Where charged sectors are localizable: a viewpoint from covariant cohomology

Given a Haag-Kastler net on a globally hyperbolic spacetime, one can consider a family of regions where quantum charges are supposed to be localized. Assuming that the net fulfils certain minimal properties (factoriality of the global observable algebra and relative Haag duality), we give a geometric criterion that the given family must fulfil to have a superselection structure with charges localized on its regions. Our criterion is fulfilled by all the families used in the theory of sectors (double cones, spacelike cones, diamonds, hypercones). In order to take account of eventual spacetime symmetries, our superselection structures are constructed in terms of covariant charge transporters, a novel cohomological approach generalizing that introduced by J.E. Roberts. In the case of hypercones, with the forward light cone as an ambient spacetime, we obtain a superselection structure with Bose-Fermi parastatistics and particle-antiparticle conjugation. It could constitute a candidate for a different description of the charged sectors introduced by Buchholz and Roberts for theories including massless particles.


Introduction
The analysis of superselection sectors has been a topic of interest since the early days of algebraic quantum field theory, in particular in the celebrated DHR analysis [17,18,19,20].There, superselection sectors are intrinsically characterized in terms of endomorphisms of the observable C*-algebra A, realized on the vacuum Hilbert space H .The endomorphisms of interest, say ρ ∈ endA, are localized in double cones O ⊂ R 4 , in the sense that ρ equals the identity on any subalgebra of A generated by observables localized in regions causally disjoint from O (DHR endomorphisms).The relation with superselection sectors in the sense of Wigner, Wick and Wightman, that define Hilbert space representations of the type π : A → B(H π ), is that there is a unitary equivalence π ≃ ρ having regarded ρ as a representation ρ : A → A ⊂ B(H).This yields the DHR criterion to select the endomorphisms of interest: the physical interpretation is that there is a quantum charge localized in O that induces a superselection sector disjoint from the vacuum.
An alternative way to look at DHR superselection sectors was proposed by J.E. Roberts.Guided by the concept of parallel transport, Roberts introduced a families of unitary operators X b ∈ A, where b are triples of double cones ∂ 0 b, ∂ 1 b ⊆ |b| ⊂ R 4 , [29,30].These unitaries satisfy a cocycle relation and realize an equivalence between the DHR endomorphisms ρ(∂ 1 b) and ρ(∂ 0 b) localized in ∂ 1 b and ∂ 0 b respectively, as Hence, the physical idea is that a quantum charge, localized in ∂ In Minkowski space the Roberts approach is equivalent to the classical DHR formulation.Yet in curved spacetimes it turned out that charge transporters are unavoidable, because the DHR endomorphisms alone do not carry all the necessary physical informations [32,1].Successive work has shown that the analogy with parallel transport is fully justified by the fact that, when A is the observable net of the free Dirac field ψ , for any charge transporter X there is a closed 1-form A on M, such that Here, ψ ∂ 0 b , ψ ∂ 1 b are charged unitaries obtained by smeared field operators by using the III-type factor property of the local algebras, inducing the DHR endomorphisms by adjoint action.They carry opposite charges, coherently with the ideas of [26,8].The physical interpretation is that A is an external potential interacting with ψ , inducing observable effects in spacetimes with non-trivial fundamental group (Aharonov-Bohm effect) and vanishing in simply connected spacetimes.Expressions analogous to (1.2) can be obtained for a non-Abelian gauge group, with A a flat connection with values in the corresponding Lie algebra [34,35,16] 1 .
A different superselection structure was proposed by Buchholz and Fredenhagen, which introduced a criterion based on positivity of the energy and arrived to a charge localization in spacelike cones [8].This type of localization reflects the idea that a spacelike cone is able to host two opposite charges, one of which is free to go to (or to come from) spacelike infinity, behind the moon following Haag and Kastler [26].This introduces a further level for the regions of interest: we have bounded regions (double cones) in which the observables are localized, and unbounded regions (spacelike cones) encoding the localization of charges.This suggests to define by additivity a new observable net, say A K , indexed by the charge localization regions instead of the usual family of double cones.As spacelike cones are not upward directed under inclusion, the so-obtained sectors are now described by net morphisms ρ : A K → B(H) (BF-morphisms) that in general do not match to form endomorphisms of the global C*-algebra.In spite of this difficulty, they form a mathematical structure analogous to the one obtained by DHR sectors, namely a symmetric tensor category with conjugates encoding a permutation symmetry with Bose-Fermi parastatistics and particle-antiparticle correspondence.
In lower dimensions, because of topological obstructions different properties manifest themselves at the level of statistics.The braid group appears instead of the permutation group when the exchange of charges is performed, and exotic statistics appear.Such sectors have been studied in [22,23].In the present paper we focus on four spacetimes dimensions, so that we will always deal with Bose-Fermi (para)statistics.
All the previous approaches share an assumption, namely the absence of massless particles.This of course excludes QED, which presents peculiarities that create serious problems for the identification of superselection sectors.Notably, the electric charge cannot be localized (not even in a spacelike cone), and charged fields cannot be local to the electromagnetic field in positive (and hence physical) gauges.Both the problems have their root in the Gauss law [33, §7.2].The search for a superselection structure describing the electric charge was approached in several papers [24,2,10,11], culminating in the analysis by Buchholz and Roberts [9].There, a crucial point is that the ambient spacetime is restricted to the future light cone V + , in such a way to rule out the infrared clouds giving rise to the overabundance of sectors with the same electric charge.The restriction on V + has also consequences as the loss (then amended) of the full group of Poincaré symmetry, which is restricted to an action by the semigroup stabilizing V + , and the eventuality that A(V + ) (now generated by observables localized in V + ) is not irreducible.This has an impact on Haag duality, that now must be referred to the von Neumann algebra A(V + ) ′′ that is not necessarily B(H) but more generally a III 1 factor.The result is a family of approximately inner morphisms σ : A(V + ) → A(V + ) ′′ , localized on hypercones and giving rise to the desired superselection structure (BR-sectors) even if some questions remain open for parastatistics.
The present paper has two main objectives.First, identify the essential features that define a class of regions within a globally hyperbolic spacetime which can serve as localization regions for charged superselection sectors.To emphasize this point, we describe these properties using a partially ordered set (poset), and consider the observable net defined on it.
Secondly, develop a novel approach to superselection sectors in terms of covariant 1cocycles: charge transporters that maintain covariance with respect to a global symmetry of the spacetime.This concept extends the cohomology introduced by Roberts and addresses a gap in this approach, as the covariant properties of superselection sectors have previously only been discussed in terms of localized and transportable morphisms.This aspect holds significance because it allows, in principle, for the examination of covariant superselection sectors on spacetimes with nontrivial topology.In such cases, in fact, the conventional approach relying on localized and transportable morphisms may prove inadequate [1].
We demonstrate that our superselection structure possesses permutation symmetry with Bose-Fermi (para)statistics, and a conjugation that encodes the particle-antiparticle correspondence.This machinery applies to the known situations described in the previous lines.Yet, whilst for double cones and spacelike cones we easily get the DHR and BF superselection structures respectively, in the case of hypercones it remains an open question whether our superselection structure agrees with the one constructed by Buchholz and Roberts.We postpone this discussion to future works, with the remark that, due to the generality of our approach, we did not take into account the energetic aspects that come into play when the transport of a charge towards the boundary of the light cone is performed2 .
In the following lines we give a sketch of the content of the next sections.
In §2 we fix a poset modelled on a family of regions of a spacetime M encoding the charge localization and the geometry of the spacetime.Namely, we consider a possibly curved spacetime denoted as M, foliated along time and equipped with a symmetry action given by spacetime transformations.In general, only symmetries that preserve the charge localization regions are of interest, and in all the mentioned examples they form a group (even in the case of charges of electromagnetic type, despite the stabilizer of the forward light cone is a semigroup of Poincaré transformations, the symmetries that stabilize the hypercones are given by the Lorentz group).
Hence, we consider an abstract poset K endowed with a causal disjointness relation ⊥ and acted upon by a symmetry P , and determine two properties that the elements of K must fulfill to play the role of localization regions in a superselection structure expressed in terms of charge transporters.The two properties are that the causal complement of any o ∈ K must be pathwise connected, and that for any pair otherwise there are õ1 , ã such that õ1 ⊂ o 1 and ã ⊥ õ1 , o 2 .The former property ensure that we can freely transport charges along paths in the causal complement of o, whilst the latter allows to add further charges without interfering with a previously given set of mutually casually disjoint charges.
We then consider in §2.2 local von Neumann algebras A(o) for any element of o of K defined in a reference Hilbert space H 3 .The correspondence A K : o → A(o) gives a net of von Neumann algebras over K on which we require minimal assumptions derived from the existing theory of superselection sectors: the symmetry action of P on A K is unitarily implemented; the C * -algebra A(K) generated by A(o) as o varies in K is factorial, A(K) ′ ∩ A(K) ′′ = C 1 H ; relative Haag duality holds [12], where A(o ⊥ ) is the von Neumann algebra associated with the causal complement o ⊥ of o.
In §3, starting from A K we introduce the notion of covariant cocycle.It simultaneously yields a cocycle (charge transporter) in the sense of Roberts and a cocycle over P .Covariant cocycles are designed to encode in a concise way P -covariant superselection sectors.Considering for simplicity only simply connected spacetimes (hence simply connected posets) in order to rule out the above mentioned Aharonov-Bohm vector potentials, we prove that covariant cocycles form a C*-category Z 1 c (A K ).A further analysis shows that Z 1 c (A K ) has permutation symmetry with Bose-Fermi (para)statistics and conjugates, and hence is endowed with the properties characterising a charged superselection structure.
M being simply connected, Z 1 c (A K ) can be described in terms of morphisms from A K into A(K) in the sense of [31]; these morphisms are localized on regions o ∈ K §3.3, and in good cases (e.g. when K is the set of double cones), they form actual endomorphisms of A(K).For various choices of M and K , we get DHR sectors (when M = R 4 and K is given by double cones), BF sectors (M = R 4 , K given by spacelike cones), and sectors in curved spacetimes (M a globally hyperbolic spacetime, K the family of diamonds).When M is the light cone and K is formed by hypercones, we get a superselection structure describing hypercone localized charges as explained in the previous lines.
In the final §4 we expose some conclusions and discuss future developments of our work.

The observable net
The investigation of charged superselection sectors within a given spacetime requires to consider observables in regions where the charges are localized, on the ground of a physical criterion.This leads to a correspondence assigning to such charge localization regions the algebras of observables measurable within them.As usual, such algebras are obtained by additivity, starting from Haag-Kastler nets.In the following we shall refer to the set of charge localization regions as the set of indices.

The set of indices
In the present section we discuss the essential properties defining a set of indices for due purposes.For convenience we regard it as an abstract partially ordered set (poset) whose properties are modelled on a suitable family of open regions, ordered under inclusion, of a connected and simply connected 4-dimensional globally hyperbolic spacetime M having non-compact Cauchy surfaces, and endowed with an action by spacetime symmetries when present.As illustrated in the introduction, the hypothesis of M being simply connected is motivated by the wish of simplifying the exposition, excluding Aharonov-Bohm type effects.Anyway we remark that, even if M is simply connected, K may be not directed.
Let K denote a non-empty partially ordered set with order relation ⊆.Elements of K are denoted by Latin letters o, a....In the following lines we give the list of properties that we assume for K : with the exception of K4 and K6 that are the crucial ones, they are natural requirements dictated by the idea that K is the abstraction of a family of causally complete regions in a 4-dimensional spacetime, stable under the action of a group P that is either the full group of spacetime symmetries or a subgroup thereof.
In the previous line, the symbol ⊂ stands for any relation implying o ⊆ õ and o = õ, and shall be defined concretely when we will consider examples of K .The poset K is endowed with a causal disjointness relation i.e. a symmetric, non-reflexive binary relation ⊥, compatible with the order relation in the sense that We assume that all the elements of K are causally complete in the sense that Note that this implies that o ⊥ = ∅.A key property is the following We assume that K is acted upon by a group P , the symmetry, and that this action is compatible with the order and causal disjointness relations Before to proceed with our list, for the reader's convenience we introduce some properties of K having a topological flavour, expressed in terms of the set of singular n-simplices Σ n (K) (see [32] for details).A 0-simplex is just an element of K , that we usually write a, o. x can be regarded as a degenerate n-simplex σ i (x) obtained by repeating its i vertex.
The symbols ∂ i and σ i define face and degeneracy maps respectively.To be concise, we write the compositions It can be proved that The support |p| of a path p is the collection of the supports of the 1-simplices by which it is composed.The reverse of p is the path p : o → a defined by p .
If q is a path from o to ô, then we can define, in an obvious way, the composition q * p : a → ô.A subset S ⊆ K is said to be pathwise connected whenever for any pair a, ã of 0-simplices in S there is a path from a to ã.We are now ready to give our last properties.
K6 We assume that the K is pathwise connected and that the causal complement o ⊥ of any element o ∈ K is pathwise connected.
An elementary deformation of a path . Two paths with the same endpoints are homotopic if they can be obtained from one another by a finite sequence of elementary deformations.Homotopy defines an equivalence relation ∼ on the set of paths with the same endpoints and, K being pathwise connected, this naturally leads to the notion of the fundamental group π 1 (K) of K .In all the cases of interest in the present paper, it turns out π 1 (M) ≃ π 1 (K) [32].The following hypothesis is formulated to simplify the discussion of the next section: K7 We assume that K is simply connected, i.e. π 1 (K) = 1.
We finally observe that the action of the symmetry P on K extends to simplices by taking λx as the n-simplex whose faces are λ∂ i x and whose support is |λx| = λ|x|.This induces an action on paths, which preserves the homotopy equivalence relation, defined by Note that if p : a → o then λp : λa → λo.

Observable net and reference representation
We now add the further ingredients given by the observable net and its reference representation.Since we are not assuming that K is upward directed, we have to take into account the notions of morphism and representation of a net, as in [31].
Let H be a Hilbert space.An observable net over K is given by a correspondence assigning to o ∈ K the von Neumann algebra A(o).We denote the C * -algebra generated by ∪ o∈K A(o) by A(K), and assume the standard properties of isotony, causality, and P -covariance under a representation U : P → U (H). Finally we assume • the Borchers property: for any o ⊂ a and for any projection E ∈ A(o) there is an isometry V ∈ A(a) such that V V * = E ; • relative Haag duality, where, in our abstract setting, we may take as a definition A(o ⊥ ) ′ = a⊥o A(a) ′ .Note that factoriality is a weaker assumption with respect to the irreducibility property usually required.It is dictated by the hypothesis made by Buchholz and Roberts for their net defined on the light cone [9].In this connection, note that when the net is irreducible relative Haag duality becomes the usual Haag duality.

Meaningful examples
We now give some concrete examples where a set of indices K and observables net over K satisfying the properties introduced above arise.The general context is that of a connected and simply connected 4-dimensional globally hyperbolic spacetime M, with non-compact Cauchy surfaces and, possibly, symmetries (i.e.global isometries).K can be any suitable family of open subsets of M, ordered under inclusion and with the causal disjointness relation induced by the causal structure of M. To be precise: • • the action λo of a symmetry λ on a region o is nothing but the image λ(o); • finally, the symmetry P is the subgroup of symmetries of M that leave invariant K .
The defining properties of K and the assumptions we made on A K are verified in the following cases.
1.The DHR sectors [19,20].Here M is the 4-dimensional Minkowski space, P the Poincaré group, K the set of double cones and A K is the observable net defined in the vacuum representation.
2. The DHR sectors in curved spacetimes [25,32,1].Here M is an arbitrary 4dimensional globally hyperbolic spacetime with non-compact Cauchy surfaces, K is the set of diamonds and A K is the observable net in a representation satisfying the microlocal spectrum condition.4. The BR charge classes (charges of electromagnetic type) [9].Here M is the forward light cone in the 4-dimensional Minkowski space and K is the set of hypercones in M.Although M has a semigroup of symmetries given by the semidirect product of non-negative time translations and the Lorentz group, K is not stable under nonnegative time translations.As a consequence P corresponds to the Lorentz group.

The BF sectors
A K is defined by the observable net in the vacuum representation: since hypercones are unbounded, elements of A K are generated, similarly to the BF sectors, by the algebras of double cones that are located within each hypercone.
We conclude by noting that violations of the properties K1-7, to the authors' knowledge, occur in low-dimensional spaces.For example, in 2-dimensional Minkowski space the causal complement of double cones is not connected, see [22].In 3-dimensional Minkowski space, spacelike cones have connected complement but form a poset with non-trivial homotopy group, isomorphic to Z, ref. [27,28].These violations and other topological restrictions like for instance that in these posets there are pairs of causally disjoint elements whose causal complements have non-connected intersection are the reasons for the appearance of anyonic sectors.

Covariant cohomology and charged representations of the observable net
In the present section we introduce covariant 1-cocycles and, following the DHR analysis, we show that they define a symmetric tensor C * -category with conjugates, closed under direct sums and subobjects.This implies that charged quantum numbers are associated with the equivalence class of any irreducible covariant 1-cocycle.Using the hypothesis that M is simply connected, we construct morphisms of the observable net A K into the global C*-algebra, describing charges localized in regions of K .Finally, we illustrate how covariant 1-cocycles shift the localization regions of our localized morphisms, confirming their interpretation as charge transporters.

Covariant 1-cocycles of the observable net
We define and start to analyze the covariant cohomology of a given observable net A K fulfilling the hypothesis of §2.1 and §2.2.The focus is on the relation between our covariant cohomology and that introduced by J.E. Roberts, which provides an equivalent description of DHR superselection sectors as mentioned in the Introduction.
The equality (3.1) is a covariant extension of the 1-cocycle equation introduced by J.E. Roberts in [29,30].For, if e ∈ P is the identity and recovering the defining property of a Roberts 1-cocycle.Now, it is worth recalling a key property of Roberts 1-cocycles and its consequences.Any Roberts 1-cocycle extends from 1-simplices to paths and (3.2) implies that any Roberts 1-cocycle is homotopy invariant, that is, X p = X q for p homotopic to q .Since K is simply connected, by K7 we find and denoting an arbitrary path from o to a by p o,a we conclude that: • λp o,a ≃ p λo,λa and X λpo,a = X p λo,λa for any λ ∈ P .
As a consequence of the above properties, for any o ∈ Σ 0 (K) we can define thus X b (λ) is independent of the support of the degenerate 1-simplex and (3.3) is welldefined.We conclude this section by showing an identity that will be extensively used in the sequel.
Lemma 3.2.Given a covariant 1-cocycle X , for any path p : o → õ and for any λ ∈ P we have Proof.First assume that p is a 1-simplex b.Consider the 2-simplex c defined by Then by (3.1) we have Considering the 2-simplex c defined by and applying again (3.1) to the previous identity we get Thus if p : o → õ then the proof follows by iterating the same reasoning to all the 1simplices of the path.

The category of covariant 1-cocycles
Our final aim is to prove that covariant 1-cocycles are nothing but covariant charge transporters of the observable net.To this end we must exhibit, analogously to the DHR analysis, a charge structure encoded by a symmetric tensor C * -category with conjugates, associated with the analogues of DHR and BF endomorphisms.In the present section we make a first step towards this direction by showing that covariant 1-cocycles form a C * -category closed under direct sums and subobjects.
We denote the set of the intertwiners from X to Y by (X, Y ).
The category of covariant 1-cocycles Z 1 c (A K ) is the category with objects covariant 1-cocycles and arrow the above-defined intertwiners, equipped with the composition law (X, The identity arrow of a covariant 1-cocycle X is defined by (1 X ) a := 1 H for any 0-simplex a.The norm and the involution of B(H) endow Z 1 c (A K ) of a structure of C * -category.In particular, the adjoint of t ∈ (X, Y ) is defined by To check that t * ∈ (Y, X), we observe that by (3.1) we have , where b is the reverse of b.So, using this identity we have Passing to the involution, we get We recall some notions on C * -categories.A projection is an arrow e ∈ (X, X) such that e * •e = e; an isometry is an arrow Two objects X, Y are said to be equivalent whenever there is a unitary arrow u ∈ (X, Y ).Finally, an object X is said to be irreducible if (X, X) = C • 1 X .A C * -category is closed under subobjects if for any projection e ∈ (X, X) there are an object Y and an isometry v ∈ (X, Y ) s.t.w • w * = e, and closed under (finite) direct sums if for any pair of objects X, Y exists an object Z and a pair of isometries w ∈ (X, Z) and An obvious example of irreducible object of Z 1 c (A K ) is the identity I defined by for any 1-simplex b.Since K is pathwise connected, this implies that a → t a is a constant field, t a = τ for any 0-simplex a, and causality implies τ ∈ A(K) ∩ A(K) ′′ = C1 H . Clearly, any covariant 1-cocycle X equivalent to I is irreducible.We conclude this section with the following Proposition 3.4.Z 1 c (A K ) is a C * -category closed under direct sums and subobjects.
Proof.We have already seen that Z 1 c (A K ) is a C * -category.Let us prove that Z 1 c (A K ) is closed under subobjects.We adapt to the case of covariant 1-cocycles the proof given by Roberts in [29] for 1-cocycles.Let e ∈ (X, X) be a projection.For any 0-simplex a we choose a 0-simplex k(a) such that k(a) ⊂ a.By the Borchers property there is an isometry and Observe that w a is an isometry of A(a).In fact Finally So Y is a covariant 1-cocycle as well and it is a subobject of X because w ∈ (X, Y ) is an isometry s.t.w • w * = e.In a similar way one can prove that Z 1 c (A K ) is closed under direct sums.

Covariant, localized and transportable endomorphisms
In this section we show that Z 1 c (A K ) is equivalent to a category of morphisms of A K with values in the global C*-algebra A(K) ⊆ B(H).The term morphism is intended in the sense of [31], that is, we have a family ̺ of *-morphisms (3.5) Our morphisms, that we shall construct starting from Z 1 c (A K ), result to be localized, transportable and covariant.Moreover, in Minkowski spacetime they reduce to the DHR endomorphisms and to the BF morphisms, picking as sets of indices the ones of double cones and spacelike cones respectively.Thus we interpret our morphisms as quantum charges, that result to be transported by covariant cocycles.From a mathematical point of view, these morphisms prove to be the key to introducing the tensor product on the category of covariant cocycles (see next section).
Let X be a covariant 1-cocycle.Given o ∈ K .For any a ∈ K we take ã ⊥ a and define This definition is well posed.For, if â another element of K which is causally disjoint from a, since the causal complement of a is pathwise connected, there is a path p â,ã contained in the causal complement of a.So where we used homotopy invariance and the fact that X p â,ã commutes with A(a) because p â,ã is in the causal complement of a.Moreover, picking a ′ ⊇ a and ã ⊥ a We note that ρ(o) can be extended to the algebra generated by a finite number of regions a 1 , . . ., a n provided that there exists ã ⊥ a 1 , a 2 , . . ., a n : In this case we shall use the notation Our aim is now to prove that (3.7) generalize DHR endomorphisms, in the sense that they are localized, transportable and, moreover, covariant.
Lemma 3.5.The following assertions hold: Since the causal complement of a is pathwise connected, we may take a path p o,ã laying in the causal complement of a.So ρ(o) a (A) = X p o,ã AX p ã,o = A for any A ∈ A(a).
(ii) Let a ⊥ õ and A ∈ A(a).By (i) we have ρ(o) a (A) = A. Now, by taking ã ⊥ õ, a (here we are using again property K4 of the poset K ) we have that Since this holds for any a ⊥ õ, the proof follows by relative Haag duality.
(iii) Given A ∈ A(a), by homotopy invariance because X ã ∈ A(ã) and commutes with A. Remark 3.1.In particular, the previous point (iii) shows that the unitaries X p ô,o intertwine ρ(o) and ρ(ô).This is interpreted as the fact that X transports along the path p ô,o the charge defined by ρ.
What remains to be proved is that ρ := {ρ(o)} is covariant.To this end we define We have the following Lemma 3.6.Let X be a covariant 1-cocycle, and ρ, U ρ be defined as above.Then the following assertions hold: for any A ∈ A(a) and λ ∈ P . Proof.(i) (ii) Given A ∈ A(a), take â ⊥ a and by a direct computation we have that completing the proof.
The above result motivates the following definition.
Definition 3.7.A localized and transportable morphism ρ of A K is given by a collection ρ(o) : and for any pair o, õ ∈ K there are unitaries v ρ o,ô ∈ A such that A localized and transportable morphism ρ is covariant whenever for any o ∈ K there is a unitary representation U ρ o of P such that  [31].When the set of indices is upward directed, ρ(o) defines a *-endomorphism of the global observable algebra A(K), see [29,30].This holds in particular in Minkowski spacetime, for K given by double cones (so that we recover DHR endomorphisms).We also note that we recover the BF-morphisms in the case of spacelike cones.
We now extend at the level of C * -categories the correspondence between covariant 1-cocycles and localized, transportable and covariant morphisms.Taking localized, transportable and covariant morphisms of A K as objects and the corresponding set of intertwiners, we get a category denoted by ∆ c (A K ).The involution and the norm of B(H) endow this category of a structure of a C * -category.We call ∆ c (A K ) the category of localized, transportable and covariant morphisms of A K .
Next step is to prove that we have a covariant functor from Z 1 c (A K ) to ∆ c (A K ).The equations (3.6) and (3.9) defines the functor on the objects.To define our functor on the arrows, for any pair X, Y of covariant 1-cocycles we consider the corresponding morphisms ρ, γ ∈ ∆ c (A K ) and t ∈ (X, Y ).Then, for any o ∈ K , by definition (3.6) we have So t ∈ (ρ, γ), and we have a covariant functor from Z 1 c (A K ) to ∆ c (A K ).
Proposition 3.9.The C * -categories Z 1 c (A K ) and ∆ c (A K ) are equivalent.
Proof.We define the functor from ∆ c (A K ) to Z 1 c (A K ).Let ρ ∈ ∆ c (A K ) and denote the corresponding transporting unitaries and representation of P by v and U , respectively (we omit the sup-script ρ to simplify the notation).Fix an element a ∈ K , the pole, and define Clearly while the definition depends on the pole a it is independent of the choice of the paths joining the pole a because v a,o are Roberts 1-cocycles.We prove that X b (λ) ∈ A(|b|): for any o ⊥ |b| and A ∈ A(o) we have and the proof follows by relative Haag duality.For any 2-simplex c we have and this proves that X is a covariant 1-cocycle.Let now t ∈ (ρ, γ) be an intertwiner.We define φ(t) o := v ρ oa t a v γ ao .Note that φ(t) o ∈ A(o) since for any ã ⊥ o and A ∈ A(ã) we have and relative Haag duality makes the rest of the proof.Then It is easy to see that this defines a covariant functor.We get an equivalence because by choosing a different pole â we get equivalent objects.
It is worth observing that the above equivalence maps irreducible covariant 1-cocycles into irreducible covariant morphisms.Here, irreducibility is intended in the sense of C *categories (whilst the global C*-algebra is assumed to be only factorial).

Tensor structure
We now focus on Z 1 c (A K ), and prove that it is a tensor C * -category.To this end, given two covariant 1-cocycles X and Y we define and for any t ∈ (X, Y ) and s ∈ (Z, L) we set where ρ is the morphism defined by X .
Proof.We use the same notation as definitions (3.10) and (3.11).We note that As for intertwiners, where γ is the localized and transportable morphism associated with Z .This proves that t ⊗ s ∈ (X ⊗ Z, Y ⊗ L).We omit the proof of the rest of the properties of tensor product because follows by standard calculations.

Permutation symmetry
We now prove that the category of covariant 1-cocycles is a symmetric tensor C * -category, in other words we prove the existence of a permutation symmetry.To this end, the first step is to extend the tensor product.Given two 1-simplex b 1 and b 2 we define This definition, in the case of Roberts cocycles, admits an extension to pairs of paths.Given p, q having the same length, We observe that if the paths had different length we may modify the shorter one by inserting degenerate 1-simplices.Since a Roberts cocycle equals the identity on degenerate 1-simplices one can easily prove that the above definition is independent of where these degenerate 1-simplices are inserted.So we can always assume that in the above definition the paths have the same length.We now prove three lemmas necessary to the proof of the existence of the permutation symmetry.
Lemma 3.11.Given two covariant 1-cocycles X and Y and two paths p and q .For any pair of paths p, q homotopy equivalent to p and q respectively, the following relation holds Proof.As homotopy equivalent paths are obtained one each other by a finite number of elementary deformations (see Section 2.1), it is enough to prove the assertion for an elementary deformation.Let p = b and q = ∂ 1 c is the 1-face of a 2-simplex c.So where we used the fact that X σ 0 (∂ 1 c) = 1.
Lemma 3.12.Let p, q be two paths such that Proof.First of all we prove that we can find to paths p In fact by K4, there is o ⊂ ∂ 1 p and a ∈ K such that a ⊥ o, ∂ 0 p.Then we define b 1 := (o, ∂ 1 p; ∂ 1 p) and as d 1 the degenerate 1-simplex σ 0 (∂ 1 q).Since and the causal complement of the elements of K is pathwise connected K6 the proof, from this point, is the same as the proof [29][ Lemma 23.6] given by Roberts.As p ∼ p and q ∼ q , by K7, we have where γ denotes the morphism associated with Y . Proof.
We now observe that where we used the identity Note that the above identity is equivalent to We are ready to prove the existence of a permutation symmetry.Given X, Y two covariant 1-cocycles define where p, q are two paths with We first prove that this definition is independent of the choice of paths.Let p 1 and q 1 be two paths satisfying the same properties as p and q .Clearly p ∼ p * p 1 * p 1 and q ∼ q * q 1 * q 1 .By Lemma 3.11 we have Since (X × Y ) p * p 1 ,q * q 1 = (Y × X) q * q 1 ,p * p 1 because of Lemma 3.12, we get showing the independence of the choice of paths.
Proof.Given a 1-simplex b, according to the definition of intertwiner 3.4, and since ǫ does not depend on the choice of paths, for each λ ∈ P , we take two paths of the form λp, λq , where p, q are paths paths satisfying the properties of the definition (3.15) with respect to ∂ 0 b.It is evident that λp, λq satisfy the properties of the definition (3.15) with respect to λ∂ 0 b.Then applying the Lemma 3.13 once, we have Applying Lemma 3.13 iteratively, gives where being . Now, by iteratively applying to the left-hand product the equation (3.14), which is nothing but the Lemma (3.13), we arrive at ,q * b because ǫ does not depends on the choice of paths.The proof that for any t ∈ (X, X) and s ∈ (Y, Ỹ ) follows by a similar reasoning.We omit the rest of the properties of permutation symmetry since they follow by standard calculations.

Statistics and conjugation
In this section we select the subcategory of covariant 1-cocycles having finite statistics and prove that any object of this category has conjugates in the sense of symmetric tensor C * -categories.In our context, the conjugate of a covariant 1-cocycle X is a covariant 1-cocycle X for which there exists a pair of arrows r ∈ (I, X ⊗ X) and r ∈ (I, X ⊗ X) that satisfy the conjugate equations The key result is that simple covariant 1-cocycles, i.e. those obeying Fermi or Bose statistics, have conjugates.This will allows us to identify the subcategory of objects having finite statistics and to prove the existence of conjugates.
Definition 3.15.A covariant 1-cocycle X is said to be simple whenever We shall see at the end of this section that simple covariant 1-cocycles obey either Bose or Fermi statistics, depending on whether the value of χ(X) is 1 or −1.
We now draw on a consequence of this relation.According to the definition of permutation symmetry (3.15), for any pair o ⊥ õ we take a path p o,õ : o → õ and as q the degenerate 1-simplex σ 0 (o) = (o, o; o) and observe that Changing the role, in this relation, of o and õ and passing to the adjoint we arrive Since by K4 there is a ⊥ o, õ, we can assume that p o,õ is in the causal complement of a.So (3.18) reduces to Now our aim is to prove that any simple covariant 1-cocycle admits a conjugate covariant 1-cocycle.Here, because of the fact that morphisms associated to 1-cocycles are defined locally, we have to follows a different route with respect to the usual one (see [19,20,32]).We first prove that the Roberts 1-cocycle defined by a covariant cocycle has a conjugate.Then we prove that the morphism associated with this conjugate 1-cocycle inverts the morphism defined by the cocycle X .This, finally, will allow us to define the conjugate of a covariant 1-cocycle.
Lemma 3.16.Let X be a simple covariant 1-cocycle.For any 1-simplex b the definition is independent of the choice of a and defines a Roberts 1-cocycle.
= ρ(ã) |dn| (X dn ) So by iterating this idea to all the 1-simplices of the path we arrive to We now prove that X is a Roberts 1-cocycle.First of all observe that Xb ∈ A |b| .In fact for any ã ⊥ |b| we may take a ⊥ ã, |b| and the paths p Since X is a Roberts 1-cocycle, it defines by (3.6) a morphism ρ of the net A K .
Lemma 3.17.Let X be a simple covariant 1-cocycle.Let ρ be the morphism of the net associated with X by (3.6).Then Proof.We need a preliminary result.Let p : o → õ be a path which lays in the causal complement of a, then Xp = X p a,õ X po,a In fact if p = b n * • • • * b 1 , using the independence of the choice of a proved in the previous Lemma we have where we used the fact that ∂ 1 b i = ∂ 0 b i−1 and the fact that Roberts 1-cocycle equals 1 when evaluated on loops.Now we take õ ∈ K with o ⊆ õ and a ⊥ õ.Then we consider â ⊥ a ∪ õ and a path p â,a in the causal complement of õ.Then for any where we have used the fact that p a,â is in the causal complement of õ and ρ(o) õ(A) ∈ A(õ).Conversely We now are ready to prove the existence of the conjugate of simple and covariant 1-cocycles.Theorem 3.18.Given a simple covariant 1-cocycle X then is the conjugate covariant 1-cocycle of X .In particular X and X are irreducible.
Proof.By Lemma 3.5 ii) we have that Xb (λ) ∈ A(|b|) for any λ ∈ P .For any 2-simplex c and any λ, σ ∈ P we have So X is a covariant 1-cocycle.Concerning the conjugate equations, given b take a ⊥ |b| and and similarly ( X ⊗ X) b (λ) = 1 H .So both X ⊗ X and X ⊗ X are equal to the identity cocycle I and the conjugate equations (3.16) are verified by taking r and r equal to 1 I = 1 H . Finally in order to prove that X is irreducible, let t ∈ (X, X).By (3.17) and by the definition of tensor product we have 1 because, as observed above, ( X ⊗ X) b = 1 H for any 1-simplex b.Since K is pathwise connected t is a constant field and causality implies that t is a multiple of the identity, completing the proof.
We now introduce the notion of objects with finite statistics.To this end we recall that a left inverse of X is a linear map φ Z,Y : (X ⊗ Z, X ⊗ Y ) → (Z, Y ) satisfying the relations for any t ∈ (X ⊗ Z, X ⊗ Y ), s ∈ (Z, Z ′ ) and r ∈ (Y, Y ′ ).A left inverse of X is said to be positive whenever, for any object Y , φ Y,Y sends positive elements of (X ⊗ Y, X ⊗ Y ) into positive elements of (Y, Y ); normalized whenever φ I,I (1 X ) = 1 I where I is the identity object of the category.A positive normalized left inverse φ of X is said to be standard whenever (φ X,X (ǫ(X, X))) 2 = c • 1 X with c > 0. Definition 3.19.A covariant 1-cocycle X is said to have finite statistics if it admits a standard left inverse.The full subcategory of Z 1 c (A K ) of objects having finite statistics is denoted by Z 1 c,f (A K ).
We note that any simple covariant 1-cocycle X has finite statistics.Since X ⊗ X = X ⊗ X = I and r = r = 1 I , defining φ Z,Y (t) := 1 X ⊗ t , t ∈ (X ⊗ Z, X ⊗ Y ) , we get a positive, normalized left inverse which is, by definition of simple objects, standard.
In particular, we note that φ Z,Y (t) a = ρ(a) a (t a ) for any a ∈ Σ 0 (K).
Proposition 3.20.The category Z 1 c,f (A K ) is a symmetric tensor C * -category closed under tensor products, subobjects and direct sums.Any object of Z 1 c,f (A K ) is a finite direct sum of irreducible objects.
Proof.The proof follows from the properties of standard left inverses, see [19,29].
If X is an irreducible covariant 1-cocycle with finite statistics, following [19], and φ is a left inverse of X , one has that φ X,X (ǫ(X, X)) = χ(X) d(X) where χ(X) ∈ {−1, 1} and d(X) ∈ N, called, respectively, the statistical phase and dimension are invariant of the equivalence class of X .These invariants means that X has a para-statics of order d(X) of Bose or Fermi type depending on whether χ(X) is 1 or −1.
Note in particular that simple covariant 1-cocycle follows ordinary Bose or Fermi statistics.
Having shown that simple covariant 1-cocycles have finite statistics and have conjugates Lemma 3.6, we now are ready to give the main result of the present paper.Proof.The fact that Z 1 c,f (A K ) has conjugates derives from the fact that simple objects have conjugates (see the appendix of [32]).

Conclusions and outlooks
In the current study, we have introduced physically motivated properties that define appropriate families (sets of indices) of spacetime regions where quantum charges are expected to be localized.Then, given such a set of indices and an observable net fulfilling factoriality and relative Haag duality, we constructed a covariant superselection structure wherein charges are localized within the aforementioned regions.This achievement was made possible by employing a novel approach based on covariant 1-cocycles.We emphasize that the definitions and proofs given in this paper do not rely on the symmetry being a group, but rather on its semigroup structure.Therefore, our approach remains valid even when the symmetry of the charge localization regions is a semigroup.
Our method allows to recover the sectors of the DHR and BF analysis and, in curved spacetimes, the sectors of DHR type encoded by the cohomology of the observable net.Yet, in the case where the ambient spacetime is the light cone and the set of indices is the one of hypercones, it remains an open problem to understand the relation between our superselection structure and the one defined by Buchholz and Roberts for charges of electromagnetic type.We believe that this question is of interest because, were the two superselection structures inequivalent, we would be led to conclude that picking the set of indices does not uniquely determine the superselection structure with that localization.In other words, besides the choice of the localization regions, a further input is needed to discriminate the superselection structure of interest among those having the same localization.
Another open point is relative to our hypothesis that the ambient spacetime is simply connected.This simplified our exposition and it made possible to rule out Aharonov-Bohm external potentials to which at the present stage we are not interested.Yet, we wish to discuss our superselection sectors in full generality, with the final goal to arrive to the reconstruction of the field net without limitations on the topology of the spacetime.In this sense the localized morphisms constructed in §3.3 should play an important role, analogous to the one played by DHR endomorphisms in Minkowski spacetime.But, in a spacetime with non-trivial fundamental group, one has to take into account the fact that localized morphisms exhibit a non-trivial parallel transport, depending on the homotopy class of the path along which they are translated.
Finally, we would like to mention that, thanks to the level of abstraction that we adopted, our methods can be applied to low dimensional spacetimes, with the natural modifications arising from the fact that permutation symmetry could be replaced by a braiding in specific situations.We may therefore apply our suitably modified construction in such scenarios.At this purpose, we note that models studied in the language adopted in the present paper are available [13], thus they constitute candidates for further examples of superselection structures that can be obtained with our method.

A 1 -
simplex is given by a triple b of 0-simplices ∂ 0 b, ∂ 1 b ⊆ |b|; we call |b| the support and ∂ 0 b, ∂ 1 b the faces.Given the 1-simplex b, the reverse b is the 1-simplex having the same support as b and such that ∂ 0b = ∂ 1 b, ∂ 1 b = ∂ 0 b.A 1-simplex b is said to be degenerate whenever ∂ 1 b = ∂ 0 b.In particular, we denote the degenerate 1-simplex whose faces and support equal o ∈ Σ 0 (K) by σ 0 (o).Inductively, for n ≥ 1, an n-simplex x is formed by n + 1, (n − 1)-simplices ∂ 0 x, . . ., ∂ n x and by an element of the poset |x|, the support of x, such that |∂ i x| ⊆ |x| for i = 0, . . ., n; on the other hand, any (n − 1)-simplex the proper inclusion o ⊂ a amounts to the inclusion of the closure cl(o) of o in a; • the causal disjontness relation o ⊥ a amounts to J(cl(o)) ∩ cl(a) = ∅ where J(cl(o)) denotes the causal set of cl(o); [8].Here M the 4-dimensional Minkowski spacetime, K the set of spacelike cones, P the Poincaré group, and A K is defined in the vacuum representation.It is worth observing that being spacelike cones unbounded regions of M, one first consider the observable net over double cones defined in the vacuum representation.Then the von Neumann algebra associated with a spacelike cone o is defined as the von Neumann algebra generated by the algebras A(O) associated with double cones O such that O ⊂ o.
and X * b = Xb , for any 1-simplex b, where b is the reverse of b.

Definition 3 . 8 .
The set of the intertwiners t ∈ (ρ, γ) between two localized, transportable and covariant morphisms ρ and γ is the set of fields t :K ∋ o → t o ∈ A(o) such that • t o ρ(o) a = γ(o) a to for any o and a; • t o U ρ o (λ) = U γ o (λ)t o for any o and λ ∈ P .

Proof.
So let us start by showing the independence of the choice of a.So take ã ⊥ b.We first assume that ã ⊥ a.So we may take a path p a,ã = d m * • • • * d 1 in the causal complement of b and in the causal complement of |b|.Clearly ∂ 1 b 1 = a and ∂ 0 b n = ã.Since the support of b 1 is spacelike separated from the support of b there is, by K4, o ⊥ (|b 1 | ∪ |b|).Note in particular that o ⊥ a, ∂ 0 b 1 .So applying the above argument first with respect to o and a and then with respect to o and ∂ 0 b 1 arrive to and the proof follows by relative Haag duality.Secondly given a 2-symplex c take a ⊥ |c| we have

Theorem 3 . 21 .
The category of covariant 1-cocycles with finite statistics Z 1 c,f (A K ) has conjugates.
for any λ ∈ P .Note that the unitaries {v ρ o,õ } are nothing but Roberts 1-cocycles.By the localization of morphisms and relative Haag duality it follows that v ρ o,õ ∈ A(a) for any a with o, õ ⊆ a.Hence, Lemmas 3.5 and 3.6 say that any covariant 1-cocycle defines a localized, transportable and covariant morphism.Remark 3.2.Localizable and transportable morphisms ρ(o) : A K → A(K) ⊆ B(H) are representations of A K on H in the sense of 1 X and this implies that ρ(o) o (t o ) = t o for any o ∈ K .So by Lemma 3.17 we also have ρ(o) o (t o ) = (ρ(o) o • ρ(o) o )(t o ) = t ofor any o ∈ K .Hence for any 1-simplex b we have