such a graphical calculus, one finds an action of O(n)\mathrm{O}(n) on 𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)}. We could act by any element of Diff(n)\mathrm{Diff}(n); since O(n)Diff(n)\mathrm{O}(n)\hookrightarrow\mathrm{Diff}(n) is a homotopy equivalence, this supplies “the same” action. But we were not precise about what regularity of manifolds are allowed. Statement 5.1 and its corollary about unique smoothings for framed PL manifolds says that one might as well work with a PL diagrams, and these are in any case more natural to draw. As such, we find an action of PL(n)\mathrm{PL}(n) on 𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)}. Given Statement 5.2, we expect:

Conjecture 5.3.
  1. (a)

    There is a natural map

    PL(n)Aut(𝐀𝐝𝐣𝐂𝐚𝐭(,n)).\mathrm{PL}(n)\to\operatorname{Aut}(\mathbf{AdjCat}_{(\infty,n)}).
  2. (b)

    This map is an equivalence.

For the remainder of this article, we will assume part (a) of Conjecture 5.3, and we will be motivated by our belief in part (b). We emphasize that, not only is the current literature far from a proof of part (b), it does not even supply a rigorous construction of this map in part (a) except when nn is very low:

Example 5.4.

When n=1n=1, having adjoints is vacuous, and PL(1)=/2\mathrm{PL}(1)=\mathbb{Z}/2\mathbb{Z} acts by 𝒞𝒞op\mathcal{C}\mapsto\mathcal{C}^{\mathrm{op}} as already described.

Example 5.5.

When n=2n=2, PL(2)=O(2)=SO(2)/2=B/2\mathrm{PL}(2)=\mathrm{O}(2)=\mathrm{SO}(2)\rtimes\mathbb{Z}/2\mathbb{Z}=\mathrm{B}\mathbb{Z}\rtimes\mathbb{Z}/2\mathbb{Z}. The /2\mathbb{Z}/2\mathbb{Z} subgroup acts by taking 𝒞𝐀𝐝𝐣𝐂𝐚𝐭(,2)\mathcal{C}\in\mathbf{AdjCat}_{(\infty,2)} to 𝒞2op\mathcal{C}^{2\mathrm{op}}, with the opposite composition of 22-morphisms. Note that there is an equivalence 𝒞2op𝒞1op\mathcal{C}^{2\mathrm{op}}\simeq\mathcal{C}^{1\mathrm{op}} which is the identity on objects and which acts on 1-morphisms by ffRf\mapsto f^{R}; as such, the assignment 𝒞𝒞1op\mathcal{C}\mapsto\mathcal{C}^{1\mathrm{op}} would produce an equivalent /2\mathbb{Z}/2\mathbb{Z}-action on 𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)}. The generator of B\mathrm{B}\mathbb{Z} acts on 𝐀𝐝𝐣𝐂𝐚𝐭(,2)\mathbf{AdjCat}_{(\infty,2)} by a natural automorphism of id𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathrm{id}_{\mathbf{AdjCat}_{(\infty,n)}}. Such a natural automorphism has components: its component at 𝒞𝐀𝐝𝐣𝐂𝐚𝐭(,2)\mathcal{C}\in\mathbf{AdjCat}_{(\infty,2)} is the autofunctor 𝒞𝒞\mathcal{C}\to\mathcal{C} that is the identity on objects and takes a 1-morphism ff to its double-right-dual fRRf^{RR}. To fully present an action of B/2\mathrm{B}\mathbb{Z}\rtimes\mathbb{Z}/2\mathbb{Z} is to present a map out of the space B(B/2)\mathrm{B}(\mathrm{B}\mathbb{Z}\rtimes\mathbb{Z}/2\mathbb{Z}), which is the total space of a nontrivial P\mathbb{C}P^{\infty}-bundle over P\mathbb{R}P^{\infty}. The fact that O(2)O(1)×SO(2)O(2)\ncong O(1)\times SO(2) is expressed by the natural isomorphism ((.)RR)2op((.)2op)RR1((.)^{RR})^{2\mathrm{op}}\cong((.)^{2\mathrm{op}})^{RR-1}, using opposites take left to right adjoints. The higher cells in (a cell model for) this space map to compatibility data between the actions of lower cells.

In analogy with Definition 2.2, we declare:

Definition 5.6.

A (,n)(\infty,n)-category with adjoints 𝒞𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathcal{C}\in\mathbf{AdjCat}_{(\infty,n)} is PL(n)\mathrm{PL}(n)-volutive if it is (equipped with the structure of) a fixed point for the PL(n)\mathrm{PL}(n)-action on 𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)}.

An (,n1)(\infty,n-1)-category, thought of as an (,n)(\infty,n)-category, never has all adjoints unless it is a groupoid: there is no organic inclusion 𝐀𝐝𝐣𝐂𝐚𝐭(,n1)𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n-1)}\to\mathbf{AdjCat}_{(\infty,n)}. The other direction, however, does work: if 𝒞\mathcal{C} is a (,n)(\infty,n)-category with adjoints, then its underlying (,n1)(\infty,n-1)-category ιn1𝒞\iota_{n-1}\mathcal{C} has adjoints. We will say that a flagged (,n)(\infty,n)-category 𝒞0𝒞1𝒞n\mathcal{C}_{0}\to\mathcal{C}_{1}\to\dots\to\mathcal{C}_{n} has adjoints if every 𝒞k\mathcal{C}_{k} does.

The functor

ιn1:𝐀𝐝𝐣𝐂𝐚𝐭(,n)𝐀𝐝𝐣𝐂𝐚𝐭(,n1)\iota_{n-1}:\mathbf{AdjCat}_{(\infty,n)}\to\mathbf{AdjCat}_{(\infty,n-1)}

cannot be PL(n)\mathrm{PL}(n)-equivariant simply because PL(n)\mathrm{PL}(n) does not act on the codomain. But it is equivariant for PL(n1)PL(n)\mathrm{PL}(n-1)\subset\mathrm{PL}(n). Even better: ιn1\iota_{n-1} is (PL(n1)×PL(1))(\mathrm{PL}(n-1)\times\mathrm{PL}(1))-equivariant, where on the domain the action is via the inclusion into PL(n)\mathrm{PL}(n), and on the codomain the PL(1)\mathrm{PL}(1)-factor acts trivially. The upshot: if 𝒞\mathcal{C} is PL(n)\mathrm{PL}(n)-volutive, then ιn1𝒞\iota_{n-1}\mathcal{C} is PL(n1)\mathrm{PL}(n-1)-volutive and also carries a /2\mathbb{Z}/2\mathbb{Z}-action. More generally, the functor ιk:𝐀𝐝𝐣𝐂𝐚𝐭(,n)𝐀𝐝𝐣𝐂𝐚𝐭(,k)\iota_{k}\colon\mathbf{AdjCat}_{(\infty,n)}\to\mathbf{AdjCat}_{(\infty,k)} is PL(k)×PL(nk)\mathrm{PL}(k)\times\mathrm{PL}(n-k) equivariant, where PL(nk)\mathrm{PL}(n-k) acts on the codomain trivially. We are led naturally to the following version of Definition 2.3 for categories with adjoints:

Definition 5.7.

A flagged PL\mathrm{PL}-dagger (,n)(\infty,n)-category, also called a flagged (fully-)dagger (,n)(\infty,n)-category with unitary duality, is a flagged (,n)(\infty,n)-category with adjoints

𝒞0𝒞1𝒞n\mathcal{C}_{0}\to\mathcal{C}_{1}\to\dots\to\mathcal{C}_{n}

such that each (,k)(\infty,k)-category 𝒞k\mathcal{C}_{k} is PL(k)\mathrm{PL}(k)-volutive, and each functor 𝒞k𝒞k+j\mathcal{C}_{k}\to\mathcal{C}_{k+j} is (PL(k)×PL(j))(\mathrm{PL}(k)\times\mathrm{PL}(j))-volutive, with trivial***More precisely, the PL(k)×PL(j)\mathrm{PL}(k)\times\mathrm{PL}(j)-volution on 𝒞k\mathcal{C}_{k} is induced by pulling back its PL(k)\mathrm{PL}(k)-volution along the projection PL(k)×PL(j)PL(k)\mathrm{PL}(k)\times\mathrm{PL}(j)\to\mathrm{PL}(k), and on 𝒞k+j\mathcal{C}_{k+j} it is induced by pulling back its PL(k+j)\mathrm{PL}(k+j)-volution along the inclusion PL(k)×PL(j)PL(k+j)\mathrm{PL}(k)\times\mathrm{PL}(j)\to\mathrm{PL}(k+j). PL(j)\mathrm{PL}(j)-volution on 𝒞k\mathcal{C}_{k}.

Given a flagged PL-dagger (,n)(\infty,n)-category

𝒞0𝒞1𝒞n\mathcal{C}_{0}\to\mathcal{C}_{1}\to\dots\to\mathcal{C}_{n}

we obtain an underlying flagged fully-dagger (,n)(\infty,n)-category. We could ask this fully-dagger to be univalent in the sense of Definition 2.4, which implements the idea that an (i+1)(i+1)-morphism in 𝒞i\mathcal{C}_{i} is exactly a unitary morphism 𝒞i+1\mathcal{C}_{i+1}. However, we claim this is not the right univalence condition in general because we want an (i+2)(i+2)-morphism in 𝒞i\mathcal{C}_{i} to be a PL(2)\mathrm{PL}(2)-unitary morphism in 𝒞i+2\mathcal{C}_{i+2}, and PL(2)\mathrm{PL}(2) is not isomorphic to PL(1)×PL(1)\mathrm{PL}(1)\times\mathrm{PL}(1). Instead, consider the diagram consisting of the (,nl)(\infty,n-l)-categories (ιnl𝒞nj)PL(k1)×PL(km)(\iota_{n-l}\mathcal{C}_{n-j})^{\mathrm{PL}(k_{1})\times\dots\mathrm{PL}(k_{m})}, where (k1,,km)(k_{1},\dots,k_{m}) is a partition of jj for jlj\leq l. There are two types of maps in the diagram: those forgetting fixed point data corresponding to (k1,,ki+ki+1,,km)(k1,,ki,ki+1,,km)(k_{1},\dots,k_{i}+k_{i+1},\dots,k_{m})\rightsquigarrow(k_{1},\dots,k_{i},k_{i+1},\dots,k_{m}) and transitions between the flaggings corresponding to (k1,,km1)(k1,,km1,km)(k_{1},\dots,k_{m-1})\rightsquigarrow(k_{1},\dots,k_{m-1},k_{m}). Note that if we were to allow the empty partition corresponding to ιnl𝒞nl=𝒞nl\iota_{n-l}\mathcal{C}_{n-l}=\mathcal{C}_{n-l} we would get a cube. Instead, set Pnl(𝒞)P_{n-l}(\mathcal{C}) to be the pullback of the diagram built from the nonempty partitions, so that there is a canonical map 𝒞nlPnl(𝒞)\mathcal{C}_{n-l}\to P_{n-l}(\mathcal{C}). For example, when n=3n=3 the diagram for l=3l=3 is:

𝒞0{\mathcal{C}_{0}}P0(𝒞){P_{0}(\mathcal{C})}ι0𝒞2PL(2){{\iota_{0}\mathcal{C}_{2}^{\mathrm{PL}(2)}}}ι0𝒞3PL(3){{\iota_{0}\mathcal{C}_{3}^{\mathrm{PL}(3)}}}ι0𝒞3PL(2)×PL(1){{\iota_{0}\mathcal{C}_{3}^{\mathrm{PL}(2)\times\mathrm{PL}(1)}}}ι0𝒞1PL(1){{\iota_{0}\mathcal{C}_{1}^{\mathrm{PL}(1)}}}ι0𝒞2PL(1)×PL(1){{\iota_{0}\mathcal{C}_{2}^{\mathrm{PL}(1)\times\mathrm{PL}(1)}}}ι0𝒞3PL(1)×PL(2){{\iota_{0}\mathcal{C}_{3}^{\mathrm{PL}(1)\times\mathrm{PL}(2)}}}ι0𝒞3PL(1)×PL(1)×PL(1){{\iota_{0}\mathcal{C}_{3}^{\mathrm{PL}(1)\times\mathrm{PL}(1)\times\mathrm{PL}(1)}}}

By definition, a morphism in Pnl(𝒞)P_{n-l}(\mathcal{C}) is a morphism which is PL(k)\mathrm{PL}(k)-unitary for every k>nlk>n-l. This is precisely what we want for the (>nl)(>n-l)-morphisms in 𝒞nl\mathcal{C}_{n-l}. Thus we arrive at the following univalence axiom:

Definition 5.8.

A flagged PL\mathrm{PL}-dagger (,n)(\infty,n)-category is univalent if for every ll, the map 𝒞nlPnl(𝒞)\mathcal{C}_{n-l}\to P_{n-l}(\mathcal{C}) into the pullback is fully faithful on >(nl)>(n-l)-morphisms. A PL\mathrm{PL}-dagger (,n)(\infty,n)-category, also called a dagger (,n)(\infty,n)-category with unitary duality, is a univalent flagged one.

Remark 5.9.

For good families of groups G(n)G(n) related to PL(n)\mathrm{PL}(n), we expect that there is a definition of GG-dagger categories with adjoints generalizing Definition 2.6. Examples should include, in particular, O(n)\mathrm{O}(n) and SO(n)\mathrm{SO}(n). We will not try to work out the precise conditions on G(n)G(n) or all details of the definition here.

Let us turn now to justifying the name “with unitary duality.” We will do so by unpacking the notion in the case of bicategories in Examples 5.10 and 5.11. Before that, note that the forgetful functor 𝐀𝐝𝐣𝐂𝐚𝐭(,n)𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)}\to\mathbf{Cat}_{(\infty,n)} is (/2)n(\mathbb{Z}/2\mathbb{Z})^{n} equivariant, where (/2)n(\mathbb{Z}/2\mathbb{Z})^{n} acts through the map (/2)n=PL(1)nPL(n)(\mathbb{Z}/2\mathbb{Z})^{n}=\mathrm{PL}(1)^{n}\to\mathrm{PL}(n). Thus to every dagger (,n)(\infty,n)-category with unitary duality we can assign an underlying (fully-)dagger (,n)(\infty,n)-category in which the unitary duality is forgotten. So the question is to understand what this extra “unitary duality” data looks like.

Example 5.10.

We specialize from (,n)(\infty,n)-categories to bicategories and look at the SO(2)\mathrm{SO}(2) subgroup of PL(2)=O(2)\mathrm{PL}(2)=\mathrm{O}(2). What is the data of an SO(2)\mathrm{SO}(2)-volution on a bicategory \mathcal{B}? Fixed-point data for an SO(2)\mathrm{SO}(2)(=B=\mathrm{B}\mathbb{Z})-action consists of data assigned to each cell in BSO(2)=P\mathrm{B}\mathrm{SO}(2)=\mathbb{C}P^{\infty}; there is one cell in each even dimension. The 0-cell selects the bicategory \mathcal{B}. The 22-cell selects a trivialization θ\theta of ()RR(-)^{RR}: such a trivialization unpacks to a family of 1-isomorphisms θb:bb\theta_{b}\colon b\to b for all bb\in\mathcal{B} and 2-isomorphisms fRRθb1θb2ff^{RR}\circ\theta_{b_{1}}\to\theta_{b_{2}}\circ f for 11-morphisms f:b1b2f:b_{1}\to b_{2} satisfying various coherence conditions. The 44-cell selects a quadratic equation that θ\theta must solve; the reader is encouraged to work out this equation as an exercise. In the special case of bicategories, this is all the necessary data: the higher cells in P\mathbb{C}P^{\infty} admit unique assignments, because the space of bicategories with adjoints is a homotopy 3-type.

The group SO(1)\mathrm{SO}(1) is trivial, and so to enhance an SO(2)\mathrm{SO}(2)-volutive bicategory \mathcal{B} to an SO(2)\mathrm{SO}(2)-dagger bicategory, one needs only to supply the data of an SO(2)\mathrm{SO}(2)-volutive  essentially surjective functor 0\mathcal{B}_{0}\to\mathcal{B} such that 0(ι0)SO(2)\mathcal{B}_{0}\to(\iota_{0}\mathcal{B})^{\mathrm{SO}(2)} is 1-fully faithful. The objects (ι0)SO(2)(\iota_{0}\mathcal{B})^{\mathrm{SO}(2)} are given by pairs consisting of of an object bb\in\mathcal{B} and a 2-isomorphism ωb:θbidb\omega_{b}\colon\theta_{b}\to\mathrm{id}_{b}. Similar to Section 4, form a new bicategory \mathcal{B}^{\prime} whose objects are those of 0\mathcal{B}_{0} and morphisms are those in \mathcal{B}. This bicategory \mathcal{B}^{\prime} comes with a trivialization of the double dual functor ()RR(-)^{RR} which is the identity on objects (and which solves a quadratic equation). In other words, \mathcal{B}^{\prime} is a pivotal bicategory as defined for example in [FSY23, Definition 2.1], also called an even-handed bicategory [Bar09]. Like traditionally-defined dagger 11-categories, pivotal bicategories are “evil” in the sense that pivotal structures do not transport across bicategorical equivalences. Remark 5.9 suggests a coherent version of “pivotal bicategory”: they are the SO(2)\mathrm{SO}(2)-dagger bicategories.

To finish the discussion of the name “unitary duality,” we now restore the reflection.

Example 5.11.

As mentioned in Example 5.5, to discuss actions by, and fixed points for, O(2)=B/2\mathrm{O}(2)=\mathrm{B}\mathbb{Z}\rtimes\mathbb{Z}/2\mathbb{Z}, one should assign data to the cells in a cell model for BO(2)\mathrm{B}\mathrm{O}(2), which is a P\mathbb{C}P^{\infty}-bundle over P\mathbb{R}P^{\infty}. In particular, BO(2)\mathrm{B}\mathrm{O}(2) has a cell model with one cell of dimension 2s+r2s+r for each pair s,rs,r\in\mathbb{N}. The cells indexed (s,0)(s,0) supply the restriction of the data along SO(2)O(2)\mathrm{SO}(2)\to\mathrm{O}(2), and the cells indexed (0,r)(0,r) supply the restriction of the data along (/2)2O(2)(\mathbb{Z}/2\mathbb{Z})_{2}\subset\mathrm{O}(2). We see that an O(2)\mathrm{O}(2)-volution consists of a (/2)2(\mathbb{Z}/2\mathbb{Z})_{2}-volution ψ2:2op\psi_{2}:\mathcal{B}\to\mathcal{B}^{2\mathrm{op}}, a trivialization fRRθb2fθb11f^{RR}\to\theta_{b_{2}}\circ f\circ\theta_{b_{1}}^{-1} as in Example 5.10, together with a natural modification equating the two ways to identify ψ2(fRR)ψ2(f)LL\psi_{2}(f^{RR})\cong\psi_{2}(f)^{LL} with ψ2(f)\psi_{2}(f), satisfying some conditions. This in particular includes a (/2)2(\mathbb{Z}/2\mathbb{Z})_{2}-fixed point datum ψ2(θb))θψ2(b1)1\psi_{2}(\theta_{b}))\cong\theta_{\psi_{2}(b_{1})}^{-1}. We see that an O(2)\mathrm{O}(2)-dagger structure consists of

  1. (a)

    an O(2)\mathrm{O}(2)-equivariant essentially surjective functor 0\mathcal{B}_{0}\to\mathcal{B} from a 22-groupoid such that 0(ι0)O(2)\mathcal{B}_{0}\to(\iota_{0}\mathcal{B})^{\mathrm{O}(2)} is fully faithful. The O(2)\mathrm{O}(2)-fixed points combine the trivializations ω\omega of Example 5.10 from SO(2)\mathrm{SO}(2) with the O(1)\mathrm{O}(1)-fixed point data hb2h_{b}^{2} such that ω\omega is compatible with ψ2(θb))θψ2(b1)1\psi_{2}(\theta_{b}))\cong\theta_{\psi_{2}(b_{1})}^{-1} and the 22-isomorphism fRRθb2fθb11f^{RR}\to\theta_{b_{2}}\circ f\circ\theta_{b_{1}}^{-1} preserves (/2)2(\mathbb{Z}/2\mathbb{Z})_{2}-fixed point data.

  2. (b)

    As in Section 4, the (2,1)(2,1)-category 1\mathcal{B}_{1} and the functors 1\mathcal{B}_{1}\to\mathcal{B} and 01\mathcal{B}_{0}\to\mathcal{B}_{1} are fixed after specifying (/2)2(\mathbb{Z}/2\mathbb{Z})_{2}-fixed point data on 11-morphisms of \mathcal{B}.

  3. (c)

    The functors 01\mathcal{B}_{0}\to\mathcal{B}_{1} and 1\mathcal{B}_{1}\to\mathcal{B} are still required to be (/2)2(\mathbb{Z}/2\mathbb{Z})^{2}-equivariant. As explained in Section 4, the (/2)2(\mathbb{Z}/2\mathbb{Z})_{2} simply specifies the agreement of fixed point data on 22-morphisms. For the (/2)1(\mathbb{Z}/2\mathbb{Z})_{1}-equivariance, first note that the underlying (/2)1(\mathbb{Z}/2\mathbb{Z})_{1}-volution of the O(2)\mathrm{O}(2)-volution can be described by ψ1=(.)Rψ2\psi_{1}=(.)^{R}\circ\psi_{2}, where we made an arbitrary choice of the right adjoint to trivialize the 180180^{\circ} rotation in SO(2)\mathrm{SO}(2). Using the pivotal structure and the fact that ψ2(fR)ψ2(f)L\psi_{2}(f^{R})\cong\psi_{2}(f)^{L}, we obtain data specifying that ψ2\psi_{2} and (.)R(.)^{R} commute. Note that the (/2)1(\mathbb{Z}/2\mathbb{Z})_{1}-fixed point data induced by the (/2)2(\mathbb{Z}/2\mathbb{Z})_{2}-fixed point data hb2h^{2}_{b} is (hb2)R(h^{2}_{b})^{R}. The (/2)1(\mathbb{Z}/2\mathbb{Z})_{1}-equivariance data of 1(ι1)(/2)2\mathcal{B}_{1}\to(\iota_{1}\mathcal{B})^{(\mathbb{Z}/2\mathbb{Z})_{2}} will ensure that if hfh_{f} is a (/2)2(\mathbb{Z}/2\mathbb{Z})_{2}-fixed point data on a 11-morphism, then there is a canonical fixed point data hfRh_{f^{R}} for fRf^{R}, which makes the right adjoint into a top dagger functor.

When the bicategory \mathcal{B} is the one-object delooping of a rigid monoidal 1-category 𝒞\mathcal{C}, and 0\mathcal{B}_{0} is declared to consist exactly of this object, this should recover the notion of a dagger category with a unitary dual functor [Sel11, Definition on page 53 part (2)], see also [Pen20].

As in Definition 1.6, one can also define coflagged PL\mathrm{PL}-dagger (,n)(\infty,n)-categories by keeping the univalence axiom Definition 5.7 but dropping the essential surjectivity (i.e. not requiring that 𝒞0𝒞n\mathcal{C}_{0}\to\dots\to\mathcal{C}_{n} be a flagging). Statement 1.7 generalizes: every coflagged PL\mathrm{PL}-dagger category can be completed to a PL\mathrm{PL}-dagger category by replacing each 𝒞k\mathcal{C}_{k} with the full image of 𝒞k1\mathcal{C}_{k-1}; this is the right adjoint to the forgetful functor from PL\mathrm{PL}-dagger to coflagged PL\mathrm{PL}-dagger categories. The further forgetful functor from coflagged PL\mathrm{PL}-dagger to PL\mathrm{PL}-anti-involutive categories that remembers only the top level also has a right adjoint which assigns to a PL\mathrm{PL}-anti-involutive (,n)(\infty,n)-category 𝒞\mathcal{C} the diagram

(3) (ι0𝒞)PL(n)(ι1𝒞)PL(n1)𝒞.(\iota_{0}\mathcal{C})^{\mathrm{PL}(n)}\to(\iota_{1}\mathcal{C})^{\mathrm{PL}(n-1)}\to\dots\to\mathcal{C}.

6. Bordism categories and reflection-positive topological quantum field theories

For some of us, our interest in higher dagger categories stems from the role that we expect them to play in the study of (topological) quantum field theories. For any space XBO(n)X\to\mathrm{B}\mathrm{O}(n) over BO(n)\mathrm{B}\mathrm{O}(n) there is a rigid symmetric monoidal (,n)(\infty,n)-category 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} of bordisms MM with a lift of their tangent bundle TM:MBO(n)\mathrm{T}_{M}\colon M\to\mathrm{B}\mathrm{O}(n) through XX. (The construction of 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} is outlined in [Lur09b] and fully implemented by one of us in [CS19].) For example, a framing is a trivialization of TM\mathrm{T}_{M}, i.e. a lift through BO(n)\ast\to\mathrm{B}\mathrm{O}(n), and 𝐁𝐨𝐫𝐝n=𝐁𝐨𝐫𝐝nfr\mathbf{Bord}_{n}^{\ast}=\mathbf{Bord}_{n}^{\mathrm{fr}}. Let 𝒞\mathcal{C} be a symmetric monoidal (,n)(\infty,n)-category. An XX-structured nn-dimensional fully extended topological quantum field theory with values in 𝒞\mathcal{C} is a symmetric monoidal functor 𝒵:𝐁𝐨𝐫𝐝nX𝒞\mathcal{Z}\colon\mathbf{Bord}_{n}^{X}\to\mathcal{C}. Since the bordism category is rigid, every topological quantum field theory will factor through the maximal rigid sub-(,n)(\infty,n)-category of 𝒞\mathcal{C}. Hence we will from now on assume without loss of generality that 𝒞\mathcal{C} is rigid. Recall that the Cobordism Hypothesis allows us to identify fully extended framed topological field theories with ι0𝒞\iota_{0}\mathcal{C}, which hence carries a PL(n)\mathrm{PL}(n)-action. This was the starting point for the discussion in the previous section. The Cobordism Hypothesis also provides a description of the space of XX-structured fully extended topological quantum field theories as the space of XX-fixed points (ι0𝒞)X(\iota_{0}\mathcal{C})^{X}.

As an example, let us focus on unoriented smooth nn-dimensional topological quantum field theories valued in 𝒞\mathcal{C}. The space of such theories is (ι0𝒞)O(n)(\iota_{0}\mathcal{C})^{\mathrm{O}(n)}. The 11-morphisms in 𝒞\mathcal{C} are the objects of a rigid symmetric monoidal (,n1)(\infty,n-1)-category ιn1𝒞\iota_{n-1}\mathcal{C}^{\to} [JFS17, Section 7], and thus carry an action by O(n1)\mathrm{O}(n-1); the maps that assign to a 1-morphism its source and target and that compose 1-morphisms are O(n1)\mathrm{O}(n-1)-equivariant, and compile into an action of O(n1)\mathrm{O}(n-1) on the whole (,1)(\infty,1)-category ι1𝒞\iota_{1}\mathcal{C}. This action is meaningful from the perspective of topological quantum field theory: there is an O(n1)\mathrm{O}(n-1)-action on the space of 1-morphisms between the objects underlying two different unoriented topological field theories, and the Stratified Cobordism Hypothesis says that fixed points for this O(n1)\mathrm{O}(n-1)-action classify unoriented codimension-11 defects between the two field theories. Similarly, 22-morphisms carry an induced O(n2)\mathrm{O}(n-2)-action whose fixed points classified unoriented codimension-22 defects, and so on. In summary, unoriented smooth defects assemble into the following diagram:

(4) (ι0𝒞)O(n)(ι1𝒞)O(n1)𝒞.(\iota_{0}\mathcal{C})^{\mathrm{O}(n)}\to(\iota_{1}\mathcal{C})^{\mathrm{O}(n-1)}\to\dots\to\mathcal{C}.

There is nothing special in (4) about unoriented smooth theories and the groups O(k)\mathrm{O}(k): any good sequence of groups G(k)G(k) would work (compare Remark 5.9). For example, replacing the O(k)\mathrm{O}(k)’s in (4) with SO(k)\mathrm{SO}(k)’s would organize the defects between oriented smooth field theories as analyzed for example in [DKR11, CMS20]; replacing the O(k)\mathrm{O}(k)’s with PL(k)\mathrm{PL}(k)’s would organize the defects between unoriented piecewise linear field theories.

The diagram (4) is suspiciously close to (3) but they are a priori different: the action of O(k)\mathrm{O}(k) on ιnk𝒞\iota_{n-k}\mathcal{C} in (4) comes from the Cobordism Hypothesis and uses the symmetric monoidal structure on 𝒞\mathcal{C}, whereas in (3) we envisioned selecting a PL(n)\mathrm{PL}(n)-volution on 𝒞\mathcal{C}, i.e. fixed-point data for the action of PL(n)\mathrm{PL}(n) on the graphical calculus for 𝒞\mathcal{C}. We expect the relation to be the following. Any symmetric monoidal (,n)(\infty,n)-category 𝒞\mathcal{C} determines a symmetric monoidal (,n+1)(\infty,n+1)-category B𝒞\mathrm{B}\mathcal{C} with one object \bullet and EndB𝒞()=𝒞\operatorname{End}_{\mathrm{B}\mathcal{C}}(\bullet)=\mathcal{C}; iterating this supplies (,n+m)(\infty,n+m)-categories Bm𝒞\mathrm{B}^{m}\mathcal{C} for every mm\in\mathbb{N}. If 𝒞\mathcal{C} is rigid, then Bm𝒞\mathrm{B}^{m}\mathcal{C} will have all adjoints. The graphical calculi for 𝒞\mathcal{C} and for Bm𝒞\mathrm{B}^{m}\mathcal{C} are compatible via the embedding of n\mathbb{R}^{n} into n+m\mathbb{R}^{n+m} as the last nn coordinates. Hence we can think of the graphical calculus for a rigid symmetric monoidal (,n)(\infty,n)-category as taking place in \mathbb{R}^{\infty}. The space of embeddings (of any finite-dimensional object) into \mathbb{R}^{\infty} is contractible. This contractibility selects a canonical trivialization of the PL(n)\mathrm{PL}(n)-action predicted in Conjecture 5.3 for any rigid symmetric monoidal (,n)(\infty,n)-category. In other words, if we let 𝐒𝐲𝐦𝐑𝐢𝐠𝐢𝐝𝐂𝐚𝐭(,n)\mathbf{SymRigidCat}_{(\infty,n)} denote the (,1)(\infty,1)-category of rigid symmetric monoidal (,n)(\infty,n)-categories:

Statement 6.1.

The forgetful functor

𝐒𝐲𝐦𝐑𝐢𝐠𝐢𝐝𝐂𝐚𝐭(,n)𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{SymRigidCat}_{(\infty,n)}\to\mathbf{AdjCat}_{(\infty,n)}

factors through the PL(n)\mathrm{PL}(n)-fixed points 𝐀𝐝𝐣𝐂𝐚𝐭(,n)PL(n)𝐀𝐝𝐣𝐂𝐚𝐭(,n)\mathbf{AdjCat}_{(\infty,n)}^{\mathrm{PL}(n)}\to\mathbf{AdjCat}_{(\infty,n)}.

In particular, a rigid symmetric monoidal structure on a (,n)(\infty,n)-category selects a canonical PL(n)\mathrm{PL}(n)-volutive structure on its underlying (,n)(\infty,n)-category with adjoints. Moreover, any symmetric monoidal functor between rigid symmetric monoidal (,n)(\infty,n)-categories will automatically intertwine these canonical PL(n)\mathrm{PL}(n)-volutive structures.

Given a rigid symmetric monoidal (,n)(\infty,n)-category 𝒞\mathcal{C}, we expect that the induced PL(n)\mathrm{PL}(n)-action on ι0𝒞\iota_{0}\mathcal{C} agrees with the one coming from the Cobordism Hypothesis.

Other symmetric monoidal PL(n)\mathrm{PL}(n)-volutive structures on 𝒞\mathcal{C} are given by twisting the canonical one by a symmetric monoidal PL(n)\mathrm{PL}(n)-action on 𝒞\mathcal{C}: symmetric monoidal PL(n)\mathrm{PL}(n)-volutive structures form a trivialized torsor over PL(n)\mathrm{PL}(n)-actions.

There is a straightforward way to define symmetric monoidal PL(n)\mathrm{PL}(n)-dagger categories by simply requiring the volution, the flagging by 𝒞i\mathcal{C}_{i}’s, and the trivialization data, to all be symmetric monoidal. Interestingly, if 𝒞\mathcal{C} is in addition rigid the sequence of deloopings 𝒞,B𝒞,B2𝒞,\mathcal{C},\mathrm{B}\mathcal{C},\mathrm{B}^{2}\mathcal{C},\dots allows more. Suppose that

(5) 𝒞0𝒞1𝒞n=𝒞\mathcal{C}_{0}\to\mathcal{C}_{1}\to\dots\to\mathcal{C}_{n}=\mathcal{C}

is a symmetric monoidal flagged (,n)(\infty,n)-category. Then the deloopings assemble into a flagged (,n+1)(\infty,n+1)-category by selecting the unit object at the bottom:

(6) {}B𝒞0B𝒞1B𝒞n=B𝒞.\{\bullet\}\to\mathrm{B}\mathcal{C}_{0}\to\mathrm{B}\mathcal{C}_{1}\to\dots\mathrm{B}\mathcal{C}_{n}=\mathrm{B}\mathcal{C}.

If 𝒞k\mathcal{C}_{k} is rigid as a symmetric monoidal (,k)(\infty,k)-category, then B𝒞k\mathrm{B}\mathcal{C}_{k} is also rigid, now as a symmetric monoidal (,k+1)(\infty,k+1)-category.

Given such a structure, just like it is natural to ask for a symmetric monoidal flagged PL(n)\mathrm{PL}(n)-dagger structure on a chosen flagging (5), it is natural to ask to give B𝒞\mathrm{B}\mathcal{C} a flagged PL(n+1)\mathrm{PL}(n+1)-dagger structure with chosen flagging  (6). Iterating, it is natural to ask to give Bm𝒞\mathrm{B}^{m}\mathcal{C} a compatible symmetric monoidal PL(n+m)\mathrm{PL}(n+m)-dagger structure. We call the structure just sketched a PL\mathrm{PL}-dagger tower with underlying (,n)(\infty,n)-category 𝒞\mathcal{C}.

After untwisting by the canonical volutive structures, a symmetric monoidal PL(n+m)\mathrm{PL}(n+m)-dagger structure on Bm𝒞\mathrm{B}^{m}\mathcal{C} unpacks to a symmetric monoidal action of PL(k+m)\mathrm{PL}(k+m) on 𝒞k\mathcal{C}_{k} for all knk\leq n, and compatible (PL(k+m)×PL(j))(\mathrm{PL}(k+m)\times\mathrm{PL}(j))-equivariant maps 𝒞k𝒞k+j\mathcal{C}_{k}\to\mathcal{C}_{k+j} for all j+knj+k\leq n. Univalence is just about the PL(j)\mathrm{PL}(j)-fixed points: it is independent of mm. A more careful treatment and definition is beyond the scope of this short article.

Example 6.2.

To illustrate the difference between the two definitions above, we look at dagger 1-categories. A (strict) symmetric monoidal dagger 1-category is a symmetric monoidal category equipped with a symmetric monoidal anti-involution which is the identity on objects. From Example 5.11 we learn that a PL\mathrm{PL}-dagger tower with underlying 1-category is in addition equipped with a unitary dual functor. There are no additional structures corresponding to higher deloopings, since they would correspond to higher morphisms.

We will now construct a dagger structure on certain bordism categories 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X}. Let us recall some more details about these (,n)(\infty,n)-categories. They depend on a choice of tangential structure XBPL(n)X\to\mathrm{B}\mathrm{PL}(n) — for example, by smoothing theory (Theorem 5.1), the smooth unoriented bordism category 𝐁𝐨𝐫𝐝nO(n)\mathbf{Bord}_{n}^{\mathrm{O}(n)} corresponds to the tangential structure BO(n)BPL(n)\mathrm{B}\mathrm{O}(n)\to\mathrm{B}\mathrm{PL}(n). Given knk\leq n, set X(k)PL(k)X(k)\to\mathrm{PL}(k) to be the pullback of XPL(n)X\to\mathrm{PL}(n) along the standard inclusion BPL(k)BPL(n)\mathrm{B}\mathrm{PL}(k)\to\mathrm{B}\mathrm{PL}(n). A kk-morphism in 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} is by definition a kk-dimensional cobordism MkM^{k} equipped with a lift of its tangent bundle TM:MBPL(k)\mathrm{T}_{M}\colon M\to\mathrm{B}\mathrm{PL}(k) through X(k)X(k); we will refer to such a lift simply as an XX-structure.

Just as the tangential structure X(k)X(k) on kk-morphisms is pulled back from an nn-dimensional tangential structure, it often happens that the input nn-dimensional tangential structure is itself pulled back from a higher-dimensional tangential structure:

Definition 6.3.

A stabilization of an nn-dimensional tangential structure X(n)BPL(n)X(n)\to\mathrm{B}\mathrm{PL}(n) is a map XBPL=inj limnBPL(n)X\to\mathrm{B}\mathrm{PL}=\injlim_{n\to\infty}\mathrm{B}\mathrm{PL}(n) and an equivalence X(n)X×BPLBPL(n)X(n)\cong X\times_{\mathrm{B}\mathrm{PL}}\mathrm{B}\mathrm{PL}(n). A tangential structure is stable when it is equipped with a stabilization.

We emphasize that stability is structure, not just a property.

Example 6.4.

Define a stable smooth structure on a PL-manifold MM to be a lift of its stabilized tangent bundle through BOBPL\mathrm{B}\mathrm{O}\to\mathrm{B}\mathrm{PL}. In other words, for an nn-manifold, stable smoothness corresponds to the tangential structure BO×BPLBPL(n)\mathrm{B}\mathrm{O}\times_{\mathrm{B}\mathrm{PL}}\mathrm{B}\mathrm{PL}(n). Stable smoothness is by construction a stable tangential structure.

Stable smoothness is weaker than smoothness: the map BO(n)BO×BPLBPL(n)\mathrm{B}\mathrm{O}(n)\to\mathrm{B}\mathrm{O}\times_{\mathrm{B}\mathrm{PL}}\mathrm{B}\mathrm{PL}(n) is not a homotopy equivalence. Indeed, actual-smoothness is not a stable tangential structure. Write 𝐁𝐨𝐫𝐝nO(n)\mathbf{Bord}_{n}^{\mathrm{O}(n)} for the (unoriented) actually-smooth bordism (,n)(\infty,n)-category and 𝐁𝐨𝐫𝐝nO\mathbf{Bord}_{n}^{\mathrm{O}} for the stably-smooth version. The map 𝐁𝐨𝐫𝐝nO(n)𝐁𝐨𝐫𝐝nO\mathbf{Bord}_{n}^{\mathrm{O}(n)}\to\mathbf{Bord}_{n}^{\mathrm{O}} is not an equivalence of (,n)(\infty,n)-categories.

That said, a careful analysis of smoothing theory shows that the map BO(n)BO×BPLBPL(n)\mathrm{B}\mathrm{O}(n)\to\mathrm{B}\mathrm{O}\times_{\mathrm{B}\mathrm{PL}}\mathrm{B}\mathrm{PL}(n) is nn-connected; in particular, this follows from [Lur09a, Lecture 21, Theorem 1]. In terms of bordism categories, this implies that 𝐁𝐨𝐫𝐝nO(n)𝐁𝐨𝐫𝐝nO\mathbf{Bord}_{n}^{\mathrm{O}(n)}\to\mathbf{Bord}_{n}^{\mathrm{O}} becomes an equivalence after quotienting to weak nn-, a.k.a. (n,n)(n,n)-, categories. The upshot is that for TQFTs valued in a weak nn-category, the notions of smooth and stably-smooth TQFT agree.

The description of kk-morphisms in 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} as XX-structured kk-dimensional cobordisms does not precisely present the actual space of kk-morphisms in 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X}. Indeed, the natural space of kk-dimensional XX-structured bordisms has as its equivalences the XX-structured diffeomorphisms. But the categorical equivalences in 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} between (<n)(<n)-dimensional morphisms also include XX-structured h-cobordisms, and in high dimensions not every h-cobordism comes from a diffeomorphism. Rather, this description presents a flagged (,n)(\infty,n)-category of bordisms as

(7) 𝐁𝐨𝐫𝐝0X𝐁𝐨𝐫𝐝1X𝐁𝐨𝐫𝐝nX.\mathbf{Bord}_{0}^{X}\to\mathbf{Bord}_{1}^{X}\to\dots\to\mathbf{Bord}_{n}^{X}.

The main result of this section is:

Statement 6.5.

Suppose that XBPLX\to\mathrm{B}\mathrm{PL} is a stable tangential structure. Then the flagged XX-structured bordism category (7) is naturally a flagged PL(n)\mathrm{PL}(n)-dagger (,n)(\infty,n)-category.

Construction.

To build a dagger on 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X}, we must first provide a PL(n)\mathrm{PL}(n)-volution. We will do this by twisting the canonical PL(n)\mathrm{PL}(n)-volution by a carefully-selected action of PL(n)\mathrm{PL}(n) on 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X}. To build such an action, consider the functor

𝐒𝐩𝐚𝐜𝐞/BPL𝐒𝐩𝐚𝐜𝐞/BPL(n)𝐒𝐲𝐦𝐂𝐚𝐭(,n)X𝐁𝐨𝐫𝐝nX\mathbf{Space}_{/\mathrm{B}\mathrm{PL}}\to\mathbf{Space}_{/\mathrm{B}\mathrm{PL}(n)}\to\mathbf{SymCat}_{(\infty,n)}\hskip 28.45274ptX\mapsto\mathbf{Bord}_{n}^{X}

which first pulls back a stable tangential structure {XBPL}𝐒𝐩𝐚𝐜𝐞/BPL\{X\to\mathrm{B}\mathrm{PL}\}\in\mathbf{Space}_{/\mathrm{B}\mathrm{PL}} to its unstable variant X(n):=X×BPLBPL(n)X(n):=X\times_{\mathrm{B}\mathrm{PL}}\mathrm{B}\mathrm{PL}(n) and then assigns the corresponding bordism category. To build an action of PL(n)\mathrm{PL}(n) on the resulting bordism category, it therefore suffices to specify a functor

BPL(n)𝐒𝐩𝐚𝐜𝐞/BPL,\mathrm{B}\mathrm{PL}(n)\to\mathbf{Space}_{/\mathrm{B}\mathrm{PL}},

i.e. an action of PL(n)\mathrm{PL}(n) on the bundle XBPLX\to\mathrm{B}\mathrm{PL}. Equivalently, we want to choose a bundle XBPL×BPL(n)X^{\prime}\to\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}(n) whose pullback along BPL=BPL×{pt}BPL×BPL(n)\mathrm{B}\mathrm{PL}=\mathrm{B}\mathrm{PL}\times\{\mathrm{pt}\}\to\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}(n) is XX.

Recall that BPL\mathrm{B}\mathrm{PL} is a coherently-associative monoid under \oplus, and that in homotopy theory a monoid is a group as soon as its π0\pi_{0} is a group. Thus BPL\mathrm{B}\mathrm{PL} comes with an operation :BPLBPL\text{``}{\ominus}\text{''}\colon\mathrm{B}\mathrm{PL}\to\mathrm{B}\mathrm{PL}, canonical up a contractible space of choices, that inverts with respect to the group operation \oplus. With this operation in hand, we choose to set XX^{\prime} to be the pullback of XBPLX\to\mathrm{B}\mathrm{PL} along the composition

BPL×BPL(n)BPL×BPLid×BPL×BPLBPL.\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}(n)\to\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}\xrightarrow{\mathrm{id}\times\ominus}\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}\xrightarrow{\oplus}\mathrm{B}\mathrm{PL}.

These actions are compatible: the inclusion 𝐁𝐨𝐫𝐝kX𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{k}^{X}\to\mathbf{Bord}_{n}^{X} intertwines the induced PL(k)\mathrm{PL}(k)-volutions. What remains is to trivialize a certain induced action of PL(nk)\mathrm{PL}(n-k) on 𝐁𝐨𝐫𝐝kX\mathbf{Bord}_{k}^{X}. Our PL(n)\mathrm{PL}(n)-volution on 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} was built out of two pieces: the canonical volution together with our choice XX^{\prime}. By the same token, the action of PL(nk)\mathrm{PL}(n-k) on 𝐁𝐨𝐫𝐝kX\mathbf{Bord}_{k}^{X} that we care about has two pieces. One piece is the restriction along PL(nk)PL(n)\mathrm{PL}(n-k)\to\mathrm{PL}(n) of the action on XBPLX\to\mathrm{B}\mathrm{PL}. The other piece comes from restricting the canonical volution along PL(nk)PL(n)\mathrm{PL}(n-k)\to\mathrm{PL}(n). Combining these pieces and writing the problem in terms of bundles, one finds that what needs trivializing is the restriction of XX along the composition

BPL(nk)diagBPL(nk)×BPL(nk)BPL×BPLid×BPL×BPLBPL.\mathrm{B}\mathrm{PL}(n-k)\xrightarrow{\operatorname{diag}}\mathrm{B}\mathrm{PL}(n-k)\times\mathrm{B}\mathrm{PL}(n-k)\to\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}\xrightarrow{\mathrm{id}\times\ominus}\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}\xrightarrow{\oplus}\mathrm{B}\mathrm{PL}.

But this composition factors through

BPLdiagBPL×BPLid×BPL×BPLBPL,\mathrm{B}\mathrm{PL}\xrightarrow{\operatorname{diag}}\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}\xrightarrow{\mathrm{id}\times\ominus}\mathrm{B}\mathrm{PL}\times\mathrm{B}\mathrm{PL}\xrightarrow{\oplus}\mathrm{B}\mathrm{PL},

which is trivial by the definition of \ominus. ∎

Remark 6.6.

Both the notion of a dagger category with unitary duals and Statement 6.5 are based on PL\mathrm{PL} geometry. There is an analogous story replacing PL(n)\mathrm{PL}(n) with O(n)\mathrm{O}(n) and PL\mathrm{PL}-geometry with smooth geometry. The smooth bordism category with smoothly stable tangential structure has a natural O\mathrm{O}-dagger structure.

Example 6.7.

Let us restrict to unextended bordism categories. Whereas the very definition of PL(n)\mathrm{PL}(n)-dagger (,n)(\infty,n)-category, and hence the content of Statement 6.5, required Conjecture 5.3, the definition in the unextended case and the construction described below are fully rigorous.

Because smooth bordism categories are more familiar than their piecewise-linear counterparts, we will focus on that case. For each XBO(n)X\to\mathrm{B}\mathrm{O}(n) there is a smooth XX-structured unextended bordism (,1)(\infty,1)-category 𝐁𝐨𝐫𝐝n,n1X\mathbf{Bord}_{n,n-1}^{X} whose objects are closed (n1)(n-1)-dimensional XX-structured manifolds and whose morphisms are XX-structured nn-dimensional bordisms. This category is naturally flagged: the naïve equivalences between objects in 𝐁𝐨𝐫𝐝n,n1X\mathbf{Bord}_{n,n-1}^{X} are the XX-structured diffeomorphisms, but the categorical equivalences also include XX-structured h-cobordisms; writing Mann1X\operatorname{Man}_{n-1}^{X} for the space of XX-structured closed (n1)(n-1)-manifolds and diffeomorphisms between them, we find a flagged (,1)(\infty,1)-category

Mann1X𝐁𝐨𝐫𝐝n,n1X\operatorname{Man}_{n-1}^{X}\to\mathbf{Bord}_{n,n-1}^{X}

which is often not univalent.

Since 𝐁𝐨𝐫𝐝n,n1X\mathbf{Bord}_{n,n-1}^{X} is rigid symmetric monoidal, it has a canonical anti-involution (which is to say a volution for the group PL(1)=/2\mathrm{PL}(1)=\mathbb{Z}/2\mathbb{Z}). It is precisely the operation ()(-)^{\vee} that takes duals. This canonical anti-involution typically does not extend to a dagger structure: for example, when X=SOX=\mathrm{SO}, the dual of an object is its orientation-reversal, and most oriented manifolds simply are not orientation-diffeomorphic to their orientation reversals. This is why we needed to find an appropriate twist by a symmetric monoidal action.

Suppose that our tangential structure is stable, i.e. (in the smooth case) pulled back from BO\mathrm{B}\mathrm{O}. We will twist the canonical anti-involution on 𝐁𝐨𝐫𝐝n,n1X\mathbf{Bord}_{n,n-1}^{X} by the involution on XBOX\to\mathrm{B}\mathrm{O} built by restricting along the composition

(8) BO×B(/2)=BO×BO(1)BO×BOid×BO×BOBO.\mathrm{B}\mathrm{O}\times\mathrm{B}(\mathbb{Z}/2\mathbb{Z})=\mathrm{B}\mathrm{O}\times\mathrm{B}\mathrm{O}(1)\to\mathrm{B}\mathrm{O}\times\mathrm{B}\mathrm{O}\xrightarrow{\mathrm{id}\times\ominus}\mathrm{B}\mathrm{O}\times\mathrm{B}\mathrm{O}\xrightarrow{\oplus}\mathrm{B}\mathrm{O}.

To finish the construction of a dagger structure, we take the corresponding twisted anti-involution, restrict it to the (flagged) groupoid Mann1X\operatorname{Man}_{n-1}^{X} of objects where it becomes an involution, and trivialize it. This involution combines duality with the chosen involution on XBOX\to\mathrm{B}\mathrm{O}.

In general, given an nn-dimensional tangential structure XBO(n)X\to\mathrm{B}\mathrm{O}(n), the duality involution on Mann1X\operatorname{Man}_{n-1}^{X} is the one built from restricting XX along BO(n1)×B(/2)=BO(n1)×BO(1)BO(n)\mathrm{B}\mathrm{O}(n-1)\times\mathrm{B}(\mathbb{Z}/2\mathbb{Z})=\mathrm{B}\mathrm{O}(n-1)\times\mathrm{B}\mathrm{O}(1)\to\mathrm{B}\mathrm{O}(n). Together with the twisting, we find that we win if the total composition

BO(n1)×B(/2)id×diagBO(n1)×B(/2)×B(/2)BO(n)×B(/2)(8)BO\mathrm{B}\mathrm{O}(n-1)\times\mathrm{B}(\mathbb{Z}/2\mathbb{Z})\xrightarrow{\mathrm{id}\times\operatorname{diag}}\mathrm{B}\mathrm{O}(n-1)\times\mathrm{B}(\mathbb{Z}/2\mathbb{Z})\times\mathrm{B}(\mathbb{Z}/2\mathbb{Z})\to\mathrm{B}\mathrm{O}(n)\times\mathrm{B}(\mathbb{Z}/2\mathbb{Z})\xrightarrow{\eqref{eqn:smoothunextended}}\mathrm{B}\mathrm{O}

agrees with the canonical map BO(n1)BO\mathrm{B}\mathrm{O}(n-1)\to\mathrm{B}\mathrm{O}. And it does by virtue of \ominus.

Statement 6.8.

The twist defined in (8) is the same twist used to form H^n(1)\hat{H}^{(1)}_{n} in [FH21, Appendix E], and hence our dagger structure agrees with the dagger structure implicit in [FH21].

Symmetric monoidal dagger structures on bordism categories are relevant for the definition of reflection positivity [Ati88, Bae06, TV17, FH21, Ste24]. As a motivating example, consider the anti-involution on the symmetric monoidal category of finite dimensional super vector spaces 𝐬𝐕𝐞𝐜𝐭\mathbf{sVect} given by twisting the canonical one by the /2\mathbb{Z}/2\mathbb{Z}-action corresponding to complex conjugation. The category of fixed points (ι0𝐬𝐕𝐞𝐜𝐭)/2(\iota_{0}\mathbf{sVect})^{\mathbb{Z}/2} describes Hermitian super vector spaces and unitary maps between them. We denote by 𝐬𝐇𝐢𝐥𝐛u(ι0𝐬𝐕𝐞𝐜𝐭)/2\mathbf{sHilb}^{u}\subset(\iota_{0}\mathbf{sVect})^{\mathbb{Z}/2} its full subcategory on the super Hilbert spaces and by 𝐬𝐇𝐢𝐥𝐛\mathbf{sHilb} the coherent dagger 1-category

𝐬𝐇𝐢𝐥𝐛u𝐬𝐕𝐞𝐜𝐭.\mathbf{sHilb}^{u}\to\mathbf{sVect}.

An XX-structured unextended topological quantum field theory Z:𝐁𝐨𝐫𝐝n,n1X𝐬𝐕𝐞𝐜𝐭Z\colon\mathbf{Bord}^{X}_{n,n-1}\to\mathbf{sVect} has a reflection structure when it is a functor of anti-involutive, or equivalently /2\mathbb{Z}/2\mathbb{Z}-equivariant, categories. A field theory with reflection structure is called reflection positive if it induces a dagger functor 𝐁𝐨𝐫𝐝n,n1X𝐬𝐇𝐢𝐥𝐛\mathbf{Bord}^{X}_{n,n-1}\to\mathbf{sHilb}: if the Hermitian structures induced by Example 6.7 on the images of ZZ are all positive definite. Reflection positivity encodes physical unitarity. Thus we propose the following tentative definition:

Proposal 6.9.

Let 𝒞\mathcal{C} be a rigid symmetric monoidal PL(n)\mathrm{PL}(n)-dagger (,n)(\infty,n)-category. A unitary XX-structured extended topological quantum field theory valued in 𝒞\mathcal{C} is a functor of symmetric monoidal PL(n)\mathrm{PL}(n)-dagger categories 𝐁𝐨𝐫𝐝nX𝒞\mathbf{Bord}_{n}^{X}\to\mathcal{C}.

Remark 6.10.

Proposal 6.9 is to be interpreted loosely as the type of definition we expect to be correct. However, there are many details to be pinned down. For instance, we expect the dagger structure on 𝐁𝐨𝐫𝐝nX\mathbf{Bord}_{n}^{X} from Statement 6.5 to be part of a PL\mathrm{PL}-dagger tower  and a unitary extended topological field theory might be required to respect this structure. In addition, our proposal prefers the PL\mathrm{PL}-bordism category, but the smooth version from Remark 6.6 might be more appropriate in certain applications.

Fully defining unitary extended topological quantum field theory furthermore requires settling on good target categories 𝒞\mathcal{C}. Without unitarity, good target categories should feel like higher categories of “higher vector spaces” or “higher super vector spaces”; with unitarity, one should instead expect 𝒞\mathcal{C} to organize the “higher (super) Hilbert spaces.” In upcoming work [CFH+], some of us construct a symmetric monoidal (,3)(\infty,3)-category 𝐇𝐢𝐥𝐛3\mathbf{Hilb}_{3} of “finite-dimensional 3-Hilbert spaces.” It is rigid by construction, and moreover it is expected to carry an organic PL(3)\mathrm{PL}(3)-dagger structure. Together with Definition 6.9 and Statement 6.5, one arrives at a definition of 33-dimensional bosonic fully-extended unitary topological quantum field theories for any stable tangential structure. The construction of 𝐇𝐢𝐥𝐛3\mathbf{Hilb}_{3} in [CFH+] starts with the usual dagger 11-category 𝐇𝐢𝐥𝐛\mathbf{Hilb} of finite-dimensional Hilbert spaces and repeatedly applies a certain manifestly-dagger delooping procedure. This delooping procedure is expected to extend to even higher categories as well.

Another candidate for 𝐇𝐢𝐥𝐛3\mathbf{Hilb}_{3} weakening the finite dimensionality conditions would be an appropriate Morita 33-category of Bicommutant Categories. Bicommutant categories as first introduced in [Hen17]; their Morita theory is under development. Similar to the 3-category 𝐓𝐞𝐧𝐬𝐂𝐚𝐭\mathbf{TensCat}, the category of Bicommutant categories, bicommutant category bimodules (W*-categories), equivariant functors and natural transformations, called 𝐁𝐢𝐜𝐨𝐦𝐂𝐚𝐭\mathbf{BicomCat} could serve as target for unitary quantum field theories, more general than just TQFTs, for instance chiral conformal field theories. It is expected that this category is a strictly fully-dagger, with involutions given by the categorical op\mathrm{}^{\mathrm{op}} operation on objects and 1-morphisms and using adjoint functors and natural transformations on the top two levels.

Further analysis of Definition 6.9 — construction of examples, a Unitary Cobordism Hypothesis, etc.  — will be the subject of future work.

Acknowledgements

The authors would like to thank the other participants of the June 2023 Zoom workshop on Dagger Higher Categories: Bruce Bartlett, André Henriques, Chris Heunen, Peter Selinger, and Dominic Verdon, along with Jan Steinebrunner. The authors acknowledge the following grant support:

GF, BH, DP NSF DMS 2154389
CK NSF GRFP 2141064
TJF NSERC RGPIN-2021-02424
TJF, LM, CS, LS Simons Collaboration on Global Categorical Symmetries (Simons Foundation grants 888996 and 1013836)
LS Atlantic Association for Research in the Mathematical Sciences
DR Deutsche Forschungsgemeinschaft (DFG) – 493608176
CS Deutsche Forschungsgemeinschaft (DFG) – SFB 1085 Higher Invariants
N James Buckee Scholarship, Merton College, Oxford

Research at Perimeter Institute is supported in part by the Government of Canada through the Department of Innovation, Science and Economic Development and by the Province of Ontario through the Ministry of Colleges and Universities.

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