Abstract
Rindler wedges are fundamental localization regions in AQFT. They are determined by the oneparameter group of boost symmetries fixing the wedge. The algebraic canonical construction of the free field provided by Brunetti–Guido–Longo (BGL) arises from the wedgeboost identification, the BW property and the PCT Theorem. In this paper we generalize this picture in the following way. Firstly, given a \(\mathbb Z_2\)graded Lie group we define a (twisted)local poset of abstract wedge regions. We classify (semisimple) Lie algebras supporting abstract wedges and study special wedge configurations. This allows us to exhibit an analog of the Haag–Kastler oneparticle net axioms for such general Lie groups without referring to any specific spacetime. This set of axioms supports a first quantization net obtained by generalizing the BGL construction. The construction is possible for a large family of Lie groups and provides several new models. We further comment on orthogonal wedges and extension of symmetries.
Introduction
Quantum Field Theory (QFT) lives in a tension between the locality principle and the underlying group of symmetries characterizing the theory. On one hand, it is a physical principle that every interesting quantity of a theory should be deducible by local measurements, namely—in the language of Algebraic Quantum Field Theory (AQFT)—by the structure of the local algebras (see e.g. [Ha96]). On the other hand, the symmetries of a theory provide a feature to describe physical objects, a “key to nature’s secrets,” as it happens in the standard model [We05, We11].
In AQFT, models are specified by a net of von Neumann algebras associated to causally complete spacetime regions satisfying fundamental quantum and relativistic principles, such as isotony, locality, covariance, positivity of the energy, and existence of a vacuum state. An important bridge between the geometry and the algebraic structure is the Bisognano–Wichmann (BW) property of (A)QFT claiming that the modular group of the algebra associated to any Rindler wedge W inside Minkowski spacetime with respect to the vacuum state implements unitarily the covariant oneparameter group of boosts fixing the wedge W. As a consequence, the algebraic structure of the model, through the Tomita–Takesaki theory, contains the information about the symmetry group acting on the model. Starting with the BW property, one can enlarge the symmetry group of a QFT [GLW98, MT18], find new relations among field theories [GLW98, LMPR19, MR20], establish proper relations among spin and statistics [GL95], and compute entropy in QFT [LX18, Wi18]. For recent results on this property we refer to [Gu19, DM20].
Particles are fieldderived concepts that can be described as unitary positive energy representations of the symmetry group. They are building blocks to construct Quantum Field Theories. The operatorvalued distribution \(\Phi _U\) defining the free field associated to any particle U is not provided by a canonical construction, see e.g. [BGL02, LMR16]. On the other hand, the von Neumann algebra net generated by \(\Phi _U\) satisfies the Bisognano–Wichmann property and the PCT Theorem.^{Footnote 1} These properties provide the tools for a canonical construction of the free algebra net [BGL02]: Segal’s second quantization gives the vacuum representation of the Weyl algebra on the Fock space associated with the oneparticle Hilbert space. The Araki lattice of von Neumann algebras is uniquely determined by the local oneparticle structure encoded in the lattice of closed real subspaces, the first quantization [Ar63]. As a result of the Tomita–Takesaki modular theory for real subspaces, the set of real states for a particle U localized in a wedge region is uniquely determined by the couple \((e^{2\pi K_W}, U(j_W))\) where \(U(j_W)\) is the antiunitary implementation of the wedge reflection and \(K_W\) is the generator of the oneparameter group of boosts associated to the wedge W. They satisfy the Tomita relation \(U(j_W) e^{2\pi K_W}U(j_W)= e^{2\pi K_W}\). The oneparticle states and the local algebra associated to bounded causally complete regions are obtained by wedge state spaces and algebra intersection, respectively.
Conversely, every pair \((x,\sigma )\), consisting of an element x of the Poincaré–Lie algebra and an involution \(\sigma \) satisfying \({\mathrm{Ad}}(\sigma )x = x\) specifies for every (anti)unitary representation \((U,\mathcal{H })\) of the Poincaré group a pair \((\Delta , J) = (e^{2\pi i \partial U(x)}, U(\sigma ))\) that in turn defines a standard subspace \(\mathtt{V}\subseteq \mathcal{H }\). This construction, called the BGL construction, was introduced in [BGL02] and allows us to observe: The algebraic construction of the free fields is uniquely determined by its symmetries and the correspondence between spacetime regions and their relative position with symmetries. In this sense, due to the onetoone correspondence between boosts and the corresponding wedges, one should be able to specify the underlying symmetry structure of a quantum field theory without any reference to the spacetime. Then one can reconstruct the spacetime features, such as locality and region inclusions from the symmetry group.
With this claim in mind, we generalize the above picture as follows. Given a suitable Lie group G, we first define an abstract wedge space. We then endow the wedge space with a Gaction, a notion of causal complement and an order structure. Eventually, starting from an (anti)unitary representation of a graded Lie group G, we construct the analogue of the BGL oneparticle net by the abstract setting.
We now collect the motivation and additional explanations of the fundamental structure we will use. In order to obtain a oneparticle net by the Tomita–Takesaki theory we need to start with a graded Lie group \(G=G^{{\uparrow }}\rtimes \mathbb{Z }_2\), such as the improper Möbius group \({\mathrm{PGL}}_2(\mathbb{R })\) or the proper Poincaré group \(\mathcal{P }_+\). For the moment, we assume that \(Z(G^{{\uparrow }})=\{e\}\) and that \(G^{{\uparrow }}\) is connected.
The key features of our approach are the following:
\(\bullet \) Abstract boost generator. The abstract oneparameter group of boosts are generated by elements x in the Lie algebra \(\mathfrak{g }\) of G defining a three grading \(\mathfrak{g }=\mathfrak{g }_1 \oplus \mathfrak{g }_0 \oplus \mathfrak{g }_{1}\) in the adjoint representation by \(\mathfrak{g }_j = \ker ({\mathrm{ad}}x  j {\mathrm{id}}_\mathfrak{g })\). To see how this complies with the well known models, see Examples 2.10. We call such elements \(x\in \mathfrak{g }\) Euler elements because they corresponds to the linear Euler vector field on the open embedding \(\mathfrak{g }_1 \hookrightarrow G/\mathbf{P}, s \mapsto \exp (s) \mathbf{P}\), where \(\mathbf{P} \subseteq G\) is the connected subgroup corresponding to the Lie algebra \(\mathfrak{g }_0 + \mathfrak{g }_{1}\). For more on the underlying geometry of theses spaces, we refer to [BN04].
\(\bullet \) The wedge reflection is obtained by analytic continuation of the oneparameter group of boosts associated to the wedge at \(i\pi \). For instance, on Minkowski space, the wedge reflection \(j_1=\Lambda _1(i\pi )\) is obtained by analytic extension of the oneparameter group of boosts in the first direction \(\Lambda _1(t)=\exp (t\sigma _1)\) where \((\sigma _i)_{i=1,2,3}\) are the Pauli matrices. In our general setting, the reflection \(\sigma \), called Euler involution, associated to an Euler element x is determined by the analytic continuation of the oneparameter group in the adjoint representation of the Lie algebra via \({\mathrm{Ad}}(\sigma )=e^{\pi i {\mathrm{ad}}x}\) (see (2.10)).
\(\bullet \) Euler wedge. An Euler wedge is defined as a couple \(W=(x_W, \sigma _W)\) of an Euler element and the related Euler involution. The need to use the couple is to implement the Gaction on the wedge space (see (2.6)) and to establish the relation with the standard subspaces \(\mathtt{V}\) and the corresponding modular objects \((\Delta _\mathtt{V}, J_\mathtt{V})\). We further remark that, in principle, it is not necessary to assume that the involution \(\sigma _W\) satisfies
in the adjoint representation, but only that it satisfies the proper commutation relation \({\mathrm{Ad}}(\sigma _W) x_W = x_W\), cf. Proposition 2.1.
\(\bullet \) \(G^\uparrow \)covariance. There is an action of the group G on the wedge space given by an adjoint action on both components that takes care of the grading (see (2.8)). In this way the language of Euler wedges is consistent with the one of the standard subspaces, cf. Sect. 2.
\(\bullet \) Locality. Complementary wedges correspond to inverted oneparameter groups of boosts. For instance dilations associated to causally complementary intervals in chiral theory or boosts associated to complementary wedges are inverse to each other. On the abstract wedge space this is captured by defining the complementary wedge of \(W=(x,\sigma )\) by \(W'=(x, \sigma )\).
\(\bullet \) Isotony. By the existence of a (positive) invariant cone C in the Lie algebra \(\mathfrak{g }\), it is possible to define a wedge endomorphism semigroup defining the wedge inclusion relation. Given an Euler wedge \(W=(x,\sigma )\), the generators in the positive cone lying in the subspaces \(\mathfrak{g }_{\pm 1}\) define proper wedge inclusions as each of them generates with x a translationdilation group (isomorphic to the affine group of the real line); see [Bo92, Wi92, Wi93] and in particular [Bo00]. This is the case of wedge endomorphisms in Minkowski spacetime given by lightlike shifting or Möbius transformations mapping an interval into itself as the translations do for the halflines. These properties define a local partially ordered set of wedges that can support key features of an AQFT structure.
It is important to note that the wedge space only depends on the Lie group and its Lie algebra, and the order structure given by the invariant cone \(C \subseteq \mathfrak{g }\). The relations among the wedges specify the abstract spacetime structure to a large extent. For example, \({\mathrm{PSL}}_2(\mathbb{R })\) is the symmetry group for the 2dimensional de Sitter spacetime and for the chiral circle. If one considers \({\mathrm{PSL}}_2(\mathbb{R })\) with the trivial cone in \({\mathfrak{sl }}_2(\mathbb{R })\)—no proper inclusions of wedges—then it describes a QFT on de Sitter spacetime; if one considers \(C\subset {\mathfrak{sl }}_2(\mathbb{R })\) as in (2.17), inclusion relations among wedges arise, and we obtain the wedge space on \(\mathbb{S }^1\).^{Footnote 2} This correspondence between isotony and and positivity of the energy was also studied in [GL03]; see also [Bo92, Bo00, Wi92, Wi93] and [NÓ17, Ne19, Ne19b]. For recent classification results for the triples \((\mathfrak{g },x,C)\), we refer to [Oeh20, Oeh21].
There is more interesting structure on the abstract wedge space:
\(\bullet \) Orthogonal wedges: We call two abstract wedges \(W_1 = (x_1, \sigma _1)\) and \(W_2 = (x_2,\sigma _2)\) orthogonal if \(\sigma _1(x_2)=x_2\), i.e., \(W_2\) is reflected into its complement \(W_2'\). Examples of orthogonal wedges are coordinate wedges on Minkowski spacetime,^{Footnote 3} or the upper and the right halfcircle in chiral theories on \(\mathbb{S }^1\). This notion, which immediately generalizes to the abstract setting, plays a central role in spinstatistics relations [GL95] and the nuclearity property in conformal field theory [BDL07].
\(\bullet \) Symmetric wedges. A wedge W is called symmetric if there exists \(g\in G^{{\uparrow }}\), such that \(g.W=~W'\). For instance, any couple of wedge regions, in \(1+s\)dimensional Minkowski spacetime with \(s\ge 2\), are transformed one into the other by the action of the Poincaré group \(G^{{\uparrow }}=\mathcal{P }_+^\uparrow \). On the other hand, in \(1+1\)dimensional Minkowski space, the right and the left wedges are not symmetric. Indeed
belong to disjoint transitive families with respect to the \(\mathcal{P }_+^\uparrow \)action. Further examples of symmetric wedges are intervals in conformal theories on the circle. Halflines in the real line are not symmetric wedges with respect to the translationdilation group. A transitive family of wedges has the feature that algebras associated to complementary wedges are  by covariance  unitary equivalent. On the other side, there is no contradiction in having a \(G^{{\uparrow }}\)covariant net of von Neumann algebras on a transitive family of nonsymmetric wedges with trivial algebras associated to the family of complements.
In the first part of the paper we define and investigate the abstract structure we have described. When the center \(Z(G^{{\uparrow }})\) is non trivial, for instance when covering groups are considered, a generalized notion of complementary wedges has to be introduced. Indeed, while Euler elements are uniquely determined as generators of oneparameter groups in \(G^{{\uparrow }}\), several involutions \(\sigma \) satisfying \({\mathrm{Ad}}(\sigma )=e^{\pi i {\mathrm{ad}}x}\) can be associated to the same Euler element x. In an analogous way, different wedge complements can be labeled by central elements. We classify wedge orbits and define a notion of a central wedge complement. Furthermore, if \(W'\) does not belong to the \(G^{{\uparrow }}\)orbit of W, a new action of G on the wedge space is defined. This happens for instance in fermionic nets.
Having specified the abstract structures, we are prepared to answer the following question:
“Which Lie algebras/groups support such a structure?” To this end, we first classify Euler elements in real simple Lie algebras in Theorem 3.10. The key point of this classification is that Euler elements are conjugate under inner automorphisms to elements in any given Cartan subspace of hyperbolic elements. Here the restriction to simple Lie algebras is not restrictive because any symmetric Euler element is contained in a semisimple Lie subalgebra. Furthermore, an Euler element is symmetric if and only if it is contained in an \({\mathfrak{sl }}_2(\mathbb{R })\)subalgebra (see Theorem 3.13 for these results). As a consequence, there is a large family of real Lie algebras supporting such wedge structures which properly contains the well known models. Note that, for a Lie algebra \(\mathfrak{g }\) containing an Euler element \(x \in \mathfrak{g }\), there always exists a graded Lie group G with Lie algebra \(\mathfrak{g }\) and a corresponding Euler wedge \((x,\sigma )\).
The second part of the paper is devoted to nets of standard subspaces.
Is it possible to construct oneparticle models supporting this abstract setting? Starting with a \(G^{\uparrow }\)orbit \(\mathcal{W }_+\) in the wedge space, we describe a set of axioms which, for the well known models, reflect fundamental quantum and relativistic principles corresponding to the oneparticle Haag–Kastler axioms. This set of axioms is fulfilled by extending the BGL construction to every graded Lie group G, supporting a suitable wedge space. A twisted locality relation among complementary wedges is introduced in order to relate central complementary wedges.
Do we get any new models out of this general construction? The answer is affirmative. All the simple Lie algebras whose restricted root system appears in Theorem 3.10 correspond to a graded Lie group with a nontrivial wedge space. There are for instance Lie algebras of type \(E_7\) that do not correspond to any known models. In this context the Jordan spacetimes of Günaydin [Gu93, Gu00, Gu01] and the simple spacetime manifolds in the sense of Mack–de Riese [MdR07] are homogeneous spaces of simple hermitian Lie groups whose Lie algebras contain Euler elements, and the corresponding abstract wedges correspond to domains in these causal manifolds. These Lie groups have many (anti)unitary representations, some of them with positive energy with respect to a nontrivial invariant cone C in the Lie algebra. As a consequence, they support many oneparticle nets [NÓ20] and second quantization models of von Neumann algebras whose physical meaning has to be investigated.
The structure of this paper is as follows: In Sect. 2 the wedge space is defined and its properties are studied. A number of examples are discussed in detail to show how the abstract setting applies to the known models and realizes the well known structure. In Sect. 3 we study the Euler elements in Lie algebras. We relate orthogonal and symmetric wedges and provide a classification of Lie algebras supporting (symmetric) Euler elements. In Sect. 4 we apply this structure to define and construct oneparticle nets associated to graded Lie groups supporting a wedge structure. We further stress new models, orthogonal wedges and extension of symmetries. An outlook on the construction is contained in Sect. 5. We hope this paper is approachable for the Lie Theory community as well as the Algebraic Quantum Field Theory community.
The Abstract Setting
In this section we develop an abstract perspective on wedge domains in spacetimes, phrased completely in group theoretic terms. As wedge domains are supposed to correspond to standard subspaces in Hilbert spaces, we orient our approach on how standard subspaces are parametrized.
Let \({\mathrm{Stand}}(\mathcal{H })\) denote the set of standard subspaces of the complex Hilbert space \(\mathcal{H }\). In Sect. 4 we shall see that every standard subspace \(\mathtt{V}\) determines a pair \((\Delta _\mathtt{V}, J_\mathtt{V})\) of modular objects and that \(\mathtt{V}\) can be recovered from this pair by \(\mathtt{V}= {\mathrm{Fix}}(J_\mathtt{V}\Delta _\mathtt{V}^{1/2})\). This observation can be used to obtain a representation theoretic parametrization of \({\mathrm{Stand}}(\mathcal{H })\): each standard subspace \(\mathtt{V}\) specifies a continuous homomorphism
We thus obtain a bijection between \({\mathrm{Stand}}(\mathcal{H })\) and the set \({\mathrm{Hom}}_{\mathrm{gr}}(\mathbb{R }^\times , {\mathrm{AU}}(\mathcal{H }))\) of continuous morphisms of graded topological groups.
The space \({\mathrm{Stand}}(\mathcal{H })\) carries three important features:

an order structure, defined by set inclusion

a duality operation \(\mathtt{V}\mapsto \mathtt{V}' = \{ \xi \in \mathcal{H }:(\forall v \in \mathtt{V})\, {\mathrm{Im}}\langle \xi , v \rangle = 0\}\)

the action of \({\mathrm{AU}}(\mathcal{H })\) as a symmetry group.
The order structure is hard to express in terms of the modular groups (see [Ne19b] for some first steps in this direction), but the duality operation corresponds to inversion
and the action of \({\mathrm{AU}}(\mathcal{H })\) translates into
where \(\varepsilon (g) = 1\) if g is unitary and \(\varepsilon (g) = 1\) otherwise. So unitary operators \(g \in \mathrm{U{}}(\mathcal{H })\) simply act by conjugation, but antiunitary operators also involve inversion. In particular, \(J_\mathtt{V}\mathtt{V}= \mathtt{V}'\) corresponds to
We now develop the corresponding structures by replacing \({\mathrm{AU}}(\mathcal{H })\) by a finite dimensional graded Lie group.
Group theoretical setting
The basic ingredient of our approach is a finite dimensional graded Lie group \((G,\varepsilon _G)\), i.e., G is a Lie group and \(\varepsilon _G :G \rightarrow \{\pm 1\}\) a continuous homomorphism. We write
so that \(G^{{\uparrow }}\trianglelefteq G\) is a normal subgroup of index 2 and \(G^{{\downarrow }}= G \setminus G^{{\uparrow }}\). We also fix a pointed closed convex cone \(C \subseteq \mathfrak{g }\) satisfying
As we shall see in the following, for graded Lie groups, it is more natural to work with the twisted adjoint action
so that (2.4) actually means that C is invariant under the twisted adjoint action. The cone C will play a role in specifying an order structure. It is related to positive spectrum conditions on the level of unitary representations. We also allow \(C=\{0\}\). For instance, the Lie algebra \(\mathfrak{g }= {\mathfrak{so }}_{1,d}(\mathbb{R })\) of the Lorentz group \(G = \mathrm{O{}}_{1,d}(\mathbb{R })\), the isometry group of de Sitter space time \({\mathrm{dS}}^d\), contains no nontrivial invariant cone.
The space \({\mathrm{Hom}}_{\mathrm{gr}}(\mathbb{R }^\times ,G)\) and abstract wedges
In this section we define the fundamental objects we will need in the forthcoming discussion. We write \({\mathrm{Hom}}_{\mathrm{gr}}(\mathbb{R }^\times ,G)\) for the space of continuous morphisms of graded Lie groups \(\mathbb{R }^\times \rightarrow G\), where \(\mathbb{R }^\times \) is endowed with its canonical grading by \(\varepsilon (r) := {\mathrm{sgn}}(r)\). On this space G acts by
where the twist is motivated by formula (2.2). Elements of \(G^{{\uparrow }}\) simply act by conjugation.
Since we are dealing with Lie groups, we also have the following simpler description of the space \({\mathrm{Hom}}_{\mathrm{gr}}(\mathbb{R }^\times ,G)\) by the set
Proposition 2.1
The map
is a bijection. It is equivariant with respect to the action of G on \(\mathcal{G }\) by
Note that center \(Z(G^{{\uparrow }})\) of \(G^{{\uparrow }}\) acts trivially on the Lie algebra but it may act nontrivially on involutions in \(G^{{\downarrow }}\).
Remark 2.2
For every involution \(\sigma \in G^{{\downarrow }}\), the involutive automorphism \(\sigma _G(g) := \sigma g \sigma \) defines the structure of a symmetric Lie group \((G^{{\uparrow }},\sigma _G)\), and \(G \cong G^{{\uparrow }}\rtimes \{{\mathrm{id}}, \sigma \}\), so that we can translate between G as a graded Lie group and the pair \((G^{{\uparrow }},\sigma _G)\), without loosing information.
To indicate the analogy of elements of \(\mathcal{G }\) with the wedge domains in QFT, we shall often denote the elements of \(\mathcal{G }\) by \(W = (x,\sigma )\).
Definition 2.3
(a) We assign to \(W = (x,\sigma ) \in \mathcal{G }\) the oneparameter group
Then we have the graded homomorphism
Note that \(\Psi (\gamma _W) = W\) in terms of (2.7).
Definition 2.4
(a) We call an element x of the finite dimensional real Lie algebra \(\mathfrak{g }\) an Euler element if \({\mathrm{ad}}x\) is diagonalizable with \({\mathrm{Spec}}({\mathrm{ad}}x) \subseteq \{1,0,1\}\), so that the eigenspace decomposition with respect to \({\mathrm{ad}}x\) defines a 3grading of \(\mathfrak{g }\):
(see [BN04] for more details on Euler elements in more general Lie algebras). Then \(\sigma _x(y_j) = (1)^j y_j\) for \(y_j \in \mathfrak{g }_j(x)\) defines an involutive automorphism of \(\mathfrak{g }\).
For an Euler element we write \(\mathcal{O }_x = {\mathrm{Inn}}(\mathfrak{g })x \subseteq \mathfrak{g }\) for the orbit of x under the group \({\mathrm{Inn}}(\mathfrak{g }) = \langle e^{{\mathrm{ad}}\mathfrak{g }} \rangle \) of inner automorphisms.^{Footnote 4} We say that x is symmetric if \(x \in \mathcal{O }_x\).
We write \(\mathcal{E }(\mathfrak{g })\) for the set of nonzero Euler elements in \(\mathfrak{g }\) and \(\mathcal{E }_{\mathrm{sym}}(\mathfrak{g }) \subseteq \mathcal{E }(\mathfrak{g })\) for the subset of symmetric Euler elements.
(b) An element \((x,\sigma ) \in \mathcal{G }\) is called an Euler couple or Euler wedge if
Then \(\sigma \) is called an Euler involution and \(\sigma =\sigma _x\) as introduced before. We write \(\mathcal{G }_E \subseteq \mathcal{G }\) for the subset of Euler couples and note that the relation \(e^{\pi i {\mathrm{ad}}x} = e^{\pi i {\mathrm{ad}}x}\) implies that the subset \(\mathcal{G }_E\) is invariant under the Gaction.
For an Euler element \(x \in \mathcal{E }(\mathfrak{g })\), the relation (2.10) only determines \(\sigma \) up to an element \(z \in G^{{\uparrow }}\cap \ker ({\mathrm{Ad}})\) for which \((\sigma z)^2 = e\), i.e., \(\sigma z \sigma = z^{1}\). Note that, if \(G^{{\uparrow }}\) is connected, then \(G^{{\uparrow }}\cap \ker ({\mathrm{Ad}}) = Z(G^{{\uparrow }})\) is the center of \(G^{{\uparrow }}\). The couples \((x,\sigma )\) that we have seen in the physics literature are all Euler couples (cf. [NÓ17, Ex. 5.15]). This ensures many properties, such as the proper relation between spin and statistics, see for instance [GL95].
Definition 2.5
(a) (Duality operation) For \(W = (x,\sigma ) \in \mathcal{G }\), we define \(W' := (x,\sigma )\). Under \(\Psi \), this operation corresponds to inverting the homomorphism \(\mathbb{R }^\times \rightarrow G\) pointwise. Note that \((W')' = W\) and \((gW)' = gW'\) for \(g \in G\) by (2.8).
(b) (Order structure on \(\mathcal{G }\)) We now define an order structure on \(\mathcal{G }\) that depends on the invariant cone C from (2.4). We associate to \(W = (x,\sigma ) \in \mathcal{G }\)

the Lie wedge
$$\begin{aligned} L_W := L(x,\sigma ) := C_+(W) \oplus \underbrace{(\mathfrak{g }^{\sigma }\cap \ker ({\mathrm{ad}}x))}_{\mathfrak{g }_W :=} \oplus C_(W), \end{aligned}$$where
$$\begin{aligned} C_\pm (W) = \pm C \cap \mathfrak{g }^{\sigma } \cap \ker ({\mathrm{ad}}x \mp \mathbf{1 }) \quad \text{ and } \quad \mathfrak{g }^{\pm \sigma } := \{ y \in \mathfrak{g }:{\mathrm{Ad}}(\sigma )(y) = \pm y \}. \end{aligned}$$ 
\(\mathfrak{g }(W) := L_W  L_W\), the Lie algebra generated by \(L_W\).

the semigroup associated to the triple \((C,x,\sigma )\):
$$\begin{aligned} \mathcal{S }_W := \exp (C_+(W)) G^{{\uparrow }}_{W} \exp (C_(W)) = G^{{\uparrow }}_{W} \exp \big (C_+(W) + C_(W)\big ),\end{aligned}$$where
$$\begin{aligned} G^{{\uparrow }}_{W} = \{g \in G^{{\uparrow }}:g.W = W \} = \{ g \in G^{{\uparrow }}:\sigma _G(g) = g, {\mathrm{Ad}}(g)x = x\} \end{aligned}$$is the stabilizer of \(W = (x,\sigma )\) in \(G^{{\uparrow }}\) (cf. [Ne19b, Thm. 3.4]).^{Footnote 5}

the subgroups \(G^{{\uparrow }}(W) := \langle \exp \mathfrak{g }(W) \rangle G^{{\uparrow }}_{W}\) and \(G(W) := G^{{\uparrow }}(W) \{e,{\sigma }\}\) with Lie algebra \(\mathfrak{g }(W)\).
As the unit group of \(\mathcal{S }_W\) is given by \(\mathcal{S }_W \cap \mathcal{S }_W^{1} = G^{{\uparrow }}_{W}\) ([Ne19b, Thm. III.4]), the semigroup \(\mathcal{S }_W\) defines a \(G^{{\uparrow }}\)invariant partial order on the orbit \(G^{{\uparrow }}.W \subseteq \mathcal{G }\) by
In particular, \(g.W \le W\) is equivalent to \(g \in \mathcal{S }_W\).
We have the following relations among these objects:
Lemma 2.6
For every \(W=(x_W,\sigma _W) \in \mathcal{G }\), \(g \in G\), and \(t \in \mathbb{R }\), the following assertions hold:

(i)
\(\lambda _W(t) W = W, \lambda _W(t) W' = W'\) and \(\sigma _W.W = W'.\)

(ii)
\(\sigma _{W'} = \sigma _W\) and \(\lambda _{W'}(t) = \lambda _W(t)\).

(iii)
\(\sigma _W\) commutes with \(\lambda _W(\mathbb{R })\).

(iv)
\(L_{W'} =  L_W\) and \(\mathcal{S }_{W'} = \mathcal{S }_W^{1}\).

(v)
\(C_\pm (g.W) = {\mathrm{Ad}}(g) C_{\pm \varepsilon _G(g)}(W)\), \(L_{g.W} = {\mathrm{Ad}}(g)L_W\), and \(\mathcal{S }_{g.W} = g \mathcal{S }_W g^{1}\).

(vi)
For \(W_1, W_2 \in \mathcal{G }\), the relation \(W_1 \le W_2\) in \(\mathcal{G }\) implies \(g.W_1 \le g.W_2\).
Proof
(i) For \(W = (x,\sigma )\in \mathcal{G }\), the first two relations follow from the fact that \(\exp (\mathbb{R }x)\) commutes with x and \(\sigma \). The second follows from \(\sigma _W. W = \sigma .(x,\sigma ) = ({\mathrm{Ad}}(\sigma ) x, \sigma ) = (x, \sigma ) = W'.\)
(ii) is clear from the definition of \(W'\).
(iii) follows from (i).
(iv) follows from \(C_\pm (W') =  C_{\mp }(W)\).
(v) The assertion is clear for \(g \in G^{{\uparrow }}\). For \(g \in G^{{\downarrow }}\), we have \(g\sigma \in G^{{\uparrow }}\), so that
This implies in particular that \(L_{g.W} = {\mathrm{Ad}}(g)L_W\). From \(G^{{\uparrow }}_{g.W} = g G^{{\uparrow }}_{W} g^{1}\), we thus obtain \(\mathcal{S }_{g.W} = g \mathcal{S }_W g^{1}\).
(vi) If \(W_1 \le W_2\), then \(W_1 = s.W_2\) for \(s \in \mathcal{S }_{W_2}\). Then \(g.W_1 = gs.W_2 = gsg^{1}.(g.W_2)\) with \(gsg^{1} \in g \mathcal{S }_{W_2} g^{1} = \mathcal{S }_{g.W_2}\) implies \(g.W_1 \le g.W_2\). \(\square \)
In this discussion we started with a Lie group. We remark that one can also start with a Lie algebra as follows: Consider a quadruple \((\mathfrak{g }, \sigma _\mathfrak{g }, h, C)\) of a Lie algebra \(\mathfrak{g }\), an involutive automorphism \(\sigma _\mathfrak{g }\) of \(\mathfrak{g }\), fixing the Euler element h and a pointed closed convex invariant cone \(C \subseteq \mathfrak{g }\) with \(\sigma _\mathfrak{g }(C) =  C\). Then \(\sigma _\mathfrak{g }\) integrates to an automorphism \(\sigma _G\) of the 1connected Lie group \(G^{{\uparrow }}\) with Lie algebra \(\mathfrak{g }\), so that we obtain all the data required above with \(G := G^{{\uparrow }}\rtimes \{{\mathrm{id}}_G,\sigma _G\}\).
For two such quadruples \((\mathfrak{g }_j, \tau _{\mathfrak{g },j}, h_j, C_j)_{j =1,2}\), a homomorphism \(\varphi :\mathfrak{g }_1 \rightarrow \mathfrak{g }_2\) of Lie algebras is compatible with this structure if
We thus obtain a category whose objects are the quadruples \((\mathfrak{g }, \tau _\mathfrak{g }, h, C)\) and its morphisms are the compatible homomorphisms.
A similar category can be defined on the group level, but there are some subtle ambiguities concerning the possible extensions of the group structure from \(G^{{\uparrow }}\) to G.
Remark 2.7
(Twisted extensions of \(G^{{\uparrow }}\) to G) We start with a graded group G for which \(G^{{\downarrow }}\) contains an involution \(\sigma \), so that \(G \cong G^{{{\uparrow }}} \rtimes \{e,\sigma \}\), where \(\sigma \) acts on \(G^{{\uparrow }}\) by the automorphism \(\sigma _G(g) := \sigma g \sigma \). This defines a split group extension
and we are now asking for other group extensions
for which the elements in \({\widehat{G}}^{{\downarrow }}\) define the same element in the group \({\mathrm{Out}}(G^{{\uparrow }}) = {\mathrm{Aut}}(G^{{\uparrow }})/{\mathrm{Inn}}(G^{{\uparrow }})\) of outer automorphisms of \(G^{{\uparrow }}\). These extensions are parametrized by the group
by assigning to \(z \in Z(G^{{\uparrow }})^+\) the group structure on \(G^{{\uparrow }}\times \{1,1\}\) given by
We write \({\widehat{G}}_z\) for the corresponding Lie group. Basically, this means that the element \({\widehat{\sigma }} := (e,1)\) has the same commutation relations with \(G^{{\uparrow }}\) but its square is z instead of e:
For two elements \(z,z' \in Z(G^{{\uparrow }})^+\), the corresponding extensions are equivalent if and only if
This follows from [HN12, Thm 18.1.13], combined with [HN12, Ex. 18.3.5(b)].
(a) For \(G = \mathrm{O{}}_{n}(\mathbb{R })\), \(n > 3\), and \(G^{{\uparrow }}= {\mathrm{SO}}_{n}(\mathbb{R })\), the situation depends on the parity of n. If n is odd, then \(Z(G^{{\uparrow }}) = \{e\}\) and no twists exist. If n is even, then \(Z(G^{{\uparrow }}) = \{\pm \mathbf{1 }\} = Z(G)\). Therefore \(Z(G^{{\uparrow }})^+ = \{ \pm \mathbf{1 }\} \not = B = \{e\}\). We therefore have one twisted group \({\widehat{G}} = {\mathrm{SO}}_n(\mathbb{R }) \{e,{\widehat{\sigma \}}}\), where \(\sigma \in \mathrm{O{}}_n(\mathbb{R })\) corresponds to a hyperplane reflection, and \({\widehat{\sigma }}^2 =  \mathbf{1 }\) in \({\widehat{G}}\).
(b) The same phenomenon occurs for Spin groups. Let \(G := {\mathrm{Pin}}_n(\mathbb{R }) \cong {\mathrm{Spin}}_n(\mathbb{R }) \rtimes \{e,\sigma \}\), where \(\sigma \) corresponds to a hyperplane reflection. If n is odd, then \(Z({\mathrm{Spin}}_n(\mathbb{R })) = \{ e,z\}\) contains two elements, and we have a twisted group
(cf. [HN12, Rem. B.3.25]). If n is even, then the situation is more complicated because the center of \({\mathrm{Spin}}_n(\mathbb{R })\) has order 4.
(c) For \(G = {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}} \rtimes \{e,\sigma \}\), where \(\sigma \) corresponds to a reflection \(\sigma (x) = x\) on \(\mathbb{R }^\infty \cong \mathbb{S }^1\), we have \(Z(G^{{\uparrow }}) \cong \mathbb{Z }\) and \(\sigma _G(z) = z^{1}\) for \(z \in Z(G^{{\uparrow }})\). Hence \(Z(G^{{\uparrow }})^+ = \{e\}\), so that there are no twists.
(d) If \(G = {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}^{(2n)} \rtimes \{e,\sigma \}\), where \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}^{(2n)}\) is the covering of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) of even order, then \(Z(G^{{\uparrow }}) \cong \mathbb{Z }_{2n}\) and \(\sigma _G(z) = z^{1}\) for \(z \in Z(G^{{\uparrow }})\). Therefore \(Z(G^{{\uparrow }})^+ = \{ e, \gamma \}\), where \(\gamma \) is the unique nontrivial involution in \(Z(G^{{\uparrow }})\) and \(B = \{e\}\). Hence there exists a nontrivial twist \({\widehat{G}} = G^{{\uparrow }}\{ e,{\widehat{\sigma \}}}\) with \({\widehat{\sigma }}^2 = \gamma \).
(e) As we shall see in Example 2.13 below, it may happen that, for the twisted groups \({\widehat{G}}_z\), the coset \({\widehat{G}}_z^{{\downarrow }}\) contains no involutions. In this example \(G^{{\uparrow }}= {\mathrm{SL}}_2(\mathbb{R })\) and \(G = G^{{\uparrow }}\{e,\gamma \}\) with \(\gamma ^2 =  \mathbf{1 }\).
In general, elements in \({\widehat{G}}_z^{{\downarrow }}\) are of the form \(g{\widehat{\sigma }}\) with \(g \in G^{{\uparrow }}\), and then
Hence \({\widehat{G}}_z^{{\downarrow }}\) contains an involution if and only if
If \(z = g \sigma _G(g)\) for some \(g \in G^{{\uparrow }}\), then conjugating with g implies that g and \(\sigma _G(g)\) commute.
The discussion in Example 2.13 shows that (2.15) is not satisfied for \(z = \mathbf{1 }\) and the Euler involution of \(G^{{\uparrow }}= {\mathrm{SL}}_2(\mathbb{R })\). For any odd degree covering \({\mathrm{SL}}_2(\mathbb{R })^{(2k+1)} \rightarrow {\mathrm{SL}}_2(\mathbb{R })\), the central involution is mapped onto \(\mathbf{1 }\), so that this observation carries over to odd coverings of \({\mathrm{SL}}_2(\mathbb{R })\).
The situation changes if we consider \(G^{{\uparrow }}= {\mathrm{SL}}_2(\mathbb{C })\) instead. Then \(g := i \begin{pmatrix} 1 &{} 0 \\ 0 &{} 1 \end{pmatrix}\) satisfies \(g^2 = \mathbf{1 }\), so that the group \({\widehat{G}} = G^{{\uparrow }}\{ \mathbf{1 },{\widehat{\sigma \}}}\) with \({\widehat{\sigma }}^2 =  \mathbf{1 }\) contains the nontrivial involution \(g{\widehat{\sigma }} \in {\widehat{G}}^{{\downarrow }}\). As this involution is central, \({\widehat{G}} \cong {\widehat{G}}^{{\uparrow }}\times \mathbb{Z }_2\) is a direct product.
The abstract wedge space, some fundamental examples
Definition 2.8
(The abstract wedge space). From here on, we always assume that \(\mathcal{G }\not =\emptyset \), i.e., that \(G^{{\downarrow }}\) contains an involution \(\sigma \). Then
(cf. Remark 2.2). For a fixed couple \(W_0 = (h,\sigma ) \in \mathcal{G }\), the orbits
are called the positive and the full wedge space containing \(W_0\).
Remark 2.9
(a) As \(\sigma .W_0 = (h,\sigma ) = W_0'\), we have \(\mathcal{W }(W_0) = \mathcal{W }_+(W_0) \cup \mathcal{W }_+(W_0')\), and \(\mathcal{W }(W_0)\) coincides with \(\mathcal{W }_+(W_0)\) if and only if \(W_0' = (h,\sigma ) \in \mathcal{W }_+(W_0)\). This is equivalent to the existence of an element \(g \in G^{{\uparrow }}\) with \(g.W_0 = W_0'\), i.e., \(g \in (G^{{\uparrow }})^\sigma \) with \({\mathrm{Ad}}(g)h =  h\).
(b) If \(W_0\) is an Euler couple, then \(\mathcal{W }(W_0)\) is a family of Euler couples, and we shall see below that in this case we have \(\mathcal{W }(W_0) = \mathcal{W }_+(W_0)\) in many important cases.
We collect some fundamental examples, starting from the low dimensional cases, that we shall refer to throughout the paper.
Examples 2.10
(a) The smallest example is the abelian group \(G = \mathbb{R }\times \{\pm 1 \}\), where \(G^{{\uparrow }}= \mathbb{R }\), \(C = \{0\}\) and \(L = \mathfrak{g }\). For \(W_0 = (h,\sigma )\) with \(h = 1\) and \(\sigma = (0,1)\), we then have the onepoint set \(\mathcal{W }_+ = \{ (h,\sigma )\}\), and \(\mathcal{W }= \{ (h,\sigma ), (h,\sigma )\}\).
(b) The affine group \(G :={\mathrm{Aff}}(\mathbb{R })\cong \mathbb{R }\rtimes \mathbb{R }^\times \) of the real line is twodimensional. Its elements are denoted (b, a), and they act by \((b,a)x = ax + b\) on the real line. The identity component \(G^{{\uparrow }}= \mathbb{R }\rtimes \mathbb{R }^\times _+\) acts by orientation preserving maps, and \(G^{{\downarrow }}\) consists of reflections \(r_p(x) = 2px\), \(p \in \mathbb{R }\).
Let \(\zeta (t) = (t,1)\) and \(\delta (t) = (0,e^t)\) be the translation and dilation oneparameter groups, respectively. We write \(\lambda = (0,1) \in \mathfrak{g }= \mathbb{R }\rtimes \mathbb{R }\) for the infinitesimal generator of \(\delta \), which is an Euler element. Therefore \(W := (\lambda , r_0)\) is an Euler couple.
The cone \(C = \mathbb{R }_+ \times \{0\} \subseteq \mathfrak{g }\) satisfies the invariance condition (2.4) and the corresponding semigroup \(\mathcal{S }_W\) is
Therefore the map
defines an order preserving bijection between the abstract wedge space \(\mathcal{W }_+(W) \subseteq \mathcal{G }\) and the set \(\mathcal{I }_+(\mathbb{R }) = \{ (t,\infty ) :t \in \mathbb{R }\}\) of lower bounded open intervals in \(\mathbb{R }\). Accordingly, we may write \(W_{(t,\infty )}=(\Lambda _{(t,\infty )},r_t) := \zeta (t) W = ({\mathrm{Ad}}(\zeta (t))\lambda , r_t)\) for \(t \in \mathbb{R }\). Acting with reflections, we also obtain the couples
corresponding to past pointing halflines \((\infty ,t)\subset \mathbb{R }\). We thus obtain a bijection between the full wedge space \(\mathcal{W }(W)\) and the set \(\mathcal{I }(\mathbb{R })\) of open semibounded intervals in \(\mathbb{R }\). We shall denote with \(\delta _I\) the oneparameter group of dilations with generator \(\lambda _I\) corresponding to the half line I.
The set \(\mathcal{E }(\mathfrak{g }) = {\mathrm{Ad}}(G^{{\uparrow }})\{\pm \lambda \}\) of nonzero Euler elements in \(\mathfrak{g }\) consists of two \(G^{{\uparrow }}\)orbits and, for each nonzero Euler element \(\pm {\mathrm{Ad}}(\zeta (t))\lambda \in \mathcal{E }(\mathfrak{g })\), the reflection \(r_t\) is the unique partner for which \((\pm {\mathrm{Ad}}(\zeta (t))\lambda , r_t) \in \mathcal{G }\). Accordingly, Euler couples in \(\mathcal{G }\) are in onetoone correspondence with semiinfinite open intervals in \(\mathbb{R }\).
(c) The Möbius group \(G :={\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2 := {\mathrm{PGL}}_2(\mathbb{R })\cong {\mathrm{GL}}_2(\mathbb{R })/\mathbb{R }^\times \) acts on the compactification \(\overline{\mathbb{R }}= \mathbb{R }\cup \{\infty \}\) of the real line by
We write \(G^{{\uparrow }}= {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\cong {\mathrm{PSL}}_2(\mathbb{R })\) for the subgroup of orientation preserving maps. The Cayley transform
is a homeomorphism, identifying \(\overline{\mathbb{R }}\) with the circle. Its inverse is the stereographic map
It maps the upper semicircle \(\{ z \in \mathbb{S }^1 :{\mathrm{Im}}z > 0\}\) to the positive half line \((0,+\infty )\). The Cayley transform intertwines the action of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) on \(\overline{\mathbb{R }}\) with the action of \({\mathrm {PSU}}_{1,1}(\mathbb{C }) ={\mathrm{SU}}_{1,1}(\mathbb{C })/\{\pm \mathbf{1 }\}\), given by
The threedimensional Lie group \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) is generated by the following oneparameter subgroups:

Rotations: \(\rho (\theta )(x) = \frac{\cos (\theta /2)x + \sin (\theta /2)}{\sin (\theta /2)x + \cos (\theta /2)}\) for \(\theta \in \mathbb{R }\); note that \(C(\rho (\theta )x) = e^{i\theta } C(x)\).

Dilations: \(\delta (t)(x)= e^t x\) for \(t \in \mathbb{R }\).

Translation: \(\zeta (t) x = x+t\) for \(t \in \mathbb{R }\).
In the circle picture \(\delta \) and \(\zeta \) will be denoted by \(\delta _{\cap }\) and \(\zeta _\cap \), referring to the upper semicircle with endpoints \(\{1,1\} = C(\{0,\infty \})\). Note that \(1\) is the unique fixed point of \(\zeta _\cap \) and one of the two fixed points \(\{\pm 1\}\) of \(\delta _\cap \). On the circle, \(\rho (\pi )\) maps 1 to \(1\) and exchanges the upper and the lower semicircle. Accordingly, \(\zeta _\cup =\rho (\pi )\zeta \rho (\pi ) \) is the subgroup of conjugated translations fixing the point \(1\in \mathbb{S }^1\).
We write \(\mathbf{K } = \rho (\mathbb{R })\), \(\mathbf{A } = \delta (\mathbb{R })\), \(\mathbf{N }^+ = \zeta (\mathbb{R })\) and \(\mathbf{N }^ = \zeta _\cup (\mathbb{R })\) for the corresponding onedimensional subgroups of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\), and \(\mathbf{P }^+ = \mathbf{A }\mathbf{N }^+ = {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_\infty \), \(\mathbf{P }^ := \mathbf{A }\mathbf{N }^ = {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_0\) for the stabilizer groups of \(\infty \) and 0 in \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\). We observe that \(\overline{\mathbb{R }}\cong {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}/\mathbf{P }^\) and that the circle group \(K= {\mathrm{PSO}}_2(\mathbb{R })\) acts simply transitively on \(\overline{\mathbb{R }}\).
On the compactified line, the point reflection \(\tau (x) = x\) in 0 acts on the Lie algebra by
Note that \(\tau \in G^{{\downarrow }}\).
The infinitesimal generator \(h := \begin{pmatrix} \frac{1}{2} &{} 0 \\ 0 &{} \frac{1}{2} \end{pmatrix}\) of \(\delta \) is an Euler element and \(W := (h,\tau )\) is an Euler couple. Since \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2 \cong {\mathrm{PGL}}_2(\mathbb{R }) \cong {\mathrm{Aut}}({\mathfrak{sl }}_2(\mathbb{R }))\), for any Euler couple \((x,\tau )\), the involution \(\tau \) is determined by the requirement that it acts on \(\mathfrak{g }={\mathfrak{sl }}_2(\mathbb{R })\) by \(e^{\pi i {\mathrm{ad}}x}\). We conclude that the action of \(G^{{\uparrow }}= {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) on the set of Euler couples is transitive, i.e., \(\mathcal{G }_E = G^{{\uparrow }}.(h,\tau )\).
To see the geometric side of Euler couples, let us call a nondense, nonempty open connected subset \(I \subseteq \mathbb{S }^1\) an interval and write \(\mathcal{I }(\mathbb{S }^1)\) for the set of intervals in \(\mathbb{S }^1\). It is easy to see that \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) acts transitively on \(\mathcal{I }(\mathbb{S }^1)\). To determine the stabilizer of an interval, we consider the upper half circle, which corresponds to the half line \((0,\infty ) \subseteq \overline{\mathbb{R }}\). Each element \(g \in {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) mapping \((0,\infty )\) onto itself fixes 0 and \(\infty \). Since it is completely determined by the image of a third point, it is of the form \(\delta (t)\) if \(g.1 = e^t\). Therefore the stabilizer of \((0,\infty )\) in \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) is the subgroup \(\delta (\mathbb{R })\), which coincides with the stabilizer of h under the adjoint action. This already shows that \(\mathcal{W }_+(W)\) and \(\mathcal{I }(\mathbb{S }^1)\) are isomorphic homogeneous spaces of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\). In particular, we can associate to an interval \(I = g(0,\infty )\) the reflection \(\tau _I=g \tau g^{1}\) and the oneparameter group \(\delta _I := g \delta g^{1}\). Note that \(\tau _I\) is an orientation reversing involution mapping I to the complementary open interval \(I'\). We write \(x_I := {\mathrm{Ad}}(g)h\) for the infinitesimal generator of \(\delta _I\), so that the assignment \(I \mapsto x_I\) defines an equivariant bijection \(\mathcal{I }(\mathbb{S }^1) \rightarrow \mathcal{E }(\mathfrak{g })\). The anticlockwise orientation of \(\mathbb{S }^1\), which can also be considered as a causal structure, is used here to pick the sign of \(x_I\) in such a way that the flow \(\delta _I\) is counter clockwise (future pointing) on I. Accordingly, \(x_{I'} = x_I\) corresponds to the complementary interval \(I'\).
To identify the natural order on the abstract wedge space \(\mathcal{G }_E = \mathcal{W }_+(W)\), we consider for \(X = \begin{pmatrix} a &{} b \\ c &{} a \end{pmatrix} \in \mathfrak{g }= {\mathfrak{sl }}_2(\mathbb{R })\) the corresponding fundamental vector field
This shows that
is a pointed generating invariant cone in \(\mathfrak{g }\). The Lie wedge specified by the triple \((h,\tau , C)\) is
We further have \(G(W) = G^{{\uparrow }}\), and the associated semigroup is
Therefore the map
defines an order preserving bijection between the abstract wedge space \(\mathcal{W }(W)\) and the ordered set \(\mathcal{I }(\mathbb{S }^1)\).
(d) We now consider the universal covering of the Möbius group \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\). Concretely, we put \(G := {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}} \rtimes \{\mathbf{1 },{\widetilde{\tau }}\}\), where \({\widetilde{\tau }}\) acts on \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) by integrating \({\mathrm{Ad}}(\tau )\) from (2.16) to an automorphism of \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\). The group G is a graded Lie group and \(G^{{\uparrow }}:= {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) is its identity component. We have a covering homomorphism \(q_G: G \rightarrow {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2\) whose kernel \(Z({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}) \cong \mathbb{Z }\) is discrete cyclic. We write \({\widetilde{\rho }}\), \({\widetilde{\delta }}\), \({\widetilde{\zeta }}\) and \({\widetilde{\zeta }}_\cup \) for the canonical lifts of the oneparameter groups \(\rho \), \(\delta \), \(\zeta \), \(\zeta _\cup \) of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\), \({\widetilde{\mathbf{P }}}^+ := {\widetilde{\delta }}(\mathbb{R }) {\widetilde{\zeta }}(\mathbb{R })\), and \({\widetilde{\mathbf{P }}}^ := {\widetilde{\delta }}(\mathbb{R }) {\widetilde{\zeta }}_\cup (\mathbb{R })\).
The action of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) on \(\mathbb{S }^1\) lifts canonically to an action of the connected group \(G^{{\uparrow }}= {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) on the universal covering \(\widetilde{\mathbb{S }^1} \cong \mathbb{R }\), where we fix the covering map \(q_{\mathbb{S }^1} :\mathbb{R }\rightarrow \widetilde{\overline{\mathbb{R }}}\), defined by \(q_{\mathbb{S }^1}(\theta ) = {\widetilde{\rho }}(\theta ).0\), which corresponds to the map \(\theta \mapsto e^{i\theta } = C({\widetilde{\rho }}(\theta ).0)\) in the circle picture. We may thus identify \(\widetilde{\mathbb{S }^1}\) with the homogeneous space \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}/{\widetilde{\mathbf{P }}}^\cong \mathbb{R }\). As conjugation with \({\widetilde{\tau }}\) on \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) preserves the subgroup \({\widetilde{\mathbf{P }}}^\), it also acts on \(\widetilde{\mathbb{S }^1}\). From (2.16) it follows that it simply acts by the point reflection \({\widetilde{\tau }}.x =  x\) in the base point 0. We also note that \(Z := \ker (q_G) = {\widetilde{\rho }}(2\pi \mathbb{Z })\) is the group of deck transformations of the covering \(q_{\mathbb{S }^1}\), which acts by
We call a nonempty interval \(I \subseteq \mathbb{R }\) admissible if its length is strictly smaller than \(2\pi \) and write \(\mathcal{I }(\mathbb{R })\) for the set of admissible intervals. An interval \(I \subseteq \mathbb{R }\) is admissible if and only if there exists an interval \(\underline{I} \in \mathcal{I }(\mathbb{S }^1)\) such that I is a connected component of \(q_{\mathbb{S }^1}^{1}(\underline{I})\). The group Z acts transitively on the set of these connected components. As \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) acts transitively on \(\mathcal{I }(\mathbb{S }^1)\), it follows that the group \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) acts transitively on the set \(\mathcal{I }(\mathbb{R })\), and that composition with \(q_{\mathbb{S }^1}\) yields an equivariant covering map
We further have:

The group \({\widetilde{\mathbf{P }}}^+ = {\widetilde{\delta }}(\mathbb{R }) {\widetilde{\zeta }}(\mathbb{R })\) fixes the points \(\{(2k+1)\pi :k\in \mathbb{Z }\}\).

For \(I \in \mathcal{I }(\mathbb{S }^1)\), let \({\widetilde{\delta }}_I\) be the lift of the oneparameter group \(\delta _I\). Then \({\widetilde{\delta }}_I\) preserves every interval in the preimage \(q_{\mathbb{S }^1}^{1}(I)\).

The inverse images of \(\tau \in {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2\) in \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_2\) are the elements \({\widetilde{\tau }}_n := {\widetilde{\rho }}(2\pi n){\widetilde{\tau }}\), \(n \in \mathbb{Z }\). These are involutions, acting by
$$\begin{aligned} {\widetilde{\tau }}_n(x)= 2\pi n x \quad \text{ for } \quad x\in \mathbb{R }\end{aligned}$$(2.21)which is a point reflection in the point \(\pi n\). All pairs \((h, {\widetilde{\tau }}_n)\) are Euler couples in \(\mathcal{G }({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_2)\), and from the discussion of the set of Euler couples \(\mathcal{G }_E({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2)\) under (c), we know that the involutions \({\widetilde{\tau }}_n\) exhaust all possibilities for supplementing h to an Euler couple.
There is an interesting difference to the situation for \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2\), where \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) acts transitively on the set \(\mathcal{G }_E({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2)\) of Euler couples. To see what happens for \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_2\), recall that the stabilizer of the element \((h,\tau )\in \mathcal{G }_E({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2)\) in \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) is the subgroup \(\delta (\mathbb{R })\). Its inverse image is the group
$$\begin{aligned} {\widetilde{\delta }}(\mathbb{R }) {\widetilde{\rho }}(2\pi \mathbb{Z }) \cong \mathbb{R }\times \mathbb{Z }.\end{aligned}$$An element \(g \in {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) fixes \((h,{\widetilde{\tau }}_n)\) if and only if \({\mathrm{Ad}}(g)h = h\) and \(g {\widetilde{\tau }}_n g^{1} = {\widetilde{\tau }}_n\). The first condition is equivalent to g being of the form
$$\begin{aligned} g = {\widetilde{\delta }}(t) {\widetilde{\rho }}(2\pi k) \quad \text{ for } \text{ some } \quad t\in \mathbb{R }, k \in \mathbb{Z }.\end{aligned}$$The second condition is equivalent to \({\widetilde{\tau }} g {\widetilde{\tau }} = {\widetilde{\tau }}_n g {\widetilde{\tau }}_n = g\), which takes the form
$$\begin{aligned} {\widetilde{\delta }}(t) {\widetilde{\rho }}(2\pi k) = {\widetilde{\delta }}(t) {\widetilde{\rho }}(2\pi k),\end{aligned}$$and this is equivalent to \(k = 0\). We conclude that the stabilizer of \((h,{\widetilde{\tau }}_n)\) is
$$\begin{aligned} {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_{(h,{\widetilde{\tau }}_n)} = {\widetilde{\delta }}(\mathbb{R }). \end{aligned}$$(2.22)We also note that
$$\begin{aligned} {\widetilde{\rho }}(\pi k).(h,{\widetilde{\tau }}_n) = ( (1)^k h, {\widetilde{\rho }}(\pi k){\widetilde{\tau }}_n{\widetilde{\rho }}(\pi k)) = ((1)^k h, {\widetilde{\rho }}(2\pi k){\widetilde{\tau }}_n) = ((1)^k h, {\widetilde{\tau }}_{n+k}).\end{aligned}$$We conclude that the group \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) does not act transitively on the set \(\mathcal{G }_E\) of Euler couples. It has two orbits:
$$\begin{aligned} \mathcal{G }_E({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_2) = G^{{\uparrow }}.W_0 {\dot{\cup }} G^{{\uparrow }}.{W_1} = \mathcal{W }_{+}(W_0) {\dot{\cup }} \mathcal{W }_{+}({W_1}) \quad \text{ for } \quad W_0 := (h,{\widetilde{\tau }}_0), W_1 := (h,{\widetilde{\tau }}_1).\nonumber \\ \end{aligned}$$(2.23)We also refer to Example 2.14 for a discussion of this issue from a different perspective.

The subgroup \({\widetilde{\delta }}(\mathbb{R })\) preserves every interval which is a nontrivial orbit of \({\widetilde{\delta }}(\mathbb{R })\), acting on \(\mathbb{R }\). If, conversely, \(g \in {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\) preserves such an interval, then its image in \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) is contained in \(\delta (\mathbb{R })\), so that
$$\begin{aligned} g = {\widetilde{\delta }}(t) {\widetilde{\rho }}(2\pi k)\quad \text{ for } \text{ some } \quad t\in \mathbb{R }, k \in \mathbb{Z }.\end{aligned}$$As every open orbit of \({\widetilde{\delta }}(\mathbb{R })\) is an interval of length \(\pi \), the element g can only preserve such an orbit if \(k = 0\). This shows that \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_{(h,{\widetilde{\tau }}_n)}\) also is the stabilizer group of any open \({\widetilde{\delta }}(\mathbb{R })\)orbit in \(\mathbb{R }\). We conclude that, for the Euler couple \(W_0 = (h, {\widetilde{\tau }}_0)\), the map
$$\begin{aligned} {\Phi } :\mathcal{W }_+(W_0) \rightarrow \mathcal{I }(\mathbb{R }), \quad g.(h,{\widetilde{\tau }}_0) \mapsto g (0,\pi ) \end{aligned}$$(2.24)defines a \(G^{{\uparrow }}\)equivariant bijection between the abstract wedge space \(\mathcal{W }_+(W_0) \subseteq \mathcal{G }\) and the set \(\mathcal{I }(\mathbb{R })\) of admissible intervals in \(\mathbb{R }\). Since the full group G acts on the space \(\mathcal{I }(\mathbb{R })\) of intervals, \(\Phi \) can be used to transport this action to a Gaction on the space \(\mathcal{W }_+(W_0)\), extending the action of the subgroup \(G^{{\uparrow }}\). Since \(\tau _0(0,\pi )=(\pi ,0)=\rho (\pi )(0,\pi ),\) we have
$$\begin{aligned} \Phi ^{1}(\tau _0(0,\pi ))=\Phi ^{1}(\rho (\pi )(0,\pi )) =\rho (\pi ).\Phi ((0,\pi ))^{1}=(h,\rho (2\pi )\tau _0), \end{aligned}$$so that \(\tau _0.W_0:=(h,\rho (2\pi )\tau _0)\). By \(G^{{\uparrow }}\)equivariance of the map \(\Phi \), we conclude that the action of \(G^{{\downarrow }}\) on \(\mathcal{W }_+(W_0)\) is given by
$$\begin{aligned} g *_{\rho (2\pi )} (x,\sigma ) := ({\mathrm{Ad}}^\varepsilon (g), \rho (2\pi ) g \sigma g^{1}) \quad \text{ for } \text{ every } \quad g \in G^{{\downarrow }}.\end{aligned}$$(2.25)Here we use that \({\widetilde{\rho }}(2\pi ) \in Z(G^{{\uparrow }})\). Note that we have chosen \((0,\pi )\) to be the image of \(W_0\) through \(\Phi \). Further possible actions come from the identifications
$$\begin{aligned} {\Phi _n} :\mathcal{W }_+(W_n) \rightarrow \mathcal{I }(\mathbb{R }), \quad g.(h,{\widetilde{\tau }}_n) \mapsto g (0,\pi ) \quad \text{ with } \quad W_n=(h,\tau _n), \end{aligned}$$(2.26)and one can likewise see that
$$\begin{aligned} g *_{\alpha _n} (x,\sigma ) := ({\mathrm{Ad}}^\varepsilon (g), \alpha _n g \sigma g^{1}) \quad \text{ for } \quad g \in G^{{\downarrow }}\quad \text{ and } \quad \alpha _n = {\widetilde{\rho }}((2n1)2\pi ) \in Z(G^{{\uparrow }}), \end{aligned}$$extends the action of \(G^{{\uparrow }}\) on \(\mathcal{W }_+(W_n)\) to G and \(\Phi =\Phi _0\) for \(n=0\) (see also (2.37) and Section 2.4.2 for this kind of action).
(e) Let \(q :{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}^{(n)} \rightarrow {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) be the nfold covering group of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\) and \(\rho ^{(n)}, \delta ^{(n)}, \zeta ^{(n)}\) and \(\zeta _{\cup }^{(n)}\) be the lifts of the corresponding oneparameter groups of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\). We further put \(\mathbf{P }^{,(n)} := \delta ^{(n)}(\mathbb{R }) \zeta _{\cup }^{(n)}(\mathbb{R })\), so that we obtain an nfold covering
of the circle, and the action of the oneparameter group \(\rho ^{(n)}\) induces a diffeomorphism
The set of wedges can be described analogously to the case (d), but there is a difference depending on the parity of n. If n is even, the group \(G^{{\uparrow }}\) has two orbits in the set \(\mathcal{G }_E\) of Euler couples, but if n is odd, there is only one. Indeed, for \(n = 2k\), the element \(\rho ^{(n)}(2\pi k)\) acts as an involution on \(\mathbb{S }^1_n\). So it fixes all Euler couples \((h,{\widetilde{\tau }}_n)\), even if it does NOT fix any proper interval in \(\mathbb{S }^1_n\) (see also Example 2.14).
(f) The example arising most prominently in physics is the proper Poincaré group
It acts on \(1+d\)dimensional Minkowski space \(\mathbb{R }^{1,d}\) as an isometry group of the Lorentzian metric given by \((x,y)= x_0y_0{\mathbf{x}}{\mathbf{y}}\) for \(x = (x_0, {\mathbf{x}}) \in \mathbb{R }^{1,d}\). Writing
for the open future light cone, the grading on G is specified by time reversal, i.e., \(gV_+ = \varepsilon (x,g) V_+\). In particular \(C := \overline{V_+}\) is a pointed closed convex cone satisfying (2.4). For \(d > 1\), this is, up to sign, the only nonzero pointed invariant cone in the Lie algebra \(\mathfrak{g }\).
The generator \(k_{1} \in {\mathfrak{so }}_{1,d}(\mathbb{R })\) of the Lorentz boost on the \((x_0,x_1)\)plane
is an Euler element. It combines with the spacetime reflection \(j_1(x) =(x_0,x_1,x_2,\ldots ,x_d)\) to the Euler couple \((k_1, j_1)\). We associate to \((k_1, j_1)\) the spacetime region
the standard right wedge, and note that \(W_1\) is invariant under \(\exp (\mathbb{R }k_{1})\). It turns out that the semigroup \(\mathcal{S }_{( k_1,j_1)}\) associated to the couple \(( k_1,j_1)\) in Definition 2.5 satisfies
(see [NÓ17, Lemma 4.12]). From (2.27) it follows that the map
defines an order preserving bijection between the abstract wedge space \(\mathcal{W }\subseteq \mathcal{G }\) and the set of wedge domains in Minkowski space \(\mathbb{R }^{1+d}\). For an abstract wedge \(W = ( k_W, j_W) \in \mathcal{W }\), the Euler element \(k_W\) is the corresponding boost generator. For an axial wedge \(W_i:=\{x\in \mathbb {R}^{1+d}:x_0<x_i\}\), \(i =1,\ldots , n\), the corresponding Euler couple will be denoted \((k_i,j_i)\).
Nets of wedges, isotony, central locality and covering groups
In the following sections we will focus on the description of relative positions of wedges, in particular wedge inclusions and the locality principle.
Wedge inclusion
Firstly consider this wedge inclusion configuration called halfsided modular inclusion:
Definition 2.11
Let \(W_0 = (x,\sigma ) \in \mathcal{G }\) and \(y \in \pm C\) with \([x,y] = \pm y\). Then \(\exp (y) \in \mathcal{S }_{W_0}\) (Definition 2.5(b)), so that
We then call \(W_1 \le W_0\) a ±halfsided modular inclusion.
The next lemma shows that any wedge inclusion can be described in terms of positive and negative halfsided modular inclusions.
Lemma 2.12
If \(W_1 \le W_3\) in \(\mathcal{G }\), then there exists an element \(W_2 \in \mathcal{G }\) with \(W_1 \le W_2 \le W_3\) for which the inclusion \(W_1 \le W_2\) is \(+\)halfsided modular and the inclusion \(W_2 \le W_3\) is −halfsided modular.
Proof
That \(W_1 \le W_3\) means that \(W_1 = s W_3\) for some
Accordingly, we write \(s = g_ g_+ g_0\) and observe that \(W_1 = g_ g_+ W_3\) because \(g_0 W_3 = W_3\). Put \(W_2 := g_ W_3\). Then \(W_2 \le W_3\) and \(g_+ W_3 \le W_3\) implies \(W_1 = g_ g_+ W_3 \le g_ W_3 = W_2\).
Further, the inclusion \(W_2 \le W_3\) is −halfsided modular because \(g_ \in \exp (C_(W_3))\). Likewise the inclusion \(g_+ W_3 \le W_3\) is \(+\)halfsided modular, and therefore \(W_1 \le W_2\) is also \(+\)halfsided modular. \(\square \)
Central locality
For a wedge \(W = (x,\sigma )\), the dual wedge \(W' = (x,\sigma )\) need not be contained in the orbit \(\mathcal{W }_+ = G^{{\uparrow }}.W\). If, however, \(G^{{\uparrow }}\) has a nontrivial central subgroup Z such that, modulo Z, the complement \(W'\) is contained in \(\mathcal{W }_+\), then we use central elements \(\alpha \in Z\) to define “twisted complements” \(W^{'\alpha }\) which are contained in \(\mathcal{W }_+\), and this in turn leads to a twisted action of the full group G on \(\mathcal{W }_+\). We also obtain on \(\mathcal{W }_+\) a complementation map \(W \mapsto W^{'\alpha }\).
Let \(Z \subseteq Z(G^{{\uparrow }})\) be a closed normal subgroup of G, and \(q :G \rightarrow {\underline{G}}:= G/Z\) be the corresponding surjective morphism of graded Lie groups with kernel Z. If Z is discrete, then q is a covering map. The morphism of graded Lie groups q induces a natural map
where \({\mathrm{Ad}}_\mathfrak{g }:{\underline{G}}\rightarrow {\mathrm{Aut}}(\mathfrak{g })\) denotes the factorized adjoint action which exists because \(Z = \ker (q)\) acts trivially on \(\mathfrak{g }\). It restricts to a map
As the following example shows, neither of these maps is always surjective. The main obstruction is that, although the differential \(\mathbf{L{}}(q):\mathbf{L{}}(G) \rightarrow \mathbf{L{}}({\underline{G}})\) is surjective, there may be involutions \(\tau \in {\underline{G}}^{{\downarrow }}\) for which no involution \(\sigma \in G^{{\downarrow }}\) with \(q(\sigma ) = \tau \) exists. This phenomenon is tightly related to the twisted groups \({\widehat{G}}_z\) discussed in Remark 2.7 because these twists disappear for \(z \in Z\) in \({\widehat{G}}/Z \cong G/Z\).
Example 2.13
We consider the graded Lie group
It has two connected component and \(G^{{\uparrow }}= {\mathrm{SL}}_2(\mathbb{R })\).^{Footnote 6} The subgroup \(Z := \{\pm \mathbf{1 }\}\) is central and the quotient map \(q :G \rightarrow {\underline{G}}:= G/Z\) is a 2fold covering. The Euler element \(x := \frac{1}{2}\begin{pmatrix} 1 &{} \quad 0 \\ 0 &{} \quad 1 \end{pmatrix} \in \mathfrak{g }= {\mathfrak{sl }}_2(\mathbb{R })\) combines with the involution \(q(\gamma ) \in {\underline{G}}^{{\downarrow }}\) to the Euler couple \((x,q(\gamma )) \in \underline{\mathcal{G }}\). However, the set \(\mathcal{G }(G)\) is empty because \(G^{{\downarrow }}\) contains no involution. In fact, for \(g = \begin{pmatrix} a &{} \quad b \\ c &{} \quad d \end{pmatrix} \in {\mathrm{SL}}_2(\mathbb{R })\), the condition that \(g\gamma \) is an involution is equivalent to
This is equivalent to \(a = d\) and \(b = c = 0\), contradicting that \(1 = \det (g) = a^2\). We conclude in particular that the maps \(\mathcal{G }(G) \rightarrow \underline{\mathcal{G }}\) and \(\mathcal{G }_E(G) \rightarrow \mathcal{G }_E({\underline{G}})\) are not surjective.
We now discuss \(G^{{\uparrow }}\)orbits in \(\mathcal{G }(G)\). In the examples we have in mind, the central subgroup Z is discrete.
Involution lifts and central wedge orbit. Each element \(\sigma \in G^{{\downarrow }}\) acts in the same way on the abelian normal subgroup Z by the involution
which restricts to an involution \(\sigma _ Z \in {\mathrm{Aut}}( Z)\) because Z is central in \(G^{{\uparrow }}\) and a normal subgroup of G. In the following we shall need the subgroups
For \(\gamma \in Z^\), the element \(\gamma ^2 = (\gamma ^\sigma \gamma ^{1})^{1}\) is contained in \( Z_1\), so that the quotient group \( Z^/ Z_1\) is an elementary abelian 2group, i.e., isomorphic to \(\mathbb{Z }_2^{(B)}\) for some index set B.
For an involution \(\sigma \in G^{{\downarrow }}\) and \(\beta \in Z(G^{{\uparrow }})\), the element \(\beta \sigma \in G^{{\downarrow }}\) is an involution if and only if \(\beta \in Z^\). Therefore
defines an action of \( Z^\) on \(\mathcal{G }(G)\), commuting with the conjugation action of \(G^{{\uparrow }}\) and satisfying
For \(W = (x,\sigma ) \in \mathcal{G }( G)\), the fiber over \({\underline{W}}:= (x,q(\sigma ))\) is thus given by
The subgroup \( Z\subseteq G^{{\uparrow }}\) acts by conjugation on the fiber \(Z^*W\):
so that the quotient group \( Z^/ Z_1\) parametrizes the Zconjugation orbits in the fiber \( Z^*W\).^{Footnote 7} Here is an example.
Example 2.14
(a) If \( Z \cong \mathbb{Z }\) and \(n^\sigma = n\), then \( Z^ = \mathbb{Z }\) and \( Z_1 = 2 \mathbb{Z }\), so that \( Z^/ Z_1 \cong \mathbb{Z }/2\mathbb{Z }\).
(b) If \( Z = \mathbb{Z }_n\) and \(\overline{n}^\sigma = \overline{n}\), then \( Z^ = \mathbb{Z }_n\) and \( Z_1 = 2 \mathbb{Z }_n\), so that
Wedge \(G^{{\uparrow }}\)orbits. Let \(W = (x,\sigma ) \in \mathcal{G }_E(G)\) and \(\underline{W} = (x,q(\sigma )) \in \underline{\mathcal{G }}\). In general the group \( G^{{\uparrow }}\) does not act transitively on the inverse image of the orbit \({\underline{\mathcal{W }}}_+ := {\underline{G}}^{{\uparrow }}.{\underline{W}}\subseteq \underline{\mathcal{G }}\) under \(q_\mathcal{G }\). We now describe how this set decomposes into orbits. By the transitivity of the \({\underline{G}}^{{\uparrow }}\)action on \({\underline{\mathcal{W }}}_{+}\), it suffices to consider the orbits of the stabilizer
on the fiber \(Z^ * W\). That \(g \in G^{{\uparrow }}\) fixes \({\underline{W}}\) implies in particular that \(g\sigma g^{1}\sigma = g (g^\sigma )^{1} \in Z\). This leads to a homomorphism
As \( Z \subseteq G^{{\uparrow }}_{{\underline{W}}}\), the image \( Z_2 := \partial ( G^{{\uparrow }}_{{\underline{W}}})\) is a subgroup containing \( Z_1\).
Example 2.15
(An example where \(Z_1 \not = Z_2\).) We consider the group \(G = {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}} \rtimes \{\mathbf{1 },{\widetilde{\tau }}\}\) from Example 2.10(d) and the canonical homomorphism
whose kernel is the central subgroup \(Z := 2 Z(G^{{\uparrow }}) \subseteq Z(G^{{\uparrow }}) \cong \mathbb{Z }\) of index two. Now \(W = (h,{\widetilde{\tau }}) \in \mathcal{G }(G)\) is an Euler couple mapped to \(\underline{W} = (h,\sigma ) \in \underline{\mathcal{G }}\). As \(z^{{\widetilde{\tau }}} = z^{1}\) for every \(z \in Z\), we have \(Z = Z^\) and \(Z_1 = 2Z\) is a subgroup of index 2. To calculate \(Z_2\), we observe that
We conclude that
The situation changes if we consider \(Z=Z(G^{{\uparrow }})\) and the centerfree group \({\underline{G}}= {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\rtimes \{\mathbf{1 },\tau \}\) instead. Then \(Z = Z^ = Z(G^{{\uparrow }})\) and \(Z_1 = Z_2 = 2 Z\).
As the \(G^{{\uparrow }}\) orbits in \(q_\mathcal{G }^{1}(\underline{G}^{{\uparrow }}.\underline{W}) = q_\mathcal{G }^{1}(\underline{\mathcal{W }}_+)\) correspond to the \(G^{{\uparrow }}_{\underline{W}}\)orbits in the fiber \(q_\mathcal{G }^{1}(\underline{W}) = Z^ * W\), we obtain the following lemma.
Lemma 2.16
The quotient group \(Z^/Z_2\) parametrizes the set of \(G^{{\uparrow }}\)orbits in \(q_\mathcal{G }^{1}({\underline{\mathcal{W }}}_{+})\).
\(\alpha \)twisted complement. The following definition generalizes the notion of complementary wedge given in Definition 2.5 (a).
Definition 2.17
For \(\alpha \in { Z^}\), we define the \(\alpha \)twisted complement of \(W = (x,\sigma ) \in \mathcal{G }( G)\) by
We will refer to couples of the form \(W^{'\alpha }\) as complementary wedges. We consider \(W^{'\alpha }\) as a “complement” of W because \(q_\mathcal{G }\) maps \(W^{'\alpha }\) to \(W'\) (see item (a) below).
Lemma 2.18
For each \(\alpha \in Z^\), the \(\alpha \)twisted complementation \(W \mapsto W^{'\alpha }\) satisfies:

(a)
For \(\alpha \in Z^\), \(W^{'\alpha }\) is mapped by \(q_\mathcal{G }\) onto the complement \(W' = (x, q(\sigma ))\) of \({\underline{W}}= (x,q(\sigma ))\).

(b)
The \(\alpha \)twisted complementation is not involutive if \(\alpha ^2 \not =e\).

(c)
The map \({}^{'\alpha } :\mathcal{G }( G) \rightarrow \mathcal{G }( G), (x,\sigma ) \mapsto (x, \alpha \sigma )\) is \( G^{{\uparrow }}\)equivariant.

(d)
In terms of the action (2.32) of \(Z^\) on \(\mathcal{G }(G)\), we have
$$\begin{aligned} W^{'\alpha } = \alpha * W' \quad \text{ for } \quad W \in \mathcal{G }(G), \alpha \in Z^. \end{aligned}$$(2.36) 
(e)
The prescription
$$\begin{aligned} g *_\alpha (x,\sigma ) :={\left\{ \begin{array}{ll} g.(x,\sigma ) &{} \text { for } g \in G^{{\uparrow }}\\ g.(\alpha ^{1} * (x,\sigma )) = \alpha * (g.(x,\sigma )) &{} \text { for } g \in G^{{\downarrow }}. \end{array}\right. } \end{aligned}$$(2.37)defines an action of G on \(\mathcal{G }(G)\). This action satisfies
$$\begin{aligned} W^{'\alpha } = \sigma *_\alpha W \quad \text{ for } \quad W = (x,\sigma ) \in \mathcal{G }(G), \alpha \in Z^. \end{aligned}$$(2.38)If \(W^{'\alpha }\in G^{{\uparrow }}.W\), then \(\mathcal{W }_+ = G^{{\uparrow }}.W\) is invariant under the full group G with respect to the \(\alpha \)twisted action.

(f)
There exists an \(\alpha \in Z^\) with \(W^{'\alpha } \in \mathcal{W }_+\) if and only if \(\underline{W}' := (x,q(\sigma )) \in G^{{\uparrow }}.\underline{W}\). If this is the case, then \(W^{'\beta } \in \mathcal{W }_+\) for \(\beta \in Z^\) if and only if \(\beta ^{1}\alpha \in Z_2\). In this case, the twisted actions of \(g \in G^{{\downarrow }}\) are related by \(g*_\beta = (\beta \alpha ^{1}) * g *_\alpha \).
Proof
(a) and (b) are easy to see.
(c) follows from \(\alpha \in Z( G^{{\uparrow }})\) and the \(G^{{\uparrow }}\)equivariance of the complementation map.
(d) is immediate from the definition of \(\alpha * W\).
(e) That the prescription defines an action follows easily from the fact that \(g_1 *_\alpha (g_2 *_\alpha W)= (g_1 g_2).W\) for \(g_1, g_2 \in G^{{\downarrow }}\) (cf. (2.33))). The relation (2.38) follows from \(\sigma .W = \sigma .(x,\sigma ) = (x,\sigma )\). For the last statement, we note that by (2.38), the relation \(W^{'\alpha } \in \mathcal{W }_+\) implies
(f) As \(q_\mathcal{G }(\mathcal{W }_+) = \underline{\mathcal{W }}_+ = G^{{\uparrow }}.\underline{W}\) and \(q_\mathcal{G }(W^{'\alpha }) = \underline{W}'\), the inclusion \(W^{'\alpha } \in \mathcal{W }_+\) implies that \(\underline{W}' \in \underline{\mathcal{W }}_+\). If, conversely, \(\underline{W}' \in \underline{\mathcal{W }}_+\), then there exists a \(g \in G^{{\uparrow }}\) with
so that \(\alpha := g\sigma g^{1} \sigma \in \ker (q) = Z\) satisfies
Now suppose that \(W^{'\alpha } = \alpha * W' \in \mathcal{W }_+\). Then \(W^{'\beta } = \beta * W' \in \mathcal{W }_+\) is equivalent to \(\beta \alpha ^{1}* W^{'\alpha } = W^{'\beta } \in \mathcal{W }_+\), and this is equivalent to \(\beta ^{1}\alpha * \mathcal{W }_+ = \mathcal{W }_+\). Next we observe that the relation \(\beta \alpha ^{1}* W \in \mathcal{W }_+\) is equivalent to the existence of some \(g \in G^{{\uparrow }}_{\underline{W}}\) with \(g.W = (x,\beta ^{1}\alpha \sigma )\), which means that \(\beta \alpha ^{1} \in Z_2 = \partial (G^{{\uparrow }}_{\underline{W}})\). \(\square \)
Example 2.19
We show that for \(G = {\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}} \rtimes \{\mathbf{1 },{\widetilde{\tau }}\}\) as in Example 2.10(d), we have to use twisted complements to obtain a \(G^{{\uparrow }}\)orbit in \(\mathcal{G }_E(G)\) invariant under complementation. We have already seen that \(\mathcal{G }_E({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}})\) contains two \(G^{{\uparrow }}\)orbits, represented by the couples \(W_0 = (h,{\widetilde{\tau }})\) and \(W_1 = (h,{\widetilde{\tau }}_1)\). The complement \(W_0' = (h, {\widetilde{\tau }})\) satisfies
so that complementation exchanges the two \(G^{{\uparrow }}\)orbits in \(\mathcal{G }_E({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}})\). On the other hand, for the action \(*_\alpha \) defined in (2.37), the full group G preserves both \(G^{{\uparrow }}\)orbits.
Since \({\mathrm{Ad}}(\rho (\pi ))h = h\), the element \(g := {\widetilde{\rho }}(\pi )\) can be used to define a suitable \(\alpha \)twisted conjugation as follows. We note that
is a generator of \(Z := Z({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}) = Z^\). We now have
Thus \(\mathcal{G }_E({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_2)\) consists of two \(G^{{\uparrow }}\)orbits, none of which is invariant under complementation, but both are invariant under \(\alpha \)complementation. An analogous computation leads to the same picture for even coverings of \({\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}\), in particular for the fermionic case.
Euler Elements and 3graded Lie Algebras
In this section we exhibit a general relation between two notions that are a priori unrelated: complementary and orthogonal wedges. For the sake of simplicity we consider in this introductory part the case of the Poincaré group \(G=\mathcal{P }_+\) on \(\mathbb {R}^{1+2}\) (cf. Example 2.10). We have seen that if \(W=( k_W,j_W)\) is a wedge of the group G, then \(W'=( k_W,j_W)\) is the opposite wedge. The \(\pi \)spatial rotation \(\rho (\pi )\) takes W onto \(W'\) and vice versa. Thus there exists a group element \(g\in G^\uparrow =\mathcal{P }_+^\uparrow \) such that \({\mathrm{Ad}}(g) k_W = k_W\), and in this sense \( k_W\) is symmetric. This ensures a symmetry between a wedge and its opposite wedge, which corresponds to its causal complement in Minkowski spacetime.
Typical pairs of orthogonal wedges are the coordinate wedges
The importance of this couple of wedges comes by the clear geometric relation: the wedge reflection of \(W_1\) acts on the orthogonal wedge as
In [GL95] the authors study the orthogonality relation in order to extend the unitary covariance representation of the Poincaré group \(\mathcal{P }_+^\uparrow \) to an (anti)unitary representation of the graded group \(\mathcal{P }_+\) and establish the Spin–Statistics Theorem. In this extension process, orthogonal Euler wedges play a crucial role. This point will be discussed from our abstract perspective in Section 4.4 below.
In this section we will see how, in our setting, the existence of a symmetric Euler element in the Lie algebra ensures the existence of an orthogonal pair. For symmetric Euler elements, the orthogonality relation for Euler elements is symmetric, and orthogonal pairs of Euler elements generate a subalgebra isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\) in \(\mathfrak{g }\).
Preliminaries on Lie algebras and algebraic groups
In this subsection we collect some basic facts on finite dimensional real Lie algebras and on real algebraic groups (see [HN12] for Lie algebras and [Ho81] for algebraic groups).
A Lie algebra \(\mathfrak{g }\) is called simple if \(\mathfrak{g }\) and \(\{0\}\) are the only ideals of \(\mathfrak{g }\). It is called semisimple if it is a direct sum of simple ideals \(\mathfrak{g }= \mathfrak{g }_1 \oplus \cdots \oplus \mathfrak{g }_n\). On the other side of the spectrum, we have solvable Lie algebras. These are the ones for which the derived series defined by \(D^0(\mathfrak{g }) := \mathfrak{g }\) and \(D^{n+1}(\mathfrak{g }) := [D^n(\mathfrak{g }), D^n(\mathfrak{g })]\) satisfies \(D^N(\mathfrak{g }) = \{0\}\) for some \(N \in \mathbb{N }\). Here
is the commutator algebra of \(\mathfrak{g }\).
The fundamental theorem on the Levi decomposition asserts that, if \(\mathfrak{r }\) is the maximal solvable ideal of \(\mathfrak{g }\), then there exists a semisimple subalgebra \(\mathfrak{s }\) (a Levi complement), such that
is a semidirect sum, i.e., a vector space direct sum of the ideal \(\mathfrak{r }\) and the subalgebra \(\mathfrak{s }\).
A key feature in the structure theory of semisimple real Lie algebras is the concept of a compactly embedded subalgebra. A subalgebra \(\mathfrak{k }\subseteq \mathfrak{g }\) is said to be compactly embedded if the subgroup \({\mathrm{Inn}}_\mathfrak{g }(\mathfrak{k }) = \langle e^{{\mathrm{ad}}\mathfrak{k }} \rangle \subseteq {\mathrm{Aut}}(\mathfrak{g })\) has compact closure. We write \({\mathrm{Inn}}(\mathfrak{g }) := {\mathrm{Inn}}_\mathfrak{g }(\mathfrak{g })\) for the subgroup of inner automorphisms of \(\mathfrak{g }\).
An element \(x \in \mathfrak{g }\) is called

elliptic, if \({\mathrm{ad}}x\) is semisimple with purely imaginary eigenvalues, which is equivalent to the onedimensional Lie subalgebra \(\mathbb{R }x\) being compactly embedded.

hyperbolic, if \({\mathrm{ad}}x\) is diagonalizable.

nilpotent, if \({\mathrm{ad}}x\) is nilpotent, i.e., \(({\mathrm{ad}}x)^n = 0\) for some \(n \in \mathbb{N }\).
The Cartan–Killing form
is a symmetric bilinear form on \(\mathfrak{g }\) invariant under the automorphism group \({\mathrm{Aut}}(\mathfrak{g })\). Recall that a finite dimensional real Lie algebra is semisimple if and only if \(\kappa \) is nondegenerate (Cartan’s criterion). Note that \(\kappa (x,x) = {\mathrm{tr}}( ({\mathrm{ad}}x)^2) \ge 0\) if x is hyperbolic and \(\kappa (x,x) \le 0\) if x is elliptic.
In the proof of Proposition 3.2 below we shall use some results from the theory of linear algebraic groups. We now recall the basic concepts. If V is a finite dimensional real vector space, then \({\mathrm{GL}}(V)\) denotes the group of linear automorphisms of V. Any polynomial function on the linear space \({\mathrm{End}}(V)\) defines a function on the group \({\mathrm{GL}}(V)\) and we call a subgroup \(G \subseteq {\mathrm{GL}}(V)\) algebraic if it is the zero set of a family of polynomial functions \(p_j :{\mathrm{End}}(V) \rightarrow \mathbb{R }\). An algebraic group G is said to be

reductive, if each Ginvariant subspace \(V_1 \subseteq V\) has a Ginvariant linear complement \(V_2\).

unipotent, if there exists a flag of linear subspaces
$$\begin{aligned} F_0 = \{0\} \subseteq F_1 \subseteq \cdots \subseteq F_n = V \end{aligned}$$such that \((g\mathbf{1 })F_j \subseteq F_{j1}\) for \(j = 1,\ldots , n\) and \(g \in G\).
In this context one has a decomposition theorem (the Levi decomposition), asserting that every algebraic subgroup \(G \subseteq {\mathrm{GL}}(V)\) is a semidirect product \(G \cong U \rtimes L\), where U is unipotent and L is reductive. Moreover, for every reductive subgroup \(L_1 \subseteq G\) there exists an element \(g \in G\) with \(gL_1 g^{1} \subseteq L\) ([Ho81, Thm. VIII.4.3]).
Symmetric and orthogonal Euler elements
Definition 3.1
A pair (h, x) of Euler elements is called orthogonal if \(\sigma _h(x) =  x\) (cf. Definition 2.4).
Proposition 3.2
The following assertions hold:

(i)
An Euler element \(h \in \mathfrak{g }\) is symmetric, i.e., \(h \in \mathcal{O }_h\), if and only if h is contained in a Levi complement \(\mathfrak{s }\) and h is a symmetric Euler element in \(\mathfrak{s }\).

(ii)
Let \(\mathfrak{g }= \mathfrak{r }\rtimes \mathfrak{s }\) be a Levi decomposition.

(a)
If \(h \in \mathfrak{g }\) is a symmetric Euler element, then \(\mathcal{O }_h = {\mathrm{Inn}}(\mathfrak{g })(\mathcal{O }_h \cap \mathfrak{s }) = \mathcal{O }_{q(h)}\), where \(q :\mathfrak{g }\rightarrow \mathfrak{s }\) is the projection map.

(b)
Two symmetric Euler elements are conjugate under \({\mathrm{Inn}}(\mathfrak{g })\) if and only if their images in \(\mathfrak{s }\) are conjugate under \({\mathrm{Inn}}(\mathfrak{s })\).

(a)
Proof
(i) As \(\mathcal{O }_h \subseteq h + [\mathfrak{g },\mathfrak{g }]\) follows from the invariance of the affine subspace \(h + [\mathfrak{g },\mathfrak{g }]\) under \({\mathrm{Inn}}(\mathfrak{g })\), the relation \(h \in \mathcal{O }_h\) implies \(h \in [\mathfrak{g },\mathfrak{g }]\). Let \(\mathfrak{g }= \mathfrak{r }\rtimes \mathfrak{s }\) be a Levi decomposition of \(\mathfrak{g }\). As \(\mathfrak{s }= [\mathfrak{s },\mathfrak{s }]\), the commutator algebra is adapted to this decomposition:
Now h is an Euler element in the ideal \([\mathfrak{g },\mathfrak{g }] = [\mathfrak{g }, \mathfrak{r }] \rtimes \mathfrak{s }\). This is the Lie algebra of an algebraic group for which \([\mathfrak{g },\mathfrak{r }]\) is the Lie algebra of the unipotent radical and \(\mathfrak{s }\) the Lie algebra of a reductive complement ([Ho81, Thm. VIII.3.3]). As the algebraic group generated by \(\exp (\mathbb{R }{\mathrm{ad}}h)\) is reductive, the conjugacy of Levi decompositions ([Ho81, Thm. VIII.4.3]) implies that \({\mathrm{ad}}h\) is contained in some Levi complement \({\mathrm{ad}}\mathfrak{s }\) of \({\mathrm{ad}}([\mathfrak{g },\mathfrak{g }]) = [{\mathrm{ad}}\mathfrak{g },{\mathrm{ad}}\mathfrak{g }]\). Replacing h by another element in \(\mathcal{O }_h\), we may thus assume that \(h \in \mathfrak{z }(\mathfrak{g }) + \mathfrak{s }\) for some Levi complement \(\mathfrak{s }\) of \(\mathfrak{g }\). Then \(\mathfrak{r }\) and \(\mathfrak{s }\) are \({\mathrm{ad}}h\)invariant, so that the \({\mathrm{ad}}h\)eigenspaces of the restrictions satisfy
and define 3gradings of \(\mathfrak{r }\) and \(\mathfrak{s }\). Further \(\mathfrak{g }_{\pm 1}(h) \subseteq [h,\mathfrak{g }] \subseteq [\mathfrak{g },\mathfrak{g }]\) and \(\mathfrak{s }= [\mathfrak{s },\mathfrak{s }] \subseteq [\mathfrak{g },\mathfrak{g }]\) imply that \(\mathfrak{g }= \mathfrak{r }_0(h) + [\mathfrak{g },\mathfrak{g }]\). As \([\mathfrak{g },\mathfrak{g }]\) is an ideal and \(\mathfrak{r }_0(h)\) a subalgebra of \(\mathfrak{g }\), the subgroup \({\mathrm{Inn}}_\mathfrak{g }([\mathfrak{g },\mathfrak{g }])\) of \({\mathrm{Inn}}(\mathfrak{g })\) is normal, and \({\mathrm{Inn}}(\mathfrak{g }) = {\mathrm{Inn}}_\mathfrak{g }([\mathfrak{g },\mathfrak{g }]) {\mathrm{Inn}}(\mathfrak{r }_0(h))\). As \({\mathrm{Inn}}(\mathfrak{r }_0(h))\) fixes h, this in turn shows that \(\mathcal{O }_h = {\mathrm{Inn}}_\mathfrak{g }([\mathfrak{g },\mathfrak{g }])h = {\mathrm{Inn}}_\mathfrak{g }([\mathfrak{g },\mathfrak{r }]) {\mathrm{Inn}}_\mathfrak{g }(\mathfrak{s })h\). Writing \(h = h_z + h_s\) with \(h_z \in \mathfrak{z }(\mathfrak{g })\) and \(h_s \in \mathcal{E }(\mathfrak{s })\), we thus find \(x \in [\mathfrak{g },\mathfrak{r }]\) and \(s \in {\mathrm{Inn}}_\mathfrak{g }(\mathfrak{s })\) such that^{Footnote 8}
Applying the Lie algebra homomorphism q to both sides, we derive from \(q(h_z) = 0\) and \(q \circ e^{{\mathrm{ad}}x} = q\) that \(h_s = s.h_s\), and therefore
We conclude that the unipotent linear map \(e^{{\mathrm{ad}}x}\) preserves the linear subspace \(\mathbb{R }h_s + \mathbb{R }h_z\), and this implies that \({\mathrm{ad}}x = \log (e^{{\mathrm{ad}}x})\) also has this property. We thus arrive at
so that we must have \(x \in \mathfrak{g }_0(h) = \mathfrak{g }_0(h_s)\), which in turn leads to \(0 = e^{{\mathrm{ad}}x}h_s  h_s = 2h_z\), i.e., \(h = h_s\in \mathfrak{s }\).
To prove the second assertion of (i), we observe that the homomorphism \(q :\mathfrak{g }\rightarrow \mathfrak{s }\cong \mathfrak{g }/\mathfrak{r }\) satisfies
Hence \(q(\mathcal{E }_{\mathrm{sym}}(\mathfrak{g })) \subseteq \mathcal{E }_{\mathrm{sym}}(\mathfrak{s })\). If, conversely, \(h \in \mathcal{E }_{\mathrm{sym}}(\mathfrak{s })\), then we clearly have \(h \in {\mathrm{Inn}}_\mathfrak{g }(\mathfrak{s })h \subseteq {\mathrm{Inn}}(\mathfrak{g })h\), so that \(h \in \mathcal{E }_{\mathrm{sym}}(\mathfrak{g })\).
(ii)(a) As \(\mathcal{O }_h\) intersects \(\mathfrak{s }\) by (i), \(q(\mathcal{O }_h) \cap \mathcal{O }_h \not =\emptyset \), and since \({\mathrm{Inn}}(\mathfrak{s })\) acts transitively on \(q(\mathcal{O }_h)\) by (3.2), we obtain \(q(\mathcal{O }_h) \subseteq \mathcal{O }_h\) and thus \(q(\mathcal{O }_h) = \mathcal{O }_h \cap \mathfrak{s }\). This further leads to
(ii)(b) follows immediately from (a). \(\square \)
Proposition 3.2 reduces the description of symmetric Euler elements up to conjugation by inner automorphisms to the case of simple Lie algebras.
Remark 3.3
Suppose that \(\mathfrak{g }\) is a finite dimensional Lie algebra containing a pointed generating invariant cone C. If \(\mathfrak{g }\) is not reductive, then \(C \cap \mathfrak{z }(\mathfrak{g }) \not =\{0\}\) ([Ne99, Thm. VII.3.10]). If \(\tau = \sigma _h\) is an involution defined by a symmetric Euler element h, then \(\tau \) fixes every central element, so that we cannot have \(\tau (C) =  C\) if \(\mathfrak{g }\) is not reductive.
Examples 3.4
(a) If \(\mathfrak{s }\) is a semisimple Lie algebra and \(h \in \mathfrak{s }\) an Euler element, then it also is an Euler element in the semidirect sum \(T\mathfrak{s }:= \mathfrak{s } \rtimes \mathfrak{s }\), where \(\mathfrak{s }\) is the linear subspace underlying \(\mathfrak{s }\), endowed with the \(\mathfrak{s }\)module structure defined by the adjoint representation.
(b) In the simple Lie algebra \(\mathfrak{g }:= {\mathfrak{sl }}_n(\mathbb{R })\), we write \(n \times n\)matrices as block \(2 \times 2\)matrices according to the partition \(n = k + (nk)\). Then
is diagonalizable with the two eigenvalue \(\frac{nk}{n} = 1  \frac{k}{n}\) and \(\frac{k}{n}\). Therefore \(h_k\) is an Euler element whose 3grading is given by
Example 3.5
For \(\mathfrak{g }= {\mathfrak{sl }}_2(\mathbb{R })\), the Euler element
Any element in \({\mathrm{Fix}}(\sigma _h)\) is of the form \(x = \begin{pmatrix} 0 &{} \quad b \\ c &{} \quad 0 \end{pmatrix},\) and it is an Euler element if and only if \(bc =  \det (x) = \frac{1}{4}\). If \(g \in {\mathrm{SL}}_2(\mathbb{R })\) commutes with h, then it is diagonal, i.e., \(g = \begin{pmatrix} a &{} \quad 0 \\ 0 &{} \quad a^{1} \end{pmatrix}\), and thus
We thus obtain two representatives
of conjugacy classes of orthogonal pairs (h, x) of Euler elements for \({\mathfrak{sl }}_2(\mathbb{R })\). The involution corresponding to \(x_\pm \) is given by
which shows in particular that
As a consequence of the preceding discussion, we see that the orthogonality relation on \(\mathcal{E }({\mathfrak{sl }}_2(\mathbb{R }))\) is symmetric:
Lemma 3.6
If (x, y) is an orthogonal pair of Euler elements in \({\mathfrak{sl }}_2(\mathbb{R })\), then \(\sigma _y(x) = x\), so that (y, x) is also orthogonal.
Example 3.7
For \(\mathfrak{g }= {\mathfrak{gl }}_2(\mathbb{R })\), the Euler element
and we see, as for \({\mathfrak{sl }}_2(\mathbb{R })\), that the orthogonal Euler elements are given by
This shows that
Therefore \({\mathfrak{gl }}_2(\mathbb{R })\) contains a pair (h, x) of orthogonal Euler elements for which \(\sigma _x(h) \not = h\). From \(h \not \in [\mathfrak{g },\mathfrak{g }]\) it immediately follows that h is not symmetric. We shall see in Theorem 3.13 below that this pathology of the orthogonality relation on the set of Euler elements does not occur for symmetric Euler elements.
Example 3.8
For \(\mathfrak{g }= {\mathfrak{sl }}_3(\mathbb{R })\), the Euler element
where we write matrices as \(2 \times 2\)block matrices according to the partition \(3 = 1 + 2\). Up to conjugacy under the centralizer of \(h_1\), the symmetric matrices in \({\mathrm{Fix}}(\sigma _{h_1})\) are represented by
These matrices have three different eigenvalues, so that \({\mathrm{ad}}x\) has five eigenvalues, and thus x cannot be an Euler elements of \({\mathfrak{sl }}_3(\mathbb{R })\). We conclude that there exists no Euler element \(x \in \mathcal{E }({\mathfrak{sl }}_3(\mathbb{R }))\) for which \((h_1,x)\) is orthogonal.
We shall see in Theorem 3.13(b) below that this never happens for symmetric Euler elements, but \(h_1\) is not symmetric. It corresponds to \(h_1\) for the root system \(A_2\) in the notation of Section 3.3.
Example 3.9
For \(\mathfrak{g }= {\mathfrak{sl }}_4(\mathbb{R })\), the Euler element
where we write matrices as \(2 \times 2\)block matrices according to the partition \(4 = 1 + 3\). Up to conjugacy under the centralizer of \(h_1\), the symmetric matrices in \({\mathrm{Fix}}(\sigma _{h_1})\) are represented by
They all have three different eigenvalues and \({\mathrm{ad}}x\) has five eigenvalues, so that they are not Euler elements. We conclude that there exists no Euler element \(x \in \mathcal{E }({\mathfrak{sl }}_4(\mathbb{R }))\) for which \((h_1,x)\) is orthogonal.
This is different for the symmetric Euler element
where we write matrices as \(2 \times 2\)block matrices according to the partition \(4 = 2 + 2\). Up to conjugacy under the centralizer of \(h_2\), the symmetric matrices in \({\mathrm{Fix}}(\sigma _{h_2})\) are represented by
and, for \(a = b = {\textstyle {\frac{1}{2}}}\), these are Euler elements orthogonal to \(h_2\).
Euler elements in simple real Lie algebras
In this section we take a systematic look at Euler elements in simple real Lie algebras. In particular we determine which of them are symmetric and show that pairs of orthogonal ones generate \({\mathfrak{sl }}_2\)subalgebras (Theorem 3.13). For the classification of 3gradings of simple Lie algebras, we refer to [KA88], the concrete list of the 18 types in [Kan98, p. 600] which is also listed below, and Kaneyuki’s lecture notes [Kan00].
Let \(\mathfrak{g }\) is a real semisimple Lie algebra. An involutive automorphism \(\theta \in {\mathrm{Aut}}(\mathfrak{g })\) is called a Cartan involution if its eigenspaces
have the property that they are orthogonal with respect to \(\kappa \), which is negative definite on \(\mathfrak{k }\) and positive definite on \(\mathfrak{p }\). Then
is called a Cartan decomposition. Cartan involutions always exist and two such involutions are conjugate under the group \({\mathrm{Inn}}(\mathfrak{g })\) of inner automorphism, so they produce isomorphic decompositions ([HN12, Thm. 13.2.11]).
If \(\mathfrak{g }= \mathfrak{k }\oplus \mathfrak{p }\) is a Cartan decomposition, then \(\mathfrak{k }\) is a maximal compactly embedded subalgebra of \(\mathfrak{g }\), \(x \in \mathfrak{g }\) is elliptic if and only if its adjoint orbit \(\mathcal{O }_x ={\mathrm{Inn}}(\mathfrak{g })x\) intersects \(\mathfrak{k }\), and \(x \in \mathfrak{g }\) is hyperbolic if and only if \(\mathcal{O }_x \cap \mathfrak{p }\not =\emptyset \).
For the finer structure theory, and also for classification purposes, one starts with a Cartan involution \(\theta \) and fixes a maximal abelian subspace \(\mathfrak{a }\subseteq \mathfrak{p }\). As \(\mathfrak{a }\) is abelian, \({\mathrm{ad}}\mathfrak{a }\) is a commuting set of diagonalizable operators, hence simultaneously diagonalizable. For a linear functional \(0 \not =\alpha \in \mathfrak{a }^*\), the simultaneous eigenspaces
are called root spaces and
is called the set of restricted roots. We pick a set
of simple roots. This is a subset with the property that every root \(\alpha \in \Sigma \) is a linear combination \(\alpha = \sum _{j =1}^n n_j \alpha _j\), where the coefficients are either all in \(\mathbb{Z }_{\ge 0}\) or in \(\mathbb{Z }_{\le 0}\). The convex cone
is called the positive (Weyl) chamber corresponding to \(\Pi \).
We have the root space decomposition
Now \(\theta (\mathfrak{g }_\alpha ) = \mathfrak{g }_{\alpha }\), and for a nonzero element \(x_\alpha \in \mathfrak{g }_\alpha \), the 3dimensional subspace spanned by \(x_\alpha , \theta (x_\alpha )\) and \([x_\alpha , \theta (x_\alpha )] \in \mathfrak{a }\) is a Lie subalgebra isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\). In particular, it contains a unique element \(\alpha ^\vee \in \mathfrak{a }\) with \(\alpha (\alpha ^\vee ) = 2\). Then
is a reflection, and the subgroup
is called the Weyl group. Its action on \(\mathfrak{a }\) provides a good description of the adjoint orbits of hyperbolic elements: Every hyperbolic element in \(\mathfrak{g }\) is conjugate to a unique element in \(\Pi ^\star \) and, for \(x \in \mathfrak{a }\), the intersection \(\mathcal{O }_x \cap \mathfrak{a }= \mathcal{W }x\) is the Weyl group orbit ([KN96, Thm. III.10]).
From now on we assume that \(\mathfrak{g }\) is simple. Then \(\Sigma \) is an irreducible root system, hence of one of the following types:
(cf. [Bo90a]). If \(\mathfrak{g }\) is a complex simple Lie algebra, then it is also simple as a real Lie algebra, and a Cartan decomposition takes the form
where \(\mathfrak{k }\subseteq \mathfrak{g }\) is a compact real form. Then \(\mathfrak{a }= i \mathfrak{t }\), where \(\mathfrak{t }\subseteq \mathfrak{k }\) is maximal abelian. In particular, the restricted root system \(\Sigma (\mathfrak{g },\mathfrak{a })\) coincides with the root system of the complex Lie algebra \(\mathfrak{g }\). This leads to a onetoone correspondence between isomorphy classes of simple complex Lie algebras and the irreducible reduced root systems. If \(\mathfrak{g }\) is not complex, then neither the isomorphy class of \(\mathfrak{g }\) nor of \(\mathfrak{g }_\mathbb{C }\) is determined by the root system \(\Sigma (\mathfrak{g },\mathfrak{a })\). For instance all Lie algebras \({\mathfrak{so }}_{1,n}(\mathbb{R })\) have the restricted root system \(A_1\) with \({\mathrm{dim}}\mathfrak{a }= 1\), but their complexifications \({\mathfrak{so }}_{n+1}(\mathbb{C })\) have the root systems \(B_k\) for \(n = 2k\) and \(D_k\) for \(n = 2k1\).
The adjoint orbit of an Euler element in \(\mathfrak{g }\) contains a unique \(h \in \Pi ^\star \). For any Euler element \(h \in \Pi ^\star \), we have \(\alpha (h) \in \{0,1\}\) for \(\alpha \in \Pi \) because the values of the roots on h are the eigenvalues of \({\mathrm{ad}}h\). If such an element exists, then the irreducible root system \(\Sigma \) must be reduced. Otherwise, for any root \(\alpha \) with \(2\alpha \in \Sigma \), we must have \(\alpha (h) = 0\) because \({\mathrm{ad}}x\) has only three eigenvalues. As the set of such roots generates the same linear space as \(\Sigma \), this leads to the contradiction \(h = 0\). This excludes the nonreduced simple root systems of type \(BC_n\).
To see how many possibilities we have for Euler elements in \(\mathfrak{a }\), we recall that \(\Pi \) is a linear basis of \(\mathfrak{a }\), so that, for each \(j \in \{1,\ldots , n\}\), there exists a uniquely determined element
A simple Lie algebra \(\mathfrak{g }= \mathfrak{k }\oplus \mathfrak{p }\) is called hermitian if the center
of a maximal compactly embedded subalgebra \(\mathfrak{k }\) is nonzero. For hermitian Lie algebras, the restricted root system \(\Sigma \) is either of type \(C_r\) or \(BC_r\) (cf. Harish Chandra’s Theorem [Ne99, Thm. XII.1.14]), and we say that \(\mathfrak{g }\) is of tube type if the restricted root system is of type \(C_r\).
The following theorem lists for each irreducible root system \(\Sigma \) the possible Euler elements in the positive chamber \(\Pi ^\star \). Since every adjoint orbit in \(\mathcal{E }(\mathfrak{g })\) has a unique representative in \(\Pi ^\star \), this classifies the \({\mathrm{Inn}}(\mathfrak{g })\)orbits in \(\mathcal{E }(\mathfrak{g })\) for any noncompact simple real Lie algebra. For semisimple algebras \(\mathfrak{g }= \mathfrak{g }_1 \oplus \cdots \oplus \mathfrak{g }_k\), an element \(x = (x_1, \ldots , x_{k})\) is an Euler element if and only if its components \(x_j \in \mathfrak{g }_j\) are Euler elements, and its orbit is
Therefore it suffices to consider simple Lie algebras, and for these the root system \(\Sigma \) is irreducible. As every complex simple Lie algebra \(\mathfrak{g }\) is also a real simple Lie algebra, our discussion also covers complex Lie algebras.
Theorem 3.10
Suppose that \(\mathfrak{g }\) is a noncompact simple real Lie algebra, with restricted root system \(\Sigma \subseteq \mathfrak{a }^*\) of type \(X_n\). We follow the conventions of the tables in [Bo90a] for the classification of irreducible root systems and the enumeration of the simple roots \(\alpha _1, \ldots , \alpha _n\). Then every Euler element \(h \in \mathfrak{a }\) on which \(\Pi \) is nonnegative is one of \(h_1, \ldots , h_n\), and for every irreducible root system, the Euler elements among the \(h_j\) are the following:
For the root systems \(BC_n\), \(E_8\), \(F_4\) and \(G_2\) no Euler element exists (they have no 3grading). The symmetric Euler elements are
Proof
Writing the highest root in \(\Sigma \) with respect to the simple system \(\Pi \) as \(\alpha _{\mathrm{max}} = \sum _{j = 1}^n c_j \alpha _j\), we have \(c_j \in \mathbb{Z }_{>0}\) for each j. If \(h \in \Pi ^\star \) is an Euler element, then \(\Pi (h) \subseteq \{0,1\}\), and \(1 = \alpha _{\mathrm{max}}(h) = \sum _{j = 1}^n c_j \alpha _j(h)\) implies that at most one value \(\alpha _j(h)\) can be 1, and then the others are 0, i.e., \(h = h_j\) for some \(j \in \{1,\ldots , n\}\). Moreover, \(h_j\) is an Euler element if and only if \(c_j = 1\). Consulting the tables on the irreducible root systems in [Bo90a], we obtain the Euler elements listed in (3.7).
To determine the symmetric ones, let \(w_0 \in \mathcal{W }\) be the longest element of the Weyl group, which is uniquely determined by \(w_0^*\Pi =  \Pi \) for the dual action of \(\mathcal{W }\) on \(\mathfrak{a }^*\). Then \(h_j' := w_0(h_j)\) is the Euler element in the positive chamber representing the orbit \(\mathcal{O }_{h_j}\). Therefore \(h_j\) is symmetric if and only if \(h_j \in \mathcal{W }h_j\), which is equivalent to \(h_j' = h_j\). Using the description of \(w_0\) and the root systems in [Bo90a], now leads to
Hence the symmetric Euler elements are given by the list (3.8). \(\square \)
This theorem requires some interpretation. So let us first see what it says about complex simple Lie algebras \(\mathfrak{g }\). In (3.7) we see that only if \(\mathfrak{g }\) is not of type \(E_8, F_4\) or \(G_2\), the Lie algebra \(\mathfrak{g }\) contains an Euler element. Euler elements correspond to 3gradings of the root system and these in turn to hermitian real forms \(\mathfrak{g }^\circ \), where \(ih_j \in \mathfrak{z }(\mathfrak{k }^\circ )\) generates the center of a maximal compactly embedded subalgebra \(\mathfrak{k }^\circ \) ([Ne99, Thm. A.V.1]). We thus obtain the following possibilities. In Table 1, we write \(\mathfrak{g }^\circ \) for the hermitian real form, \(\mathfrak{g }\) for the complex Lie algebra, \(\Sigma \) for its root system, and \(h_j\) for the corresponding Euler element:
Note that \({\mathfrak{sl }}_2(\mathbb{R }) \cong {\mathfrak{so }}_{2,1}(\mathbb{R }) \cong {\mathfrak{su }}_{1,1}(\mathbb{C })\). More expectional isomorphisms are discussed in some detail in [HN12, Sect. 17].
In this correspondence, those hermitian simple Lie algebras corresponding to symmetric Euler elements are of particular interest. Comparing with the list of hermitian simple Lie algebras of tube type (cf. [FK94, p. 213]), we see that they correspond precisely to the 3gradings specified by symmetric Euler elements, as listed in (3.8). Since the Euler elements \(h_{n1}\) and \(h_n\) for the root system of type \(D_n\) are conjugate under a diagram automorphism, they correspond to isomorphic hermitian real forms.
In our context hermitian simple Lie algebras are of particular interest. We therefore collect some of their main properties in the following proposition.
Proposition 3.11
For a simple real Lie algebra, the following assertions hold:

(a)
\(\mathfrak{g }\) is hermitian if and only if there exists a closed convex \({\mathrm{Inn}}(\mathfrak{g })\)invariant cone \(C \not = \{0\},\mathfrak{g }\).

(b)
A simple hermitian Lie algebra contains an Euler element if and only if it is of tube type, and in this case \({\mathrm{Inn}}(\mathfrak{g })\) acts transitively on \(\mathcal{E }(\mathfrak{g })\).
Proof
(a) is a consequence of the Kostant–Vinberg Theorem (cf. [HÓ96, Lemma 2.5.1]).
(b) Since the restricted root system of a hermitian simple Lie algebra is of type \(C_r\) or \(BC_r\), and the first case characterizes the algebras of tube type, the assertion follows from Theorem 3.10 because \(C_r\) only permits one class of Euler elements. \(\square \)
There are many types of simple 3graded Lie algebras that are neither complex nor hermitian of tube type; for instance the Lorentzian algebras \({\mathfrak{so }}_{1,n}(\mathbb{R })\). We refer to [Kan98, p. 600] or [Kan00]. for the list of all 18 types which is reproduced below.
Remark 3.12
As \(h \in \mathfrak{a }\) implies \(\theta (h) = h\), the Cartan involution \(\theta \) always maps h into \(h\), but this only implies that h is symmetric if \(\theta \in {\mathrm{Inn}}(\mathfrak{g })\). This is the case if \(\mathfrak{g }\) is hermitian, so that in these Lie algebras all Euler elements are symmetric.
We conclude this section with some finer results concerning orthogonality and symmetry of Euler elements.
Theorem 3.13
If \(\mathfrak{g }\) is simple and \(h \in \mathcal{E }(\mathfrak{g })\), then the following assertions hold:

(a)
If \(x \in \mathcal{E }(\mathfrak{g })\) is such that (h, x) is orthogonal, then

(i)
h and x are symmetric,

(ii)
the Lie algebra generated by h and x is isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\), and

(iii)
\(\sigma _x(h) = h\), so that (x, h) is also orthogonal.

(i)

(b)
There exists an Euler element x such that (h, x) is orthogonal if and only if h is symmetric.
Proof
(a) We split the proof into the two cases, according to whether \(\mathfrak{g }\) is a complex Lie algebra or not. We then reduce the second case to the first one.
Case 1: \(\mathfrak{g }\) is complex: A simple complex Lie algebra \(\mathfrak{g }\) contains an Euler element, i.e., it possesses a 3graded root system, if and only if it has a real form \(\mathfrak{g }^\circ \) which is hermitian, i.e., \(\mathfrak{g }= (\mathfrak{g }^\circ )_\mathbb{C }= \mathfrak{g }^\circ \oplus i \mathfrak{g }^\circ \). This follows for example by comparing the list of irreducible root systems for which Euler elements exist (see (3.7)) with the classification of hermitian simple Lie algebras \(\mathfrak{g }^\circ \) (see [Ne99, Thm. A.V.1] and Table 1). In this case the real Lie algebra \(\mathfrak{g }^\circ \) has a Cartan decomposition \(\mathfrak{g }^\circ = \mathfrak{k }^\circ \oplus \mathfrak{p }^\circ \) and the center \(\mathfrak{z }(\mathfrak{k }^\circ )\) is onedimensional and generated by an element z with \({\mathrm{Spec}}({\mathrm{ad}}z) = \{0,\pm i\}\) ([Ne99, Thm. A.V.1]). Then \(h = i z\) is an Euler element in the complexification \(\mathfrak{g }\) for which \(\mathfrak{k }^\circ = \ker ({\mathrm{ad}}z) \cap \mathfrak{g }^\circ \) and \([z,\mathfrak{g }^\circ ] = \mathfrak{p }^\circ \), where \({\mathrm{ad}}z\vert _{\mathfrak{p }^\circ }\) is a complex structure on the real vector space \(\mathfrak{p }^\circ \). The corresponding Euler involution \(\sigma _h = e^{\pi i {\mathrm{ad}}h} = e^{\pi {\mathrm{ad}}z} \in {\mathrm{Aut}}_\mathbb{C }(\mathfrak{g })\) thus restricts to the Cartan involution on \(\mathfrak{g }^\circ \), corresponding to the decomposition \(\mathfrak{k }^\circ \oplus \mathfrak{p }^\circ \). Accordingly, we obtain
A Cartan decomposition of \(\mathfrak{g }\) is obtained by \(\mathfrak{k }= \mathfrak{k }^\circ + i \mathfrak{p }^\circ \) and \(\mathfrak{p }= \mathfrak{p }^\circ + i \mathfrak{k }^\circ \). If \(\mathfrak{t }\subseteq \mathfrak{k }^\circ \) is a maximal abelian Lie subalgebra, then \(\mathfrak{a }:= i \mathfrak{t }\subseteq \mathfrak{p }\) is a maximal abelian subspace which contains \(h = i z \in i \mathfrak{z }(\mathfrak{k }^\circ ) \subseteq i\mathfrak{t }\). The orthogonality of the pair (h, x) means that \(x \in \mathfrak{q }= {\mathrm{Fix}}(\sigma _h)\). By [KN96, Cor. III.9], \(x \in \mathcal{E }(\mathfrak{g }) \cap \mathfrak{q }\) is conjugate under the centralizer of h to an element in \(\mathfrak{q }\cap \mathfrak{p }= \mathfrak{p }^\circ \). Fixing a maximal abelian subspace \(\mathfrak{a }^\circ \subseteq \mathfrak{p }^\circ \), we may therefore assume that x is an Euler element for the corresponding restricted root system \(\Sigma ^\circ := \Sigma (\mathfrak{g }^\circ , \mathfrak{a }^\circ ) \subseteq (\mathfrak{a }^\circ )^*\), which is of type \(C_r\) or \(BC_r\) (cf. [Ne99, Thm. XII.1.14]). As we have already observed above, the existence of an Euler element \(x \in \mathfrak{a }^\circ \) implies that the restricted root system \(\Sigma ^\circ \) is reduced, which excludes the case \(BC_r\). Therefore \(\mathfrak{g }^\circ \) is of tube type (cf. Proposition 3.11) and Table 2 thus implies that h is symmetric.
The fact that \(\mathfrak{g }^\circ \) is of tube type implies that \(x \in \mathfrak{a }^\circ \) corresponds to the unique Euler element \(h_r\) for the restricted root system \(\Sigma ^\circ \) of type \(C_r\) (see (3.7)). From (3.8) it now follows that x is symmetric (see also Proposition 3.11). This proves (i).
To verify (ii) and (iii), we observe that the root system \(C_r\) contains the maximal subset \(\{2 \varepsilon _1, \ldots , 2 \varepsilon _r\}\) of strongly orthogonal roots, i.e., neither sums nor differences of these roots are roots. The multiplicities of these restricted roots are 1 ([Ne99, Thm. XII.1.14]), and
(cf. [Ne99, Lemma XII.1.11], [Ta79, p. 12]). As the roots \(2\varepsilon _j\) all take the value 1 on the Euler element \(x \in \mathfrak{a }^\circ \), we have \(x = {\textstyle {\frac{1}{2}}}\sum _{j =1}^r (2\varepsilon _j)^\vee \), which is the diagonal element in \({\mathfrak{sl }}_2(\mathbb{R })^r\), corresponding to \(\begin{pmatrix} {\textstyle {\frac{1}{2}}}&{} \quad 0 \\ 0 &{} \quad {\textstyle {\frac{1}{2}}} \end{pmatrix}\). Likewise, ih is contained in \(\mathfrak{s }\cong {\mathfrak{sl }}_2(\mathbb{R })^r\) as the diagonal element corresponding to \(\begin{pmatrix} 0 &{} \quad {\textstyle {\frac{1}{2}}}\\ {\textstyle {\frac{1}{2}}}&{} \quad 0 \end{pmatrix}\). As the Lie subalgebra of \({\mathfrak{gl }}_2(\mathbb{C })\), generated by
is isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\), the same holds for the real Lie subalgebra of \(\mathfrak{g }\) generated by h and x. Now (ii) and (iii) follow from Lemma 3.6.
Case 2: \(\mathfrak{g }\) is not complex: Then \(\mathfrak{g }_\mathbb{C }\) is a simple complex Lie algebra to which all arguments in Case 1 apply. In particular, the real Lie subalgebra \(\mathfrak{s }\) spanned by h, x and [h, x] is isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\). This proves (ii) and (iii). As \(\mathfrak{s }\subseteq \mathfrak{g }\) and all Euler elements in \({\mathfrak{sl }}_2(\mathbb{R })\) are symmetric, we also obtain (i).
(b) If there exists an Euler element x for which (h, x) is orthogonal, then (a)(i) implies that h is a symmetric Euler element. Suppose, conversely, that h is a symmetric Euler element. For a Cartan involution \(\theta \) with \(\theta (h) = h\), we choose a maximal abelian subspace \(\mathfrak{a }\subseteq \mathfrak{p }= {\mathrm{Fix}}(\theta )\) containing h and choose in the subset
a maximal set \(\{ \gamma _1, \ldots , \gamma _r\}\) of strongly orthogonal roots (cf. [Ta79, p.13] or [Kan00, p. 134]). From these references we further infer the existence of elements \(e_j \in \mathfrak{g }_{\gamma _j}\) such that, for each j, the subalgebra \(\mathfrak{s }_j := {\mathrm{span}}_\mathbb{R }\{e_j, \theta (e_j), [e_j, \theta (e_j)]\}\) is isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\). We normalize \(e_j\) in such a way that \(x_j := e_j  \theta (e_j)\) is an Euler element of \(\mathfrak{s }_j\). Then loc. cit. further implies that
is maximal abelian in \(\mathfrak{q }_\mathfrak{p }= \mathfrak{q }\cap \mathfrak{p }\) for \(\mathfrak{q }:= \mathfrak{g }^{\sigma _h}\). Since h is a symmetric Euler element and the root system \(\Sigma (\mathfrak{g },\mathfrak{a })\) is irreducible, h corresponds to some \(h_j\) in the list (3.8). The restricted root system \(\Sigma (\mathfrak{g },\mathfrak{a }_\mathfrak{q })\) is always of type \(C_r\). The explicit description of the restricted roots in [Kan98, p. 596] now implies that \(x := \sum _{j = 1}^r x_j \in \mathfrak{a }_\mathfrak{q }\) is an Euler element. By construction, it satisfies \(\sigma _h(x) = x\), so that (h, x) is orthogonal. This completes the proof. \(\square \)
Corollary 3.14
Let \(\mathfrak{g }\) be a finite dimensional Lie algebra and (h, x) be orthogonal Euler elements such that h is also symmetric. Then the following assertions hold:

(a)
There exists a Levi complement containing h and x.

(b)
The Lie algebra generated by h and x is isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\).

(c)
(x, h) is also orthogonal.
Proof
By Proposition 3.2(i), there exists a Levi decompositions \(\mathfrak{g }= \mathfrak{r }\rtimes \mathfrak{s }\) with \(h \in \mathfrak{s }\). We then have for \(\mathfrak{q }:= {\mathrm{Fix}}(\sigma _h)\) the decompositions
and \(x \in \mathfrak{q }\) is an Euler element, hence in particular hyperbolic. Let \(\mathfrak{a }_\mathfrak{r }\subseteq \mathfrak{q }_\mathfrak{r }\) be a maximal hyperbolic subspace, i.e., \(\mathfrak{a }_\mathfrak{r }\) is abelian, consists of \({\mathrm{ad}}\)diagonalizable elements and is maximal with respect to this property. Then \(\mathfrak{a }_\mathfrak{r }\subseteq [h,\mathfrak{r }] \subseteq [\mathfrak{g },\mathfrak{r }]\) consists also of \({\mathrm{ad}}\)nilpotent elements, hence is central. As \({\mathrm{ad}}h\vert _\mathfrak{q }\) is injective, it follows that \(\mathfrak{a }_\mathfrak{r }= \{0\}\). By [KN96, Prop. III.5], \(\mathfrak{q }_\mathfrak{s }\) contains a maximal hyperbolic subspace \(\mathfrak{a }\) of \(\mathfrak{q }\) and x is conjugate under \({\mathrm{Inn}}_\mathfrak{g }(\mathfrak{h })\) to an element of \(\mathfrak{a }\subseteq \mathfrak{q }_\mathfrak{s }\). This proves(a).
(b) In view of (a), we may w.l.o.g. assume that \(\mathfrak{g }\) is semisimple, and by Theorem 3.13, which applies to each simple ideal, even that \(\mathfrak{g }\cong {\mathfrak{sl }}_2(\mathbb{R })^r\) for some \(r \in \mathbb{N }\). As \({\mathrm{Aut}}({\mathfrak{sl }}_2(\mathbb{R }))\cong {\mathrm{PGL}}_2(\mathbb{R })\) acts transitively on the set of orthogonal pairs of Euler elements in \({\mathfrak{sl }}_2(\mathbb{R })\) (Example 3.5), we may further assume that
so that the Lie subalgebra generated by x and h is the diagonal in \({\mathfrak{sl }}_2(\mathbb{R })^r\), hence isomorphic to \({\mathfrak{sl }}_2(\mathbb{R })\).
(c) follows directly from (b) and Lemma 3.6. \(\square \)
Covariant Nets of Real Subspaces
In this section we develop an axiomatic setting for covariant nets of standard subspaces parametrized by \(G^{{\uparrow }}\)orbits in \(\mathcal{G }_E(G)\).
Standard subspaces
Here we collect some fundamental notions concerning real subspaces of a complex Hilbert space \(\mathcal{H }\) with scalar product \(\langle \cdot ,\cdot \rangle \), linear in the second argument. We call a closed real subspace \(\mathsf{H}\subseteq \mathcal{H }\) cyclic if \(\mathsf{H}+i\mathsf{H}\) is dense in \(\mathcal{H }\), separating if \(\mathsf{H}\cap i\mathsf{H}=\{0\}\), and standard if it is cyclic and separating. The symplectic “complement” of a real subspace \(\mathsf{H}\) is defined by the symplectic form \({\mathrm{Im}}\langle \cdot ,\cdot \rangle \), namely
Note that \(\mathsf{H}\) is separating if and only if \(\mathsf{H}'\) is cyclic, hence \(\mathsf{H}\) is standard if and only if \(\mathsf{H}'\) is standard. For a standard subspace \(\mathsf{H}\), we define the Tomita operator as the closed antilinear involution
The polar decomposition \(S_\mathsf{H}=J_\mathsf{H}\Delta _\mathsf{H}^{\frac{1}{2}}\) defines an antiunitary involution \(J_\mathsf{H}\) and the modular operator \(\Delta _\mathsf{H}\). For the modular group \((\Delta _\mathsf{H}^{it})_{t \in \mathbb{R }}\), we then have
([Lo08, Thm. 3.4]). This construction leads to a onetoone correspondence between Tomita operators and standard subspaces:
Proposition 4.1
([Lo08, Prop. 3.2]). The map \(\mathsf{H}\mapsto S_\mathsf{H}\) is a bijection between the set of standard subspaces of \(\mathcal{H }\) and the set of closed, densely defined, antilinear involutions on \(\mathcal{H }\). Moreover, polar decomposition \(S = J\Delta ^{1/2}\) defines a onetoone correspondence between such involutions and pairs \((\Delta , J)\), where J is a conjugation and \(\Delta >0\) selfadjoint with \(J\Delta J =\Delta ^{1}\).
The modular operators of symplectic complements satisfy the following relations
From Proposition 4.1 we easily deduce:
Lemma 4.2
([Mo18, Lemma 2.2]). Let \(\mathsf{H}\subset \mathcal{H }\) be a standard subspace and \(U\in {\mathrm{AU}}(\mathcal{H })\) be a unitary or antiunitary operator. Then \(U\mathsf{H}\) is also standard and \(U\Delta _\mathsf{H}U^*=\Delta _{U\mathsf{H}}^{\varepsilon (U)}\) and \(UJ_\mathsf{H}U^*=J_{U\mathsf{H}}\).
Lemma 4.3
([Lo08, Cor. 2.1.8]). Let \(\mathsf{H}\subset \mathcal{H }\) be a standard subspace, and \(\mathsf{K}\subset \mathsf{H}\) be a closed, real linear subspace of \(\mathsf{H}\). If \(\Delta _\mathsf{H}^{it}\mathsf{K}=\mathsf{K}\) for all \(t\in \mathbb{R }\), then \(\mathsf{K}\) is a standard subspace of \(\mathcal{K }:= \overline{\mathsf{K}+i\mathsf{K}}\) and \(\Delta _\mathsf{H}_\mathsf{K}\) is the modular operator of \(\mathsf{K}\) on \(\mathcal{K }\). If, in addition, \(\mathsf{K}\) is a cyclic subspace of \(\mathcal{H }\), then \(\mathsf{H}=\mathsf{K}\).
The following theorem relates positive generators and inclusions of real subspaces.
Theorem 4.4
([Lo08, Thms. 3.15, 3.17], [BGL02, Thm. 3.2]). Let \(\mathsf{H}\subset \mathcal{H }\) be a standard subspace and \(U(t)=e^{itP}\) be a unitary oneparameter group on \(\mathcal{H }\) with a generator P.

(a)
If \(\pm P > 0\) and \(U(t)\mathsf{H}\subset \mathsf{H}\) for all \(t\ge 0\), then
$$\begin{aligned} \Delta _\mathsf{H}^{is/2\pi }U(t)\Delta _\mathsf{H}^{is/2\pi } = U(e^{\pm s}t)\quad \text{ and } \quad J_{\mathsf{H}}U(t)J_{\mathsf{H}}=U(t) \quad \text{ for } \text{ all } \quad t,s \in \mathbb{R }.\nonumber \\ \end{aligned}$$(4.1) 
(b)
If \(\Delta _\mathsf{H}^{is/2\pi }U(t)\Delta _\mathsf{H}^{is/2\pi } = U(e^{\pm s}t)\) for \(s,t \in \mathbb{R }\), then the following are equivalent:

(1)
\(U(t)\mathsf{H}\subset \mathsf{H}\) for \( t\ge 0\);

(2)
\(\pm P\) is positive.

(1)
Part (a) is also called the Oneparticle Borchers Theorem. Borchers originally proved it for von Neumann algebras with a cyclic and separating vectors, see [Bo92]. Part (b) is in [BGL02].
With the notation introduced in Examples 2.10(b), we have seen that any couple \((U,\mathsf{H})\) of a oneparameter group \((U_t)_{t \in \mathbb{R }}\) with positive (resp. negative) generator and a standard subspace \(\mathsf{H}\) satisfying the assumptions of Theorem 4.4(a) defines a unitary, positive energy representation of the affine group \({\mathrm{Aff}}(\mathbb{R }) \cong \mathbb {R}\rtimes \mathbb {R}^\times \) implemented by
A representation of \({\mathrm{Aff}}(\mathbb{R })\) can also be obtained by looking at some peculiar relative positions of standard subspaces: The halfsided modular inclusions.
Definition 4.5
An inclusion \(\mathsf{K}\subseteq \mathsf{H}\) of standard subspaces of \(\mathcal{H }\) is called a ±halfsided modular inclusion (±HSMI) if
Theorem 4.6
([Lo08, Cor. 3.6.6.], [NÓ17, Thm. 3.15]). \(\mathsf{K}\subseteq \mathsf{H}\) is a positive halfsided modular inclusion if and only if there exists an (anti)unitary positive energy representation \((U,\mathcal{H })\) of \({\mathrm{Aff}}(\mathbb{R }) \cong \mathbb{R }\rtimes \mathbb{R }^\times \) with \(U(\delta (t))=\Delta _\mathsf{H}^{\frac{it}{2\pi }}\), \(U(r_0)=J_\mathsf{H}\), \(U(\delta _{(1,\infty )}(t))=\Delta _\mathsf{K}^{\frac{it}{2\pi }}\), \(U(r_1)=J_\mathsf{K}\). Suppose that \(W_0=(\lambda ,r_0)\) corresponds to the halfline \((0,\infty )\). For \(g \in {\mathrm{Aff}}(\mathbb{R })\), let \(\mathsf{N}(g.W_0)\) be the standard subspace associated to \(g.W_0 = (x_{g.W_0},\sigma _{g.W_0})\) through the (anti)unitary representation U. In this picture,
and the translations satisfy
As a consequence, negative halfsided modular inclusions \(\mathsf{K}\subseteq \mathsf{H}\) are in in 11 correspondence with (anti)unitary negative energy representation \((U,\mathcal{H })\) of \({\mathrm{Aff}}(\mathbb{R }) \cong \mathbb{R }\rtimes \mathbb{R }^\times \) with
and with \(U(\delta (t))=\Delta _\mathsf{H}^{\frac{it}{2\pi }}\), \(U(r_0)=J_\mathsf{H}\), \(U(\delta _{(\infty ,1)}(t))=\Delta _\mathsf{K}^{\frac{it}{2\pi }}\), \(U(r_{1})=J_\mathsf{K}\).
Corollary 4.7
([Lo08, Corollary 2.4.3.]). If \(\mathsf{K}\subset \mathsf{H}\) is +HSMI, then \(\mathsf{H}'\subset \mathsf{K}'\) is HSMI
The axiomatics of abstract covariant nets
Hereafter we will make the following assumption on the group G.
Assumption 1
We assume that \(\mathcal{G }_E(G) \not =\emptyset \) and write \(G=G^{{\uparrow }}\rtimes \{e,\sigma \}\) for some Euler involution \(\sigma \).
Example 4.8
Note that \(G^{{\downarrow }}\) may contain involutions which are not Euler.
We consider the graded Lie group \(G := {\mathrm{SO}}_{1,n}(\mathbb{R })\) with the identity component \(G^{{\uparrow }}= {\mathrm{SO}}_{1,n}(\mathbb{R })^{{\uparrow }}\). For \(n \ge 2\), the Lie algebra \(\mathfrak{g }= {\mathfrak{so }}_{1,n}(\mathbb{R })\) is simple, \(\theta (x) =  x^\top \) is a Cartan involution, and \(\mathfrak{a }:= {\mathfrak{so }}_{1,1}(\mathbb{R }) \subseteq \mathfrak{p }\) (acting on the first two components) is a maximal abelian subspace. As the corresponding restricted root system is of type \(A_1\), our classification scheme (see (3.8) in Theorem 3.10) implies that all Euler elements in \(\mathfrak{g }\) are conjugate to the one corresponding to the boost generator
Accordingly, an involution \(\sigma \in G\) is Euler if and only if \(\sigma \) or \(\sigma \) is the orthogonal reflection in a 2dimensional Lorentzian plane.
However, \(G^{{\downarrow }}\) contains all reflections of the type
In particular neither \({\mathrm{Fix}}(\tau )\) nor \({\mathrm{Fix}}(\tau )\) must have dimension 2.
We now present the analogs of the oneparticle Haag–Kastler axioms and further fundamental properties in our general setting.
Definition 4.9
Let \(G = G^{{\uparrow }}\rtimes \{e,\sigma \}\) be as above, \(C \subseteq \mathfrak{g }\) be a closed convex \({\mathrm{Ad}}^\varepsilon (G)\)invariant cone in \(\mathfrak{g }\), and fix a \(G^{{\uparrow }}\)orbit \(\mathcal{W }_+ = G^{{\uparrow }}.W \subseteq \mathcal{G }_E(G)\). Let \((U,\mathcal{H })\) be a unitary representation of \(G^{{\uparrow }}\) and
be a map, also called a net of standard subspaces. In the following we denote this data as \((\mathcal{W }_+,U,\mathsf{N})\). We consider the following properties:

(HK1)
Isotony: \(\mathsf{N}(W_1) \subseteq \mathsf{N}(W_2)\) for \(W_1 \le W_2\).

(HK2)
Covariance: \(\mathsf{N}(gW) = U(g)\mathsf{N}(W)\) for \(g \in {G}^{{\uparrow }}\), \(W \in \mathcal{W }_+\).

(HK3)
Spectral condition: \( C \subseteq C_U := \{ x \in \mathfrak{g }:i \partial U(x) \ge 0\}.\) We then say that U is Cpositive.

(HK4)
Central twisted locality: For \(\alpha \in Z(G^{{\uparrow }})^\) and \(W \in \mathcal{W }_+\) with \(W^{'\alpha }\in \mathcal{W }_+\), there exists a unitary \(Z_\alpha \in U(G^\uparrow )'\) satisfying
$$\begin{aligned} Z_\alpha ^2 = U(\alpha ) \quad \text{ and } \quad J_{\mathsf{N}(W)} Z_\alpha J_{\mathsf{N}(W)}=Z_\alpha ^{1}, \end{aligned}$$(4.3)such that
$$\begin{aligned} \mathsf{N}(W^{'\alpha }) \subset Z_\alpha \mathsf{N}(W)'. \end{aligned}$$(4.4)Moreoever, such an \(\alpha \) exists.
When \(Z_\alpha \) is trivial, for instance when \(\partial (G^\uparrow _{{\underline{W}}})=\{e\}\), then the central twisted locality reduces to the more familiar locality relation.
 (HK4\(_e\)):

Locality: If \(W \in \mathcal{W }_{+}\) is such that \(W'\in \mathcal{W }_+\), then \(\mathsf{N}(W') \subset \mathsf{N}(W)'.\)
Concerning (HK3), note that \(C_U\) is pointed if and only if \(\ker (U)\) is discrete. Therefore the assumption that C is pointed is compatible with the possible existence of representations with discrete kernel satisfying (HK3). Furthermore, if \(C=\{0\}\), then (HK3) trivially holds.
The following property will be central in our discussion because it connects the modular groups of standard subspaces to the unitary representation U of \(G^{{\uparrow }}\).

(HK5)
Bisognano–Wichmann (BW) property: \(U(\lambda _W(t)) = \Delta _{\mathsf{N}(W)}^{it/2\pi }\) for \(W \in \mathcal{W }_+, t \in \mathbb{R }\).
We will see in Proposition 4.19 that a consequence of (HK15) is the following stronger form of (HK4):

(HK6)
Central Haag Duality: \(\mathsf{N}(W^{'\alpha })=Z_\alpha \mathsf{N}(W)'\) for \(\alpha \in Z(G^{{\uparrow }})^\), \(W \in \mathcal{W }_+\) with \(W^{'\alpha }\in \mathcal{W }_+\) and \(Z_\alpha \) as in (4.3).
If the representation U extends antiunitarily to G we can further require:

(HK7)
Gcovariance: For any \(\alpha \in Z(G^{{\uparrow }})^\) such that \(W^{'\alpha }\in \mathcal{W }_+\), there exists an (anti)unitary extension \(U^\alpha \) of U from \(G^{{\uparrow }}\) to G such that the following condition is satisfied:
$$\begin{aligned} \mathsf{N}(g *_\alpha W) = U^\alpha (g) \mathsf{N}(W) \quad \text{ for } \quad g \in G, \end{aligned}$$(4.5)where \(*_\alpha \) is the \(\alpha \)twisted action (2.37) of G on \(\mathcal{W }_+\) defined in Lemma 2.18(e).
It is enough to provide an extension \(U^\alpha \) w.r.t. one \(\alpha \in Z(G^{{\uparrow }})^\) such that \(W^{'\alpha }\in \mathcal{W }_+\). All the other extensions come as described in Lemma 2.18(f). The modular conjugation of standard subspaces can have a geometric meaning when the extension \(U^\alpha \) from (HK7) has the following specific form:

(HK8)
Modular reflection: \(U^\alpha (\sigma _W)= Z_\alpha J_{\mathsf{N}(W)}\) for \(\alpha \in Z(G^{{\uparrow }})^\), \(W \in \mathcal{W }_+\) with \(W^{'\alpha }\in \mathcal{W }_+\) and \(Z_\alpha \) as in (4.3).
In the next sections we will show that there exist nets of standard subspaces satisfying all the above assumptions. It is the analog of the BGL construction in this general setting.
Wedge isotony and halfsided modular inclusions
Taking the wedge modular inclusion defined in Section 2.4.1 into account, we now prove that isotony can be deduced from covariance, the Bisognano–Wichmann property and the Cspectral condition. On specific models this has been checked in [BGL02, Lo08].
Proposition 4.10
Let \((\mathcal{W }_+,\mathsf{N},U)\) be a net of standard subspaces. Then the spectral condition (HK3), the BW property (HK5) and \(G^{{\uparrow }}\)covariance (HK2) imply isotony (HK1).
Proof
Let \(W_0 = (h,\tau ) \in \mathcal{G }_E\) and \(\mathsf{H}_0 = \mathsf{N}(W_0)\). By covariance, the net \(\mathsf{N}\) is isotone if and only if
As the stabilizer \(G^{{\uparrow }}_{W_0}\) stabilizes \(\mathsf{H}_0\) by covariance, isotony is equivalent to \(\exp (x) \in \mathcal{S }_{\mathsf{H}_0}\) for every \(x \in C_+ \cup C_\).
By the spectral condition (HK3), we have \(\mp i \partial U(x) \ge 0\). Therefore Theorem 4.4 shows that isotony is equivalent to
By the BW property (HK5), \(U^{\mathsf{H}_0}(e^s)= \Delta _{\mathsf{H}_0}^{is/2\pi } = U(\exp s h)\), so that \([h,x]= \pm x\) for \(x \in C_\pm \) implies (4.6). \(\square \)
The Brunetti–Guido–Longo (BGL) construction
We have seen in the introduction to Section 2 that each standard subspace \(\mathsf{H}\) specifies a homomorphism
and that this leads to a bijection
between continuous (anti)unitary representations of the graded Lie group \(\mathbb{R }^\times \) and standard subspaces ([NÓ17, Prop. 3.2]). By Lemma 4.2, \(\Phi \) is equivariant with respect to the natural action of \({\mathrm{AU}}(\mathcal{H })\) on \({\mathrm{Stand}}(\mathcal{H })\) and the action (2.3) on \({\mathrm{Hom}}_{\mathrm{gr}}(\mathbb{R }^\times ,{\mathrm{AU}}(\mathcal{H }))\).
Now every (anti)unitary representation \(U :G \rightarrow {\mathrm{AU}}(\mathcal{H })\) defines by composition a natural Gequivariant map
Combining this with \(\Phi \) leads to the socalled Brunetti–Guido–Longo (BGL) construction:
Definition 4.11
(Brunetti–Guido–Longo (BGL) net.) If (U, G) is an (anti)unitary representation, then we obtain a Gequivariant map \(\mathsf{N}_U :\mathcal{G }\rightarrow {\mathrm{Stand}}(\mathcal{H })\) determined for \(W = (k_W, \sigma _W)\) by
This means that, with respect to Definition 2.3, \(U^{\mathsf{N}_U(W)} = U \circ \gamma _W\) for \(W \in \mathcal{G }\) (see [BGL02, NÓ17, Prop. 5.6]).
The BGL net associates to every wedge \(W\in \mathcal{G }\) a standard subspace \(\mathsf{N}_U(W)\). We shall denote with \((\mathcal{W }_+,\mathsf{N}_U,U)\) the restriction of the BGL net to the \(G^{{\uparrow }}\)orbit \(\mathcal{W }_+ \subseteq \mathcal{G }_E(G)\).
Theorem 4.12
The restriction of the BGL net \(\mathsf{N}_U\) associated to an (anti)unitary Cpositive representation U of \(G=G^\uparrow \rtimes \{e,\sigma \}\) to a \(G^{{\uparrow }}\)orbit \(\mathcal{W }_+\subseteq \mathcal{G }_E\) satisfies all the axioms (HK1)(HK3) and (HK5).
We shall see in Proposition 4.16 that the twisted locality (HK4), Central Haag Duality (HK6) and (HK78) are also satisfied.
Proof
Let \(\mathcal{W }_+ \subseteq \mathcal{G }_E(G)\) be a \(G^{{\uparrow }}\)orbit. By construction, the restriction of the BGL net \(\mathsf{N}_U\) to \(\mathcal{W }_+\) satisfies (HK2) and by construction it satisfies (HK5). By Proposition 4.10, isotony (HK1) follows from the Spectral Condition (HK3), which is the Cpositivity of U. \(\square \)
As a last remark in this section we stress that two (anti)unitary extensions of a unitary representation \((U,\mathcal{H })\) of \(G^{{\uparrow }}\) are unitarily equivalent, but the corresponding BGL nets depend on the choice of the (anti)unitary extension. The following proposition makes this dependence explicit and provides a natural parameter space.
Proposition 4.13
(The space of (anti)unitary extensions). Fix \((h,\tau ) \in \mathcal{G }\), let \(U :G \rightarrow {\mathrm{AU}}(\mathcal{H })\) be an (anti)unitary representation and let \(\mathcal{M }:= U(G^{{\uparrow }})'\). Then the following assertions hold:

(i)
All (anti)unitary representations \(({\widetilde{U}},\mathcal{H })\) extending \(U\vert _{G^{{\uparrow }}}\) are of the form \({\widetilde{U}} = T U T^{*}\) for some \(T\in \mathrm{U{}}(\mathcal{M })\). The corresponding BGL nets are related by
$$\begin{aligned} \mathsf{N}_{{\widetilde{U}}}(W) = T\mathsf{N}_U(W) \quad \text{ for } \quad W \in \mathcal{G }. \end{aligned}$$(4.9) 
(ii)
(Parametrization of (anti)unitary extensions) Let \(J := U(\tau )\), \(\tau \in G^\downarrow \). For every
$$\begin{aligned} N \in \mathrm{U{}}(\mathcal{M })^{} := \{ M \in \mathrm{U{}}(\mathcal{M }) :J M J = M^{1} \}, \end{aligned}$$there exists a unique (anti)unitary extension \({\widetilde{U}}\) of \(U\vert _{G^{{\uparrow }}}\) with \({\widetilde{U}}(\tau ) = N J\), and we thus obtain a bijection between the set \(\mathrm{U{}}(\mathcal{M })^\) and the set of (anti)unitary extensions of \(U\vert _{G^{{\uparrow }}}\) to G.
Proof
(i) follows from Proposition A.1 and the assertion on the BGL nets is an immediate consequence of the definitions.
(ii) Let \(T \in \mathrm{U{}}(\mathcal{M })\), so that \({\widetilde{U}} = T U T^{1} :G \rightarrow {\mathrm{AU}}(\mathcal{H })\) is an (anti)unitary extension of \(U\vert _{G^{{\uparrow }}}\) with \({\widetilde{J}} := {\widetilde{U}}(\tau ) = T J T^{1}\). Since \({\widetilde{U}}\) and U extend the same representation of \(G^{{\uparrow }}\),
This element satisfies \(J N J = J {\widetilde{J}} = N^{1}\), so that \(N \in \mathrm{U{}}(\mathcal{M })^\) and \({\widetilde{J}} = NJ\).
If, conversely, \(N \in \mathrm{U{}}(\mathcal{M })^\), then Lemma A.2 implies the existence of an \(X =  X^* \in \mathcal{M }\) with \(N = e^{2X}\) and \(J X J =  X\). For \(T := e^X \in \mathrm{U{}}(\mathcal{M })\) and \({\widetilde{J}} := T J T^{1}\), we then have
Therefore the manifold \(\mathrm{U{}}(\mathcal{M })^\) parametrizes the (anti)unitary extensions of \(U\vert _{G^{{\uparrow }}}\). \(\square \)
Twisted locality
We have seen in Section 2.4.2 that it can happen that \(W'\notin \mathcal{W }_+ = G^{{\uparrow }}.W\). One can anyway attach to \(W'\) a real subspace by the BGL net and by construction obtain the relation \(\mathsf{H}(W')=\mathsf{H}(W)'\). On the other hand one can define natural complementary wedges \(W^{'\alpha }\) indexed by central elements \(\alpha \). In this section we will see that in the BGL construction, the complementary wedge subspaces satisfy the central Haag duality condition (HK6), hence the twisted locality relation (HK4). We start with a lemma on standard subspaces.
Lemma 4.14
Let \(\mathsf{H}\subset \mathcal{H }\) be a standard subspace, and \(U\in \mathrm{U{}}(\mathcal{H })\) be a unitary operator commuting with \(\Delta _\mathsf{H}\) and satisfying \(J_\mathsf{H}UJ_\mathsf{H}= U^{1}\). Let \(\mathsf{H}_1\) be the standard subspace defined by \((\Delta _\mathsf{H}, UJ_\mathsf{H}).\) There exists a unitary square root Z of U commuting with \(\Delta _\mathsf{H}\) such that \(J_\mathsf{H}ZJ_\mathsf{H}= Z^{1}\) and \(Z\mathsf{H}=\mathsf{H}_1\). The standard subspace \(\mathsf{H}_1\) does not depend on this choice of Z.
Proof
The existence of the square root and the commutation relation with the modular conjugation and the modular operator follows by Lemma A.3. Then
implies that \(\mathsf{H}_1 = Z \mathsf{H}\). It is clear that \(\mathsf{H}_1\) does not depend on the choice of Z. \(\square \)
In order to conclude (HK6), hence the central locality condition on a BGL net \(\mathsf{N}_U\), we will need an analogous statement relating complementary wedge subspaces.
Proposition 4.15
Let \((U,\mathcal{H })\) be an (anti)unitary representation of the graded group \(G=G^\uparrow \rtimes \{e,\sigma \}\) and \(\alpha \in Z(G^{{\uparrow }})^\). Then the commutant \(U(G^{{\uparrow }})'\) contains a unitary square root \(Z_\alpha \) of \(U(\alpha )\) satisfying
Proof
First we note that \(U(\alpha ) \in \mathcal{M }:= U(G^{{\uparrow }})'\). We fix \(\sigma _0 \in {\mathrm{Inv}}(G^{{\downarrow }})\) and observe that conjugation with \(U(\sigma _0)\) defines an antilinear isomorphism \(\beta \) of \(\mathcal{M }\). As \(\beta (U(\alpha )) = U(\alpha )^{1}\) follows from \(\alpha \in Z(G^{{\uparrow }})^\), we find with Lemma A.3(c) in the appendix, a unitary square root \(Z_\alpha \) of \(U(\alpha )\) satisfying
For any other \(\sigma \in G^{{\downarrow }}\) we have \(\sigma = \sigma _0g\) with \(g \in G^{{\uparrow }}\), so that
\(\square \)
We are now ready to verify that the BGL net is compatible with the twistings appearing in (HK4), (HK6) and (HK7).
Proposition 4.16
For every (anti)unitary representation \((U,\mathcal{H })\) of G, the BGL net \(\mathsf{N}_U\) satisfies (HK4) and (HK6). Moreover, for \(\alpha \in Z(G^{{\uparrow }})^\), \(W \in \mathcal{W }_+\) with \(W^{'\alpha } \in \mathcal{W }_+\) and \(Z_\alpha \in U(G^{{\uparrow }})'\) satisfying (4.3), the (anti)unitary extension \((U^\alpha , \mathcal{H })\) of \(U\vert _{G^{{\uparrow }}}\) to G, determined by \(U^\alpha (\sigma _W) := Z_\alpha U(\sigma _W)\), satisfies (HK7) and (HK8).
Proof
Let \(\alpha \in Z(G^{{\uparrow }})^\) and \(W = (x,\sigma ) \in \mathcal{W }_+\) be such that \(W^{'\alpha } = (x, \alpha \sigma )\in \mathcal{W }_+\). Proposition 4.15 implies the existence of \(Z_\alpha \in U(G^{{\uparrow }})'\) satisfying (4.3). Then
imply that \(\mathsf{N}_U(W^{'\alpha }) = Z_\alpha \mathsf{N}_U(W)'.\) This shows that (HK6), hence also (HK4) are satisfied. We also have
Since \(\mathsf{N}_U\) is Gequivariant on \(\mathcal{G }\), this leads for \(g \in G^{{\uparrow }}\) to
This proves (HK7). As \(J_{\mathsf{N}_U(W)} = U(\sigma _W)\) by definition, we also have
so that \(U^\alpha \) also satisfies (HK8). \(\square \)
Remark 4.17
(a) If \(U\vert _{G^{{\uparrow }}}\) is irreducible, then \(U(Z(G^{{\uparrow }})) \subseteq \mathbb{T }\mathbf{1 }\), so that, we find for any \(\alpha \in Z(G^{{\uparrow }})\) that \(U(\alpha ) = \zeta \mathbf{1 }\) with \(\zeta  = 1\). We may thus put \(Z_\alpha := z\mathbf{1 }\) for any complex number z with \(z^2 = \zeta \). In this case \(J Z_\alpha J = Z_\alpha ^*\) holds for any antiunitary operator J.
(b) Let \((U,\mathcal{H })\) be an (anti)unitary representation of G. For any other square root Z of \(U(\alpha )\) satisfying the same requirements as \(Z_\alpha \), the unitary operator \(Z^{1} Z_\alpha \) is an involution commuting with U(G), so that it leaves all standard subspaces \(\mathsf{N}(W)\) of the BGL net invariant.
(c) If \(\alpha \in Z(G^{{\uparrow }})\) satisfies \(\alpha ^\sigma = \alpha \) for \(\sigma \in G^{{\downarrow }}\), then \(\alpha \) acts trivially on \(\mathcal{G }( G)\) and, by covariance of \(\mathsf{N}\), leaves all standard subspaces \(\mathsf{N}(W)\) invariant. This happens in particular if \(\alpha ^2 = e\). Then also \(\alpha \in {Z(G^{{\uparrow }})^}\), so that \(\alpha \)twisted complements are useful in the context of fermionic theories. Here \(U(\alpha )\) is an involution and one choice of a square root of \(U(\alpha )\) is given by
Given a net satisfying (HK1)(HK5), the commutation relation among twist operators and the wedge modular operators immediately hold.
Proposition 4.18
Let \((\mathcal{W }_+,U, \mathsf{N})\) be a Gcovariant net satisfying (HK1)(HK5), suppose that U extends to an (anti)unitary representation of G, and let \(Z_\alpha \in U(G^{{\uparrow }})'\) as in (4.3). Then, for every \(W \in \mathcal{W }_+\), we have
The latter proposition allows to conclude that (HK6) is a consequence of (HK1)(HK5).
Proposition 4.19
Let \((\mathcal{W }_+,\mathsf{N},U)\) be a net of standard subspace satisfying (HK1)(HK5). Then it also satisfies central Haag duality (HK6):
In particular, the right hand side does not depend on the choice of \(Z_\alpha \).
Proof
By (HK5), the unitary operator \(Z_\alpha \in U(G^{{\uparrow }})'\) commutes with the modular operator of \(\mathsf{N}(W)\), by Proposition 4.18. Therefore the two standard subspaces \(\mathsf{N}(W^{'\alpha })\) and \(Z_\alpha \mathsf{N}(W)'\) have the same modular operator. By twisted locality \(\mathsf{N}(W^{'\alpha }) \subseteq Z_\alpha \mathsf{N}(W)'\), so that Lemma 4.3 implies that they coincide. \(\square \)
Remark 4.20
Let \((\mathcal{W }_+,\mathsf{N},U)\) be a net of standard subspaces with a unitary Cpositive representation \((U,\mathcal{H })\) of \(G^\uparrow \). Let \(W_0=(x,\sigma )\in \mathcal{W }_+\subset \mathcal{G }_E\) and \(\mathsf{H}_0 := \mathsf{N}(W_0)\). We claim that (HK13) imply that
defines an (anti)unitary extension of \(U\vert _{G^{{\uparrow }}(W_0)}\) to the graded subgroup \(G(W_0) = G^{{\uparrow }}(W_0)\rtimes \{e,\sigma \}\) of G. In fact, \(J_{\mathsf{H}_0}\) commutes with \(G^\uparrow _{W_0}\) by Lemma 4.2. Further, the Cpositivity and Theorem 4.4(b) imply that it also has the correct commutation relation with \(\exp (C_\pm )\), hence also with \(G^{{\uparrow }}(W_0)\). We shall see in Section 4.4, when we actually obtain an extension to the full group G.
Example 4.21
(The Poincaré case). Let \({\underline{G}}:= \mathcal{P }_+ := \mathbb{R }^{1,3} \rtimes {\mathrm{SO}}_{1,3}(\mathbb{R })_0^\uparrow \) be the proper Poincaré group and
be its simply connected covering. We write \(\lambda _{\underline{W}}\) for the oneparameter group lifting the boost group \(\Lambda _{\underline{W}}\) associated to a wedge \({\underline{W}}\in \mathcal{W }= {\underline{G}}.W_1\) (see e.g. [Mo18]). For \({\underline{G}}^{{\uparrow }}\), a wedge is defined by a pair \({\underline{W}}= (x,r_x)\), where x generates \(\Lambda _{{\underline{W}}}\) and \(r_x = e^{\pi i x}\) is the spacetime reflection in the direction of the wedge. Since \(Z=Z( G)= \{ \pm \mathbf{1 }\}\) is a 2element group, a wedge \(W \in \underline{\mathcal{G }}\) has two lifts which belong to two different \( G^{{\uparrow }}\)orbits in \(\mathcal{G }( G)\). To see this, we note that \(Z = Z^\) and \(Z_2 = \{e\}\). For the second equality we use the isomorphism \({\mathrm{Spin}}_{1,3}(\mathbb{R })\) with \({\mathrm{SL}}_2(\mathbb{C })\) and note that the centralizer of any Euler element x, which may be assumed to be \(x = \begin{pmatrix} {\textstyle {\frac{1}{2}}}&{} 0 \\ 0 &{} {\textstyle {\frac{1}{2}}} \end{pmatrix}\), is connected and isomorphic to the multiplicative group \(\mathbb{C }^\times \), on which the involution \(\sigma _x\) acts trivially. Therefore the central elements \(\partial (g) = g^\sigma g^{1}\), \(g \in G^{{\uparrow }}_{(x,\sigma _x)}\), are all trivial, which leads to \(Z_2 = \{e\}\).
For \(\alpha := \mathbf{1 }\), the twisted complement of \(W = (k_W, \sigma _W)\) is \(W^{'1}=(k_W, \sigma _W)\). Any lift \({\widetilde{r}} :\mathbb{R }\rightarrow G^{{\uparrow }}\) of a rotation oneparameter group \(\rho :\mathbb{R }\rightarrow {\mathrm{SO}}_2(\mathbb{R }) \hookrightarrow {\mathrm{SO}}_{1,3}(\mathbb{R })\) in \({\underline{G}}^{{\uparrow }}\) satisfying \({\mathrm{Ad}}(\rho (\pi )) k_W =  k_W\) now satisfies \({\widetilde{\rho }}(2\pi ) = \mathbf{1 }\). This shows that, \(W' = (k_W, \sigma _W) \not \in G^{{\uparrow }}.W\), but that \(W^{'1} = (k_W, \sigma _W) \not \in G^{{\uparrow }}.W\).
Let \((U,\mathcal{H })\) be an irreducible unitary positive energy representation of \( G^{{\uparrow }}\) for which \(U(1) \not = \mathbf{1 }\), then \(U(1) =  \mathbf{1 }\) by Schur’s Lemma. For the BGL net \(\mathsf{N}:\mathcal{G }( G) \rightarrow {\mathrm{Stand}}(\mathcal{H })\) we therefore have \(\mathsf{N}(W^{'1})=i\mathsf{N}(W)'\) and \(Z_\alpha = i\mathbf{1 }\) is a suitable twist operator (cf. [Mo18, Thm. 2.8]).
Example 4.22
(Finite coverings of the Möbius group). Consider the nfold covering of the Möbius group \( G^{{\uparrow }}:={\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}^{(n)} \subseteq G:={\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}^{(n)}_2\), where \({\underline{G}}= {\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}_2\) (cf. Example 2.10(e)). This group is obtained from \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_2\) by factorization of the subgroup \(n Z({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}})\). Then \(Z := Z(G^{{\uparrow }}) \cong \mathbb{Z }_n\) is a cyclic group of order n. Let \(\alpha := {\widetilde{\rho }}(2\pi ) \in Z\) be a generator, where \({\widetilde{\rho }} :\mathbb{R }\rightarrow G^{{\uparrow }}\) is the lift of the rotation group.
Let \((U,\mathcal{H })\) be an (anti)unitary representation of G whose restriction to \(G^{{\uparrow }}\) is irreducible. Then, by Schur’s Lemma, \(U(\alpha ^n) = U({\widetilde{\rho }}(\pi n))\) is an involution in \(\mathbb{T }\mathbf{1 }\), hence \(\pm \mathbf{1 }\). We now define ntwisted local nets of real subspaces as follows:

n is even. As \(\beta ^\tau = \beta ^{1}\) for \(\beta \in Z\), we have \( Z^ = Z\) and \( Z_1\cong \mathbb{Z }_{n/2}\) is a subgroup of index 2. As for \({\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}_2\), we have \( Z_2 = Z_1\). We therefore obtain for every Euler couple \(W = (x,\sigma ){\in \mathcal{G }_E(G)}\) two \( G^{{\uparrow }}\)orbits \( G^{{\uparrow }}.{(\pm x,\sigma )}\) covering \({\underline{G}}^{{\uparrow }}.{\underline{W}}\subseteq \mathcal{G }_E(\underline{G})\). Choosing \( G^{{\uparrow }}.(x,\sigma )\), one obtains with the BGL construction a net of real subspaces \(I\mapsto \mathsf{N}(I)\), where I denotes an interval of length smaller than \(2\pi \) in the \(\frac{n}{2}\)covering \(\mathbb{S }^1_{(n/2)} {\simeq \mathbb{R }/\pi n\mathbb{Z }}\) of \(\mathbb{S }^1\). We can realize the net on intervals in \(\mathbb{S }^1_{(n/2)}\) because \(U({\widetilde{\rho }}(n\pi ))\mathsf{N}(I)={\pm }\mathsf{N}(I)=\mathsf{N}(I)\). For the central element \(\alpha ={\widetilde{\rho }}(2\pi )\in Z\), twisted complements look as follows. For \(I=(a,b)\subset \mathbb{R }/\pi n\mathbb{Z }\) with \(ba < 2\pi \), we have \(I^{'\alpha }= I^c\), where \(I^c=(b2\pi ,a)\) is the “complement” obtained by conformal reflection on the left endpoint, cf. (2.25). All the other twisted complement, belonging to the same orbit, are obtained by covariance.
The locality relation then is given by
$$\begin{aligned} \mathsf{N}(I^{'\alpha })=\omega ^k \mathsf{N}(I)', \qquad k\in {\mathbb {Z}}, \end{aligned}$$where \(\alpha ={\widetilde{\rho }}(2\pi k)\) and \(\omega \in \mathbb{T }\) satisfies \(\omega ^2 \mathbf{1 }= U({\widetilde{\rho }}(2\pi ))\). Since U is irreducible and Z is a cyclic group of order n, \(U({\widetilde{\rho }}(2\pi ))\) is an nth root of the unity, hence \(\omega ^{2n} = 1\) and \(Z_\alpha =\omega ^k\mathbf{1 }\).

n is odd. Then \( Z^ = Z_1\) implies that \( G^{{\uparrow }}\) acts transitively on the inverse images of \({\underline{G}}^{{\uparrow }}\)orbits in \(\underline{\mathcal{G }}\). Fixing the orbit \(G^{{\uparrow }}.(x,\sigma )\), we have by the BGL construction a net of real subspaces \(I\mapsto \mathsf{N}(I)\), where, again, I is an interval of length smaller than \(2\pi \) in the nfold covering of \(\mathbb{S }^1\). Here the locality relation is
$$\begin{aligned} \mathsf{N}(I^{'\alpha })=\omega ^k \mathsf{N}(I)', \qquad k\in {\mathbb {Z}}, \end{aligned}$$where \(\alpha ={\widetilde{\rho }}(2\pi k)\) and \(\omega ^{2n} = 1\), \(I^{'\alpha }\) and \(Z_\alpha \) are as above.
New models
Theorem 3.10 provides the list of restricted root systems for real simple Lie algebras containing (symmetric) Euler elements, hence supporting (symmetric) Euler wedges. Any such Lie algebra \(\mathfrak{g }\) is the Lie algebra of a simply connected Lie group \(G^{{\uparrow }}\). Then (2.10) defines an Euler involution on the group \(G^{{\uparrow }}\), so that we obtain the extension to \(G=G^\uparrow \rtimes \{{\mathrm{id}},\sigma \}\).
Such a Lie group \(G^{{\uparrow }}\) has many unitary representations, possibly with positive energy if the Lie algebra \(\mathfrak{g }\) is hermitian. By unitary induction, one can construct a unitary representation of \(G^{{\uparrow }}\) from a unitary representation of a subgroup, for instance from a covering of \({\mathrm{PSL}}_2(\mathbb{R })\subset G^{{\uparrow }}\) [Ma52]. It is always possible, to extend a unitary representation \((U,\mathcal{H }_U)\) of \(G^\uparrow \) to an (anti)unitary representation of G by doubling the Hilbert space, if the representation does not extend on \(\mathcal{H }_U\) itself. Indeed, we can choose any conjugation C on \(\mathcal{H }_U\) and observe that the representation defined by \({\widetilde{U}}(g) = U(g) \oplus CU(\sigma g\sigma )C\) on \(\mathcal{H }_U \oplus \mathcal{H }_U\) extends to G by \(U(\sigma )=\left( \begin{array}{cc}0&{}C\\ C&{}0\end{array}\right) \). By the BGL construction there exists a (twisted)local oneparticle net satisfying (HK18).
As a consequence we have the theorem:
Theorem 4.23
Let \(\mathfrak{g }\) be a simple real Lie algebra containing an Euler element, i.e., whose restricted root system occurs in Theorem 3.10. Then there exists a graded Lie group \(G=G^{{\uparrow }}\cup G^{{\downarrow }}\) as in Section 2.1 with an (anti)unitary representations U, and these in turn define twisted Gcovariant BGL nets \((\mathcal{W }_+,U,\mathsf{N})\).
This theorem shows, for instance, that it is possible to associate a covariant homogeneous net of standard subspace to a Lie algebra \(\mathfrak{g }\) with restricted root system \(E_7\). The subgroups \(G_{\pm 1} = \exp (\mathfrak{g }_{\pm 1}(x)) \subseteq G^{{\uparrow }}\) are closed, and if \(G_0 := \{ g \in G^{{\uparrow }}:{\mathrm{Ad}}(g)x = x\}\), then so is \(\mathbf{P} := G_0 G_{1}\). Then \(M := G^{{\uparrow }}/\mathbf{P}\) is a homogeneous space whose tangent space in the base point can be identified with the eigenspace \(\mathfrak{g }_1(x) = \ker ({\mathrm{ad}}x \mathbf{1 })\). If \(\mathfrak{g }\) is simple hermitian of tube type and \(C \subseteq \mathfrak{g }\) is a pointed generating invariant cone, then \(C_+ := C \cap \mathfrak{g }_1(x)\) defines a \(G^{{\uparrow }}\)invariant causal structure on M. The soobtained manifolds include the Jordan spacetimes of Günaydin [Gu93, Gu00, Gu01] and the simple spacetime manifolds in the sense of Mack–de Riese [MdR07]. If the rank of the restricted root system \(\Sigma \) of \((\mathfrak{g },\mathfrak{a })\) is 2, then M is a Lorentzian manifold, but in general it is not. As a consequence of Proposition 3.11 and Table 2, there exists a real form with a nontrivial positive cone i.e., \(\mathfrak{g }\) is hermitian of tube type, for every root system appearing in Theorem 3.10. Thus models with a proper notion of positive energy can be associated to every root system supporting symmetric Euler elements.
Recently, in [NÓ20] it has been shown that irreducible (anti)unitary representations \((U,\mathcal{H })\) of G which are of positive energy in the sense that \(i \partial U(y) \ge 0\) for \(y \in C\), lead to Gcovariant nets \((\mathtt{V}_\mathcal{O })\) of real subspace of \(\mathcal{H }\), indexed by open subsets \(\mathcal{O }\subseteq M\). If \(\mathcal{O }\not =\emptyset \), then \(\mathtt{V}_\mathcal{O }\) is generating, and it is standard if \(\mathcal{O }\) is not “too big”. In particular, the open subset \(\mathcal{O }= \exp (C_+^0)\mathbf{P} \subseteq M\) corresponds to a standard subspace with the Bisognano–Wichmann property for which the modular group is represented by the oneparameter group \((\exp tx)_{t \in \mathbb{R }}\) of G (see [NÓ20, §5.2]).
The \({\mathrm{SL}}_2\)problem, symmetry extension
In Section 3.2 we have seen that the existence of orthogonal Euler wedges corresponds to the existence of an \({\mathfrak{sl }}_2\)subalgebra containing both Euler elements. In this section we will discuss when we can extend a covariant net of standard subspaces \((\mathcal{W }_+,\mathsf{N}, U)\) of Euler wedges satisfying (HK1)(HK5) to a Gcovariant net.
We first look at the (anti)unitary extensions of unitary representations of \({\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\). In \({\mathfrak{sl }}_2(\mathbb{R })\), we consider the two Euler elements
Let \((U,\mathcal{H })\) be a unitary representation of the group \(G := {\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\) and consider the two selfadjoint operators
Theorem 4.24
Every continuous unitary representation of \({\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\) extends to an (anti)unitary representation of the group
where \(\tau _G\) is the involutive automorphism of \({\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\) induced by the Lie algebra automorphism
corresponding to the Euler element h.
In [GL95, Lo08] this theorem was proved for \({\mathrm{SL}}_2(\mathbb{R })\)representations of the principal and discrete series. Here the argument does not depend on the family of the representation.
Proof
Since \({\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\) is a type I group, every unitary representation has a unique direct integral decomposition into irreducible unitary representations. This reduces the problem to the irreducible case. We have to show that \(U \circ \tau _G \cong U^*\) (the dual representation). Let
Then h, k, u is a basis of \({\mathfrak{sl }}_2(\mathbb{R })\) and
is a Casimir element, so that
The antilinear extension \(\overline{\tau }\) of \(\tau \) to \({\mathfrak{sl }}_2(\mathbb{C })\) satisfies \(\overline{\tau }(iu) = iu\) and the operator \(i\partial U(u)\) is selfadjoint and diagonalizable. We have
so that \(U^* \circ \tau _G\) is an irreducible with the same uweights and the same Casimir eigenvalue c. Below we argue that U is uniquely determined by any pair \((\mu ,c)\), where \(\mu \) is an eigenvalue of \(i\partial U(u)\) occurring in the representation ([Sa67, Lo08]), and this implies that \(U \circ \tau _G \cong U^*\).
To see that U is determined by the pair \((\mu ,c)\), we first recall that \(\mathcal{H }\) decomposes into onedimensional eigenspaces of \(i\partial U(u)\) and, by irreducibility, it is generated by any eigenvector \(\xi _\mu \) of eigenvalue \(\mu \). Let \(\mathcal{U }(\mathfrak{g })\) denote the complex enveloping algebra of \(\mathfrak{g }\). Then \(V_\mu := \mathcal{U }(\mathfrak{g })\xi _\mu \) is a dense subspace consisting of analytic vectors, so that the representation U is determined by the \(\mathfrak{g }\)representation on this space. In \(\mathcal{U }(\mathfrak{g })\) the centralizer \(\mathcal{C }_u\) of u is generated by u and the Casimir element. Therefore \(\xi _\mu \) is a \(\mathcal{C }_u\)eigenvector and the corresponding homomorphism \(\chi :\mathcal{C }_u \rightarrow \mathbb{C }\) is determined by \(\chi (u) = \mu \) and \(\chi (\omega ) = c\). It is now easy to verify that these two values determine the \(\mathcal{U }(\mathfrak{g })\)module structure on \(V_\mu \), hence the unitary representation U. \(\square \)
Remark 4.25
Here the determination of the representation is obtained by considering in the enveloping algebra \(\mathcal{U }({\mathfrak{sl }}_2(\mathbb{R }))\), the centralizer subalgebra \(\mathbb{C }[\omega ,u]\) of u. Any cyclic weight vector \(\xi _{\mu ,c}\) defines a character \(\chi \) of this subalgebra by \(\chi (iu) = \mu \) and \(\chi (\omega ) = c\), and \(\mathcal{U }(\mathfrak{g })\xi _{\mu ,c}\) is isomorphic to the quotient of \(\mathcal{U }(\mathfrak{g })\) by the left ideal generated by \(\mu \mathbf{1 } iu\) and \(\omega  c\mathbf{1 }\).
Now, we consider the positive selfadjoint operator
By Theorem 4.24, U extends to an (anti)unitary representation of \({\widetilde{{\mathrm{GL}}}}_2(\mathbb{R })\), and we put
Lemma 4.26
For a unitary operator \(T \in \mathrm{U{}}(\mathcal{H })\), the following assertions are equivalent:

(a)
\(S T S \subseteq T\) holds on a dense subspace.

(b)
\(T^{1} \mathtt{V}\cap \mathtt{V}\) is standard.
If these conditions are satisfied, then (a) holds on \(T^{1} \mathtt{V}\cap \mathtt{V}\).
Proof
If (b) holds, then any \(\xi \in T^{1}\mathtt{V}\cap \mathtt{V}\) satisfies \(S T S \xi = S T \xi = T \xi ,\) so that (a) holds.
Conversely, assume that
is dense in \(\mathcal{H }\). For any \(\xi \in \mathcal{D }\) we then have \(T\xi \in \mathcal{R }(S) = \mathcal{D }(S)\) and
so that \(\mathcal{D }\) is Sinvariant. This implies that \(\mathcal{D }= (\mathcal{D }\cap \mathtt{V}) + i (\mathcal{D }\cap \mathtt{V}),\) so that \(\mathcal{D }\cap \mathtt{V}\) is standard. For \(\xi \in \mathtt{V}\), we have \(T\xi \in \mathtt{V}\) if and only if \(\xi \in \mathcal{D }\), so that \(\mathcal{D }\cap \mathtt{V}= T^{1} \mathtt{V}= \mathtt{V}.\) This proves the lemma. \(\square \)
Proposition 4.27
The following assertions are equivalent:

(a)
\(\Delta _h^{1/2} e^{itK} \Delta _h^{1/2} \subseteq e^{itK}\) holds for every \(t \in \mathbb{R }\) on a dense subspace of \(\mathcal{H }\).

(b)
\(S e^{itK} S \subseteq e^{itK}\) holds for every \(t \in \mathbb{R }\) on a dense subspace of \(\mathcal{H }\).

(c)
\(e^{itK} \mathtt{V}\cap \mathtt{V}\) is standard for every \(t \in \mathbb{R }\).
If these conditions are satisfied, then (a) holds on \(J(e^{it K}\mathtt{V}\cap \mathtt{V})\) and (b) on \(e^{it K}\mathtt{V}\cap \mathtt{V}\).
Proof
(a) \(\Leftrightarrow \) (b): From \(\tau (k) = k\) it follows that
so that conjugating with J translates (a) into (b).
(b) \(\Leftrightarrow \) (c) follows from Lemma 4.26. \(\square \)
From [GL95, Thm. 1.1, Cor. 1.3(c)] one can deduce that the equivalent conditions in Proposition 4.27 are satisfied for principal series representations and lowest and highest weight representations, but it is not known for complementary series representations.
The following theorem shows that an isotone, central twisted local \(G^{{\uparrow }}\)covariant net of standard subspaces satisfying the BW property is actually Gcovariant. The argument needs the density property described in Proposition 4.27 for \({\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\). The extension is done by (HK8).The proof generalizes the argument in [GL95].
Theorem 4.28
(Extension Theorem). Let \(G=G^\uparrow \rtimes \{{\mathrm{id}},\sigma \}\) be a graded Lie group, where \(\sigma \) is an Euler involution. Let \((U,\mathcal{H })\) be a unitary Cpositive representation of \(G^\uparrow \), \(\mathcal{W }_+\subseteq \mathcal{G }_E(G)\) be a \(G^{{\uparrow }}\)orbit, and \((\mathcal{W }_+, \mathsf{N},U)\) be a net of standard subspaces satisfying (HK14) and the BW property (HK5). If \(h_1, \ldots , h_n\), \(n \ge 2\), is a pairwise orthogonal family of Euler elements generating the Lie algebra \(\mathfrak{g }\), and the conditions in Proposition 4.27 hold for the representations of the connected subgroups corresponding to the \({\mathfrak{sl }}_2\)subalgebras generated by \(h_1\) and \(h_j\) for \(j =2,\ldots , n\), then U extends to an (anti)unitary representation of G such that Gcovariance (HK7) and modular reflection (HK8) hold.
Proof
Let \((\mathcal{W }_+,\mathsf{N},U)\) be a net of standard subspaces satisfying (HK15). The Bisognano–Wichmann property (HK5) implies Central Haag Duality (HK6) by Proposition 4.19. Let \(H_j:=i\partial U(h_j)\) be the selfadjoint generators of the unitary oneparameter group corresponding to \(h_j\). By Corollary 3.14, every pair \((h_1,h_j)\) generates a subalgebra isomorphic to \({\mathfrak{sl }}_2(\mathbb {R})\) and the generators \(H_1\) and \(H_j\) integrate to a representation of \({\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\). Consider the Euler wedges \(W_1, W_j\in \mathcal{W }_+\) associated to \(h_1\) and \(h_j\), respectively.
We claim that Proposition 4.27 implies that \(U(\sigma _{h_1}) := J_{\mathsf{N}(W_1)}\) associated to the standard subspace \(\mathsf{N}(W_1)\) extends the \({\widetilde{{\mathrm{SL}}}}_2(\mathbb{R })\)representation to an (anti) unitary representation of \({\widetilde{{\mathrm{PGL}}}}_2(\mathbb{R })\). Indeed, by Proposition 4.27(b) we have that
on the dense domain \(J_{\mathsf{N}(W_1)}(e^{itH_j} \mathtt{V}\cap \mathtt{V})\) with \(\mathtt{V}={\mathrm{Fix}}(J_{\mathsf{N}(W_1)}\Delta _{\mathsf{N}(W_1)}^{1/2}) = \mathsf{N}(W_1)\), cf. condition (c) in Proposition 4.27. On the previous domain we then have
With Proposition 4.27(a) we can now conclude that
because both sides are bounded operators which coincide on a dense subspace. Since the Lie algebra \(\mathfrak{g }\) is generated by \(h_1,\ldots ,h_n,\) we obtain
In particular, U defines an (anti)unitary representation of G. Pick \(\alpha \in Z(G^{{\uparrow }})^\) such that (HK4) is satisfied and consider the twisted representation of G defined by \(U^\alpha (\sigma _{h_1}):=Z_\alpha J_{\mathsf{N}(W_1)} = Z_\alpha U(\sigma _{h_1})\). Since \(\mathsf{N}\) coincides with the restriction to \(\mathcal{W }_+\) of the BGL net of the (anti)unitary representation U of G, the representation \(U^\alpha \) satisfies (HK7) and (HK8) by Proposition 4.16. \(\square \)
Note that the density property as well as the existence of orthogonal wedges are sufficient but not necessary to have a Gcovariant action: Consider the BGL net associated to the unique irreducible positive energy representation U of the \(G = {\mathrm{Aff}}(\mathbb{R })\) on the real line. Then the standard subspaces \(\mathsf{N}_U(a,\infty )\) and \(\mathsf{N}_U(\infty , b)\) are associated to positive and negative halflines and satisfy (HK1)(HK5). There are noorthogonal wedges in this case but the extension to an (anti)unitary representation of G is given by
We further remarks that in this case \(\sigma _W\) does not preserve the wedge family \(\mathcal{W }_+\).
For the Poincaré group, with the identification of wedge regions and Euler elements (see (2.28)), the axial wedges
define a family of orthogonal wedge regions, namely wedge regions associated to orthogonal Euler elements. Considering wedges as subsets of Minkowski spaces one can define further regions by wedge intersection. Spacelike cones are particularly important: they are defined, up to translations by finite intersection of wedges obtained by Lorentz transforms of \(W_1\). Analogously one can define, by intersecting wedge subspaces, subspaces associated to any spacelike cone. In principle this can also be trivial, but if they are standard, the cyclicity assumption of 4.27(c) is ensured, cf. [GL95].
Consider \(G={\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}}\rtimes \{{\mathrm{id}},{\widetilde{\tau }}\}\). Let \((\mathcal{W }_+,U,\mathsf{N})\) be a net of standard subspaces satisfying (HK1)(HK5). Let \({\widetilde{I}}_\supset \subseteq \mathbb{R }\) be an interval with \(q({\widetilde{I}}_\supset )=I_\supset \) where the latter is the right semicircle with endpoints \((i,i)\subset \mathbb{S }^1\). Then the dilation generators \({\widetilde{\delta }}_\cap \) and \({\widetilde{\delta }}_\supset \) define orthogonal Euler elements generating \(\widetilde{{\textsf {M}}\ddot{\textsf {o}}{\textsf {b}}}\). Considering the wedges \(W_\cap =(x_\cap , \sigma _\cap )\) and \(W_\supset =(x_\supset , \sigma _\supset )\) with \(W_\cap ={\widetilde{\rho }}(\pi /2)W_\supset \), the intersection is again a wedge interval \({\widetilde{I}}={\widetilde{I}}_\cap \cap {\widetilde{I}}_\supset \). In particular, by isotony, \(\mathsf{N}({\widetilde{I}}_\cap )\cap \mathsf{N}({\widetilde{I}}_\supset )\supset \mathsf{N}({\widetilde{I}})\) is standard and condition (c) in Proposition 4.27 holds.
Outlook
Nets of von Neumann algebras and standard subspaces
The fundamental objects in algebraic quantum field theory are the local algebras of observables depicted by von Neumann algebras. In this setting standard subspaces arise naturally in the modular theory of von Neumann algebras when the vacuum state is specified. Indeed, if \(\mathcal{M }\subseteq B(\mathcal{H })\) is a von Neumann algebra and \(\Omega \in \mathcal{H }\) is a cyclic and separating vector, then the modular conjugation \(J_{\mathcal{M },\Omega }\) and the modular operator \(\Delta _{\mathcal{M },\Omega }\) specified by the Tomita–Takesaki Theorem coincide respectively with the modular conjugation \(J_{\mathtt{V}}\) and the modular operator \(\Delta _{\mathtt{V}}\) determined by the standard subspace \(\mathtt{V}:= \overline{\{ M\Omega :M = M^* \in \mathcal{M }\}}\). However, our discussion aims at another realization of von Neumann algebra nets. One can use the Second Quantization procedure to associate to each standard subspace \(\mathtt{V}\subseteq \mathcal{H }\) a pair \((\mathcal{R }_{+}(\mathtt{V}),\Omega )\), where \(\mathcal{R }_{+}(\mathtt{V})\) is a von Neumann algebra on the bosonic Fock space \(\mathcal{F }_{+}(\mathcal{H })\), see e.g. [LRT78, NÓ17, §6]. For other statistics, such as fermions and anyons, we refer to [EO73, BJL02, Sc97]. This correspondence permits to translate between results on configurations of standard subspaces and configurations of von Neumann algebras and to construct a net of von Neumann algebras out of a one particle net of standard subspaces (see for instance [LRT78]).
This procedure can be applied in our case. For instance it is straightforward to construct the bosonic second quantization of the BGL net associated to an (anti)unitary positive energy representation of a \({\mathbb {Z}}_2\)graded Lie group G supporting Euler wedges, provided \(Z(G)=e\). In the general case an appropriate symmetrization of the Fock space has to be carried out, which requires a finer analysis of the twisted locality in the second quantization picture. This first example suggests that a generalized axiomatic framework for Haag–Kastler nets of von Neumann algebras on the abstract set of Euler wedges is possible and deserves to be explored.
Once wedge localization of one particle states or von Neumann algebra has been properly defined, the next step is to look for finer localization properties in our abstract setting. In general, due to the a priori lack of a reference spacetime for the orbits of Euler wedges, a possible definition of wedge intersection is an intriguing step to face. Indeed, very different configurations are visible in the literature for the well known models. For example fundamental localization regions on the Minkowski spacetime are obtained by intersecting wedges. They can be bounded, for instance doublecones,^{Footnote 9} or unbounded. The latter are called spacelike cones when—up to a Poincaré transformation—we consider an intersection of a family of wedges through the origin. In this case the spacelike cones are characterized by a semigroup of translations sending the cone into itself. In a chiral theory, wedges are intervals on the circle and connected regions obtained by wedge intersections are intervals again. In this case, intersections can be described again in terms of Euler wedges. On the de Sitter spacetime, wedge intersections are still possible. On the other hand it is not clear how to define them at the group level: for instance there is no Lorentz transformation fixing or sending intersections into themselves. Once a proper notion of spacelike cone is determined in our abstract setting, it will be possible to explore fundamental properties and notions in AQFT such as spinstatistics relations or nuclearity properties [GL95, DF84, BDL07].
3graded Lie algebras
For an orbit \(\mathcal{W }_+ := G^{{\uparrow }}.(x,\sigma )\) in the abstract wedge space of G, any (anti)unitary representation leads by the BGL construction to an equivariant map \(\mathsf{N}:\mathcal{W }_+ \rightarrow {\mathrm{Stand}}(\mathcal{H })\), which can be considered as a homogeneous net of standard subspaces. To see which of these nets are most interesting, one may ask which of the orbits \(U(G^{{\uparrow }})\mathtt{V}\subseteq {\mathrm{Stand}}(\mathcal{H })\) carry a nondegenerate order structure in the sense that the semigroup
is “large”, meaning that its interior clusters in e. From [Ne19, Ne19b] we know that this happens if and only if \(({\mathrm{ad}}x)^3 = {\mathrm{ad}}x\), i.e., if \({\mathrm{ad}}x\) defines a 3grading on the Lie algebra \(\mathfrak{g }\) (cf. Definition 2.4) and the positive cone \(C_U := \{ x \in \mathfrak{g }:i \partial U(x) \ge 0\}\) is such that the intersections \(C_U \cap \mathfrak{g }_{\pm 1}(x)\) generate \(\mathfrak{g }_{\pm 1}(x)\). This motivates our focus on pairs \((x,\sigma )\), where x is an Euler element and \({\mathrm{Ad}}(\sigma )\) the corresponding Lie algebra involution \(\sigma _x\).
On the abstract level, this leads to configurations represented by quadruples \((\mathfrak{g },\sigma , C, x)\), where \(\mathfrak{g }\) is a Lie algebra, \(\sigma \in {\mathrm{Aut}}(\mathfrak{g })\) an involution, \(x \in \mathcal{E }(\mathfrak{g })\) an Euler element with \(\sigma (x) = x\), and \(C \subseteq \mathfrak{g }\) an invariant convex cone with \(\sigma (C) =  C\). For classification results concerning such configurations, we refer to the recent work of D. Oeh ([Oeh20, Oeh21]).
Now consider a general net of standard subspaces \(\mathsf{N}\) undergoing an action of the group G satisfying the assumptions (HK14). It is a consequence of Lemma 4.2 and Theorem 4.4 that
is a oneparameter group in \(U(S_{\mathsf{N}(W)})'\). So the BisognanoWichmann property holds if \({Z_{\mathsf{N}(W)}(t)\equiv 1}\). In particular an analysis of the gauge space \(U(S_{\mathsf{N}(W)})'\) will allow us to understand possible counterexamples to the BW property, possibly generalizing the ones contained in [Mo18, LMR16], to the case where the modular theory of the net does not implement any geometric global action.
Geometric realization of wedge spaces
In the present paper, we studied the abstract wedge spaces \(\mathcal{W }_+ = G^{{\uparrow }}.(x,\sigma )\) on an algebraic level, having in mind that there are many interesting concrete situations, where the elements of this space correspond to “wedge domains” in various kinds of spacetime manifolds.
A systematic descriptions of “wedge domains” in causal symmetric spaces has to be undertaken. A causal symmetric space is a homogeneous space \(M = G/H\), where G is a connected Lie group,^{Footnote 10} and there exists an involution \(\tau \) on G for which \(H \subseteq G^\tau \) is an open subgroup (i.e., a union of connected components) such that M carries a Ginvariant field of pointed open cones \(V_+(m) \subseteq T_m(M)\) (the causal structure). The nonflat causal symmetric spaces come in two flavors, the compactly causal ones with closed causal geodesics, and the noncompactly causal ones for which M carries a global order structure defined by the causal curves (see [HÓ96] for details on these concepts). Important examples are de Sitter space \({\mathrm{dS}}^d \cong {\mathrm{SO}}_{1,d}^{{\uparrow }}(\mathbb{R })/{\mathrm{SO}}_{1,d1}(\mathbb{R })^{{\uparrow }}\) (noncompactly causal) and anti de Sitter space \({\mathrm{AdS}}^d \cong {\mathrm{SO}}_{2,d1}(\mathbb{R })_e/{\mathrm{SO}}_{1,d1}(\mathbb{R })^{{\uparrow }}\) (compactly causal).
In particular, any Lie group G is a symmetric space with respect to the transitive action of \(G\times G\) by \((g_1, g_2).g = g_1 g g_2^{1}\), and any pointed generating invariant cone \(C\subseteq \mathfrak{g }\cong T_e(G)\) defines a \((G \times G)\)invariant causal structure. In this case any Euler element h for which the cones \(C_\pm := \pm C \cap \mathfrak{g }_{\pm 1}(h)\) are generating, leads to the semigroup
which plays in the symmetric space G the role of a wedge domain. If \(G = (\mathbb{R }^{1,d1},+)\) is ddimensional Minkowski space, \(C = V_+\) is the open light cone and h the generator of a Lorentz boost, then S coincides with the corresponding Rindler wedge.
It is also possible to describe for any reductive causal symmetric space \(M = G/H\) and Euler elements \(h \in \mathfrak{g }\) generating a flow on M fixing the base point, a wedge domain \(W_M(h)\). Then \(\mathcal{W }_M(h) := \{ g W_M(h) :g \in G \}\) is a geometric wedge space. Up to coverings, this construction leads in particular to a geometric realisation of all abstract wedge spaces corresponding to Euler couples of semisimple Lie algebras. The geometric wedge spaces have a natural order if M is compactly causal (such as Minkowski space or antide Sitter space), but if M is noncompactly causal, there is no natural order structure (as for de Sitter space). This picture can be used to obtain, for compactly causal spaces, from certain unitary representations of G satisfying a spectral condition covariant nets of real subspace \(\mathtt{V}(\mathcal{O }) \subseteq \mathcal{H }\), \(\mathcal{O }\subseteq M\) open, that assign to the wedge domain \(W_M(h)\) the standard subspace \(\mathtt{V}\) associated to the pair \((h,\tau )\). In this sense, they have the Bisognano–Wichmann property ([NÓ20]). Several aspects of the underlying geometry will be discussed in the forthcoming papers [NÓ21a, NÓ21b].
These constructions are only first steps in a theory that needs to be developed. Important open questions concern characterizations of (irreducible) representations for which such geometric nets exist. In particular, the case of noncompactly causal spaces, which corresponds to nonordered wedge spaces, is largely open, but there are well known nets on de Sitter space (such as the ones obtained from covariant quantum fields) that fit into this picture.
Notes
The spacetime reflection \(j_1(t,x_1,x_2,\ldots ,x_n)=(t,x_1,x_2,\ldots , x_n) \) is implemented by the modular conjugation corresponding to the standard right wedge \(W_1\).
In [GL03] it is used that the 2dimensional de Sitter space \({\mathrm{dS}}^2 \cong {\mathrm{SO}}_{1,2}(\mathbb{R })^{{\uparrow }}/{\mathrm{SO}}_{1,1}(\mathbb{R })^{{\uparrow }}\) has the same abstract wedge space as the circle \({\mathrm{SO}}_{1,2}(\mathbb{R })/\mathbf{P}\) to set up a \({\mathrm{dS}}/CFT\) correspondence.
For instance \(W_i\) and \(W_j\) for \(i\ne j\), where \(W_i=\{(t,x)\in \mathbb {R}^{1+s}:t<x_i\}\).
For a Lie subalgebra \(\mathfrak{s }\subseteq \mathfrak{g }\), we write \({\mathrm{Inn}}_\mathfrak{g }(\mathfrak{s })= \langle e^{{\mathrm{ad}}\mathfrak{s }} \rangle \subseteq {\mathrm{Aut}}(\mathfrak{g })\) for the subgroup generated by \(e^{{\mathrm{ad}}\mathfrak{s }}\).
In [Ne19b] it is shown that the different descriptions as a product of two sets (polar decomposition) and a product of two abelian subsemigroups and a group yield the same set \(\mathcal{S }_W\) which actually is a subsemigroup.
This is the twisted version of the 2fold cover of the extended Möbius groups; see Remark 2.7(d).
Considering Z as a module \(\mathbb{Z }_2\)module via the involution \(\sigma _ Z\), we have \(Z^1(\mathbb{Z }_2, Z)\cong Z^\) and \(B^1(\mathbb{Z }_2, Z) \cong Z_1,\) so that the cohomology group is \(H^1(\mathbb{Z }_2, Z) := Z^1(\mathbb{Z }_2, Z)/B^1(\mathbb{Z }_2, Z) \cong Z^/ Z_1\). We refer to [HN12, Ex. 18.3.15] or [ML63, Thm. IV.7.1] for more on group cohomology.
Here we use that the Lie algebra \([\mathfrak{g },\mathfrak{r }]\) is nilpotent, so that the exponential function of the corresponding group \({\mathrm{Inn}}_\mathfrak{g }([\mathfrak{g },\mathfrak{r }])\) is surjective, see [HN12].
Up to Poincaré transformations, these are the causal closures of a ball in the timezero surface.
In this subsection we write G instead of \(G^{{\uparrow }}\) to simplify notation.
References
Araki, H.: A lattice of von Neumann algebras associated with the quantum theory of a free Bose field. J. Math. Phys. 4, 1343–1362 (1963)
Baumgärtel, H., Jurke, M., Lledo, F.: Twisted duality of the CARalgebra. J. Math. Phys. 43:8, 4158–4179 (2002)
Bertram, W., Neeb, K.H.: Projective completions of Jordan pairs, Part I. The generalized projective geometry of a Lie algebra. J. Algebra 277:2, 474–519 (2004)
Borchers, H.J.: The CPTTheorem in twodimensional theories of local observables. Commun. Math. Phys. 143, 315–332 (1992)
Borchers, H.J.: On revolutionizing quantum field theory with Tomita’s modular theory. J. Math. Phys. 41, 3604–3673 (2000)
Bourbaki, N.: Groupes et algèbres de Lie, Chap. IV–VI. Masson, Paris (1990)
Brunetti, R., Guido, D., Longo, R.: Modular localization and Wigner particles. Rev. Math. Phys. 14, 759–785 (2002)
Buchholz, D., D’Antoni, C., Longo, R.: Nuclearity and thermal states in conformal field theory. Commun. Math. Phys. 270(1), 267–293 (2007)
D’antoni, F., Fredenhagen, K.: Charges in spacelike cones. Commun. Math. Phys. 94, 537–544 (1984)
Dybalski, W., Morinelli, V.: Bisognano–Wichmann property for asymptotically complete massless QFT. Commun. Math. Phys. 380, 1267–1294 (2020)
Eckmann, J.P., Osterwalder, K.: An application of Tomita’s theory of modular Hilbert algebras: duality for free Bose Fields. J. Funct. Anal. 13(1), 1–12 (1973)
Faraut, J., Koranyi, A.: Analysis on Symmetric Cones. Oxford Math. Monographs. Oxford University Press, Oxford (1994)
Gui, B.: Bisognano–Wichmann property for rigid categorical extensions and nonlocal extensions of conformal nets. arXiv:1912.10682
Guido, D., Longo, R.: An algebraic spin and statistics theorem. Commun. Math. Phys. 172(3), 517–533 (1995)
Guido, D., Longo, R.: A converse Hawking–Unruh effect and \({{\rm dS}}^{2} /CFT\) correspondence. Ann. Henri Poincaré 4, 1169–1218 (2003)
Guido, D., Longo, R., Wiesbrock, H.W.: Extensions of conformal nets and superselection structures. Commun. Math. Phys. 192(1), 217–244 (1998)
Günaydin, M.: Generalized conformal and superconformal group actions and Jordan algebras. Modern Phys. Lett. A 8(15), 1407–1416 (1993)
Günaydin, M.: AdS/CFT Dualities and the unitary representations of noncompact groups and supergroups: Wigner versus Dirac, contribution to “6th International Wigner Symposium (WIGSYM 6). arXiv:hepth/0005168
Günaydin, M.: Generalized AdS/CFT dualities and unitary realizations of spacetime symmetries of \(M\)theory. Class. Quantum Grav. 18, 3131–3141 (2001)
Haag, R.: Local Quantum Physics. Fields, Particles, Algebras. Texts and Monographs in Physics, 2nd edn. Springer, Berlin (1996)
Hilgert, J., Neeb, K.H.: Structure and Geometry of Lie Groups. Springer, New York (2012)
Hilgert, J., Ólafsson, G.: Causal symmetric spaces, geometry and harmonic analysis. Perspectives in Mathematics, vol. 18. Academic Press, Cambridge (1996)
Hochschild, G.P.: Basic theory of algebraic groups and Lie algebras. Graduate Texts in Mathematics, vol. 75. Springer, New York (1981)
Kaneyuki, S., Asano, H.: Graded Lie algebras and generalized Jordan triple systems. Nagoya Math. J. 112, 81–115 (1988)
Kaneyuki, S.: The Sylvester’s law of intertia in simple graded Lie algebras. J. Math. Soc. Jpn 50(3), 593–614 (1998)
Kaneyuki, S.: Graded Lie algebras and pseudohermitian symmetric space. In: Faraut, J., et al. (eds.) Analysis and Geometry on Complex Homogeneous Domains. Progress in Math., vol. 185. Birkhäuser, Boston (2000)
Krötz, B., Neeb, K.H.: On hyperbolic cones and mixed symmetric spaces. J. Lie Theory 6(1), 69–146 (1996)
Leyland, P., Roberts, J.E., Testard, D.: Duality for quantum free fields. unpublished manuscript, Marseille 1978
Longo, R.: Real Hilbert subspaces, modular theory, SL(2, R) and CFT in “Von Neumann Algebras in Sibiu”, 3391, Theta Ser. Adv. Math. 10, Theta, Bucharest
Longo, R., Morinelli, V., Preta, F., Rehren, K.H.: Split property for free finite helicity fields. Ann. Henri Poincaré 20(8), 2555–2584 (2019)
Longo, R., Morinelli, V., Rehren, K.H.: Where infinite spin particles are localizable. Commun. Math. Phys. 345, 587–614 (2016)
Longo, R., Xu, F.: Comment on the Bekenstein bound. J. Geom. Phys. 130, 113–120 (2018)
Mack, G., de Riese, M.: Simple spacetime symmetries: generalizing conformal field theory. J. Math. Phys. 48(5), 052304 (2007)
Mackey, G. W.: Induced Representations of Locally Compact Groups I. Annals of Mathematics, Second Series, Vol. 55, No. 1, pp. 101–139 (1952)
MacLane, S.: Homological Algebra. Springer, Berlin (1963)
Morinelli, V.: The Bisognano–Wichmann property on nets of standard subspaces, some sufficient conditions. Ann. Henri Poincaré 19(3), 937–958 (2018)
Morinelli, V., Rehren, K.H.: Spacelike deformations: higherspin fields from scalar fields. Lett. Math. Phys. 110, 2019–2038 (2020)
Morinelli, V., Tanimoto, Y.: Scale and Möbius covariance in twodimensional Haag–Kaster net. Commun. Math. Phys. 371(2), 619–650 (2019)
Mund, J.: The Bisognano0–Wichmann theorem for massive theories. Ann. Henri Poincaré 2, 907–926 (2001)
Neeb, K.H.: Holomorphy and Convexity in Lie Theory. Expositions in Mathematics 28. de Gruyter Verlag, Berlin (1999)
Neeb, K.H.: Finite dimensional semigroups of unitary endomorphisms of standard subspaces. Representation Theory, to appear arXiv:math.OA.1902.02266
Neeb, K.H.: Semigroups in 3graded Lie groups and endomorphisms of standard subspaces. arXiv:OA:1912.13367; Kyoto J. Math., to appear
Neeb, K.H., Ólafsson, G.: Antiunitary representations and modular theory, in “50th Sophus Lie Seminar”, Eds. K. Grabowska et al, J. Grabowski, A. Fialowski and K.H. Neeb; Banach Center Publications 113, pp. 291–362 (2017). arXiv:mathRT:1704.01336
Neeb, K.H., Ólafsson, G.: Nets of standard subspaces on Lie groups. Advances in Math., to appear arXiv:2006.09832
Neeb, K.H., Ólafsson, G.: Wedge domains in noncompactly causal symmetric spaces, in preparation
Neeb, K.H., Ólafsson, G.: Wedge domains in compactly causal symmetric spaces, in preparation
Oeh, D.: Classification of 3graded causal subalgebras of real simple Lie algebras, Transformation Groups, 2021. https://doi.org/10.1007/s00031020096358, arXiv:math.RT:2001.03125
Oeh, D.: Lie wedges of endomorphism semigroups of standard subspaces in admissible Lie algebras. arXiv:math.RT:2007.13445v1
Sally, P.: Analytic Continuation of the Irreducible Unitary Representations of the Universal Covering Group of SL(2,R). Memoirs of the Amer. Math. Soc. 69, Amer. Math. Soc., Providence, Rhode Island (1967)
Schroer, B.: Wigner representation theory of the Poincaré group, localization, statistics and the Smatrix. Nuclear Phys. B 499–3, 519–546 (1997)
Takeuchi, M.: On conjugate loci and cut loci of compact symmetric spaces II. Tsukuba J. Math. 3(1), 1–29 (1979)
Weinberg, S.: The Quantum Theory of Fields. Vol. I. Foundations. Cambridge University Press, Cambridge (2005)
Weinberg, S.: Symmetry: A Key to Nature’s Secrets, The New York Review of Books (2011). https://www.nybooks.com/articles/2011/10/27/symmetrykeynaturessecrets/
Wiesbrock, H.W.: A comment on a recent work of Borchers. Lett. Math. Phys. 25, 157–159 (1992)
Wiesbrock, H.W.: Halfsided modular inclusions of von Neumann algebras. Commun. Math. Phys. 157, 83–92 (1993)
Witten, E.: Notes on some entanglement properties of Quantum Field Theory. Rev. Mod. Phys. 90, 45003 (2018)
Acknowledgements
VM was supported by the European Research Council Advanced Grant 669240 QUEST and by Indam from March 2019 to February 2020. VM acknowledges the MIUR Excellence Department Project awarded to the Department of Mathematics, University of Rome “Tor Vergata”, CUP E83C18000100006 and the University of Rome “Tor Vergata” funding scheme “Beyond Borders”, CUP E84I19002200005.
KHN acknowledges support by DFGgrant NE 413/101.
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Communicated by Y. Kawahigashi
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Toolbox
Proposition A.1
([NÓ17, Thm. 2.11(a)]). If \((U,\mathcal{H })\) is a unitary representation of \(G^{{\uparrow }}\), then any two (anti)unitary extensions \(({\widetilde{U}}_j, \mathcal{H })\), \(j =1,2\), of U to G are unitarily equivalent, i.e., there exists \(\Gamma \in U(G^{{\uparrow }})'\) with
Lemma A.2
Let \(\mathcal{M }\subseteq B(\mathcal{H })\) be a von Neumann algebra and \(J \in {\mathrm{Conj}}(\mathcal{H })\) such that \(J \mathcal{M }J = \mathcal{M }\). Then the exponential function of the Banach symmetric space
is surjective, i.e., for every \(U \in \mathrm{U{}}(\mathcal{M })^{J,}\) there exists an element \(X =  X^* \in \mathcal{M }\) with \(J X J =  X\) such that \(U = e^X\).
Proof
We consider the antilinear automorphism
of the von Neumann algebra \(\mathcal{M }\). Let \(\mathcal{N }\subseteq \mathcal{M }\) be the abelian von Neumann algebra generated by a fixed element \(U \in \mathrm{U{}}(\mathcal{M })^{J,}\). Then \(\alpha (U) = U^{1} = U^*\) implies that \(\alpha (\mathcal{N }) = \mathcal{N }\) with \(\alpha (A) = A^*\) for every \(A \in \mathcal{N }\). Any spectral resolution of U in \(\mathcal{N }\) and any bounded measurable function \(f :\mathbb{T }\rightarrow i\mathbb{R }\) with \(e^{f} = {\mathrm{id}}_\mathbb{T }\) yields an element \(X := f(U)\in \mathcal{N }\) with \(X^* = X\) and \(e^{X} = U\). Then \(J X J = \alpha (X) = X^* =  X.\) \(\square \)
The following lemma is [NÓ17, Lemma A.1]:
Lemma A.3
Let \(\mathcal{M }\subseteq \mathcal{H }\) be a von Neumann algebra, \(\alpha :\mathcal{M }\rightarrow \mathcal{M }\) a reallinear weakly continuous automorphism and \(U \in \mathrm{U{}}(\mathcal{M })\) be a unitary element. Then the following assertions hold:

(a)
If \(\alpha \) is complex linear and \(\alpha (U)= U\), then there exists a \(V \in \mathrm{U{}}(\mathcal{M })\) with \(\alpha (V) = V\) and \(V^2 = U\).

(b)
If \(\alpha \) is complex linear and \(\alpha (U)= U^{1}\) with \(\ker (U+\mathbf{1 }) = \{0\}\), then there exists a \(V \in \mathrm{U{}}(\mathcal{M })\) with \(\alpha (V) = V^{1}\) and \(V^2 = U\).

(c)
If \(\alpha \) is antilinear and \(\alpha (U)= U^{1}\), then there exists a \(V \in \mathrm{U{}}(\mathcal{M })\) with \(\alpha (V) = V^{1}\) and \(V^2 = U\).

(d)
If \(\alpha \) is antilinear and \(\alpha (U)= U\) with \(\ker (U+\mathbf{1 }) = \{0\}\), then there exists a \(V \in \mathrm{U{}}(\mathcal{M })\) with \(\alpha (V) = V\) and \(V^2 = U\).
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Morinelli, V., Neeb, KH. Covariant Homogeneous Nets of Standard Subspaces. Commun. Math. Phys. 386, 305–358 (2021). https://doi.org/10.1007/s00220021040466
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DOI: https://doi.org/10.1007/s00220021040466