On the linearity of order-isomorphisms
Bas Lemmens, Hent van Imhoff, and Onno van Gaans

TL;DR
This paper characterizes conditions under which order-isomorphisms in certain partially ordered vector spaces are linear, extending previous results to infinite dimensions and broader classes of cones.
Contribution
It introduces a milder condition for linearity of order-isomorphisms, extending known results to infinite-dimensional spaces and general cones.
Findings
Order-isomorphisms are linear for every Archimedean cone satisfying the new condition.
Provides a general form of order-isomorphisms on specific cones.
Proves linearity of homogeneous order-isomorphisms in new settings.
Abstract
A basic problem in the theory of partially ordered vector spaces is to characterise those cones on which every order-isomorphism is linear. We show that this is the case for every Archimedean cone that equals the inf-sup hull of the sum of its engaged extreme rays. This condition is milder than existing ones and is satisfied by, for example, the cone of positive operators in the space of bounded self-adjoint operators on a Hilbert space. We also give a general form of order-isomorphisms on the inf-sup hull of the sum of all extreme rays of the cone, which extends results of Artstein-Avidan and Slomka to infinite dimensional partially ordered vector spaces, and prove the linearity of homogeneous order-isomorphisms in a variety of new settings.
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On the linearity of order-isomorphisms
Bas Lemmens Email: [email protected] School of Mathematics, Statistics & Actuarial Science, University of Kent, Canterbury, CT2 7NX, United Kingdom
Onno van Gaans Email: [email protected] Mathematical Institute, Leiden University, P.O.Box 9512, 2300 RA Leiden, The Netherlands
Hendrik van Imhoff Email: [email protected] Mathematical Institute, Leiden University, P.O.Box 9512, 2300 RA Leiden, The Netherlands
Abstract
A basic problem in the theory of partially ordered vector spaces is to characterise those cones on which every order-isomorphism is linear. We show that this is the case for every Archimedean cone that equals the inf-sup hull of the sum of its engaged extreme rays. This condition is milder than existing ones and is satisfied by, for example, the cone of positive operators in the space of bounded self-adjoint operators on a Hilbert space. We also give a general form of order-isomorphisms on the inf-sup hull of the sum of all extreme rays of the cone, which extends results of Artstein-Avidan and Slomka to infinite dimensional partially ordered vector spaces, and prove the linearity of homogeneous order-isomorphisms in a variety of new settings.
Keywords: order-isomorphisms, affine maps, inf-sup hull
**Subject Classification: Primary 46B40; Secondary 15B48, 47H07 **
1 Introduction
A fundamental problem in the study of partially ordered vector spaces is to understand the structure of their order-isomorphisms, i.e., order preserving bijections whose inverses are also order preserving. In particular one would like to characterise those partially ordered vector spaces on which all order-isomorphisms are affine.
Pioneering research on this problem was motivated by special relativity theory where the causal order is considered on the Minkowski spacetime. During the 1950s and 1960s several results were obtained in finite dimensional spaces by Alexandrov and Ovčinnikova [3] and Zeeman [13], who showed that the order-isomorphisms from the causal cone onto itself are linear. Later Alexandrov [2] extended his result to order-isomorphisms on finite dimensional ordered vector spaces, where every extreme ray of the cone is engaged, that is to say, each extreme ray of the cone lies in the linear span of the other extreme rays. Rothaus [9] obtained a similar result where the domain of the order-isomorphism could also be the interior of the cone, but he assumes that the cone does not have any isolated extreme rays, which is a stronger assumption than the one used by Alexandrov. In the 1970s Noll and Schäffer made numerous contributions to this area in a series of papers, [7, 8, 10, 11]. Like Alexandrov, they considered the case where the cone is the sum of its engaged extreme rays, but they do not require the partially ordered vector spaces to be finite dimensional. More recently, Artstein-Avidan and Slomka [5] obtained a complete description of the order-isomorphisms between finite dimensional partially ordered vector spaces.
In many natural infinite dimensional settings the results of Noll and Schäffer are not applicable. A case in point is the space consisting of bounded self-adjoint operators on a Hilbert , ordered by the cone of positive (semi-definite) operators. Even though the cone contains many engaged extreme rays, namely the rays through the rank-one projections, it does not satisfy the condition of Noll and Schäffer. Even so Molnár [6] showed, by using operator algebra techniques, that every order-isomorphism on is linear. In this paper we obtain a generalisation of [8, Theorem A] by Noll and Schäffer that is sufficiently strong to yield Molnár’s result.
Before we outline the main results in the paper, we point out that the domain on which the order-isomorphisms are considered plays a key role. In the paper we will work on so called upper sets, i.e, sets which contain all upper bounds of its elements. Such domains include cones, their interiors, and the whole space. It turns out that without this assumption order-isomorphisms can be more complicated. Indeed, Šemrl [12] gave a complete characterisation of the order-isomorphisms on order intervals of , which include maps that are not affine.
Our generalisation of [8, Theorem A] exploits the fact that infima and suprema in a partially ordered vector space are preserved under order-isomorphisms. Instead of the conditions imposed by Noll and Schäffer, we assume that the cone, , is equal to the inf-sup hull of the positive span of its engaged extreme rays, which is much weaker. In other words, we require that each can be written as , where each belongs to
[TABLE]
and and arbitrary index sets. The main result can be formulated as follows.
Theorem 1.1**.**
Suppose and are upper sets in Archimedean partially ordered vector spaces, and is an order-isomorphism. If is directed and equals the inf-sup hull of , then is affine.
A key step in our argument is Theorem 3.10, which says that every order-isomorphism from onto is the restriction of an affine map on the affine span of . The proof requires a careful reworking of some of the ideas in [8].
Of course not every order-isomorphism is affine, Simply consider the space , consisting of continuous real functions on a compact Hausdorff space , and the map . On Schäffer [10] showed that each order-isomorphism, which is homogeneous (of degree one), is linear. In [11] he strengthened this result to general order unit spaces. In finite dimensional spaces the existence of a disengaged extreme ray in the cone is necessary and sufficient to yield a nonlinear order-isomorphism. This follows from [5, Theorem 1.7] by Artstein-Avidan and Slomka, who showed that any order-isomorphism in a finite dimensional space has a particular diagonal form. In Section 5 we obtain an infinite dimensional analogue of this result. We also give an alternative condition that guarantees that all homogeneous order-isomorphisms are linear, which can applied in partially ordered vector spaces without an order unit such as spaces.
2 Preliminaries
Let be a real vector space and be a cone in , so is convex, for all , and . The cone induces a partial order on by if . The pair is called a partially ordered vector space. For simplicity we write instead of if is clear from the context, and we write if and .
A partially ordered vector space is said to be Archimedean if for each and with for all we have that . A subset of is said to be directed if for each there exists such that and . It is well known that is directed if and only if is generating, i.e., . Given we define the order interval by . We denote the cone with apex by
[TABLE]
Extreme rays of the cone play an important role in this paper. A vector is called an extreme vector if , and implies that for some , or, if , and implies for some . For an element we define the ray through as . If is an extreme vector, is said to be an extreme ray. The notion of an extreme ray coincides with the ray being extreme in the convex sense. Indeed, a ray in is extreme if, and only if, for any two rays and in satisfying for some we have that , see [4, Lemma 1.43]. Given an extreme ray we call an extreme half-line with apex . The following elementary property of extremal vectors will be used frequently in the sequel, see [4, Lemma 1.44].
Lemma 2.1**.**
In a partially ordered vector space any three extremal vectors in that generate three distinct extremal rays are linearly independent.
Another useful basic observation is the following.
Lemma 2.2**.**
Let be Archimedean. If are such that , and for each we have that or , then there exists a such that .
Proof.
Let be as in the statement. We may assume without loss of generality that and are non-zero. Now define . By assumption is well-defined and .
Note that . Indeed, for we have that , so that , which implies that , as is Archimedean.
To show that we distinguish two cases: and . In the case we have that for all sufficiently large. Thus, , which shows that , as the space is Archimedean. If , then , since by assumption, and as showed before. ∎
Given vector spaces and , a map is called affine if it is a translation of a linear map, that is, there is such that is linear.
Let and be partially ordered vector spaces. A set is called an upper set if and imply . So, , and translations thereof are all upper sets in . Let be an upper set. A map is called affine or linear if it is the restriction of an affine map or a linear map , respectively. If is generating then we have . A map is affine if and only if for all and with such that . It is a well-known fact that, if the upper set is convex, then is affine if and only if is convex-linear, that is, for each and we have that .
An element in a partially ordered vector space is an order unit if for all there exists a such that . If is generating, then is an order unit if and only if for every there exists with . If is Archimedean and is an order unit then the formula
[TABLE]
defines a norm on , called the order unit norm. A triple , where is an Archimedean partially ordered vector space and is an order unit in , is called an order unit space. In an order unit space we denote the interior of the cone with respect to the order unit norm by . The set is an upper set and consists of all order units of .
3 Linearity of order-isomorphisms
In the sequel and will be Archimedean partially ordered vector spaces. Initially we only consider order-isomorphisms , where and . However, the main result, Theorem 1.1, holds for more general domains.
A key role in the analysis of order-isomorphisms is played by extreme half-lines. This idea has been exploited to analyse order-isomorphisms on finite dimensional partially ordered vector spaces [5] as well as in infinite dimensions in [8]. In infinite dimensions, however, the extreme half-lines are not as useful, as there are cones that have none or only very few extreme rays. The following order theoretic characterization of extreme half-lines is due to Noll and Schäffer, see [8, Proposition 1]. For completeness we provide a proof.
Proposition 3.1**.**
If is Archimedean and , then is an extreme half-line with apex if and only if is maximal among subsets with that satisfy:
- (P1)
* is directed.* 2. (P2)
For any the order interval is totally ordered. 3. (P3)
* contains at least two distinct points.*
Proof.
Suppose is maximal among subsets that satisfy properties (P1)–(P3). We first argue that is contained in a half-line. Let be given, so . Due to (P1) there exists a such that . Since is preserved under addition, (P2) guarantees that the order interval is totally ordered. Moreover, it contains , , and for all . Therefore, by Lemma 2.2 there exist such that and . This shows that and are on the half-line through with apex . We conclude that any pair of points in lie on a half-line with apex , and hence is contained in a half-line with apex . Let be a ray in such that .
By (P3) there exists an such that and . Note that satisfies properties (P1) and (P3). We now show that also satisfies (P2). Consider with . Then equals the interval up to dilation. We know that is totally ordered, as and satisfies property (P2). Hence is also totally ordered. It now follows from the maximality assumption on that .
To see that is an extreme half-line, we note that is totally ordered, as is totally ordered. It follows from Lemma 2.2 that is an extreme vector.
Conversely, suppose is an extreme half-line. Clearly, satisfies properties (P1)–(P3). Suppose also satisfies (P1)–(P3) and . Since is directed, there exists a with . Moreover, is totally ordered by (P2) and, hence, is totally ordered and . If , then there is a such that , as is extreme, so that . Otherwise, we have and for each we have , so or . By Lemma 2.2 it follows that there is a such that . Then and . ∎
We note that property (P3) is only a necessary condition if does not have any extreme rays and can be dropped otherwise.
As a direct corollary we obtain the following result.
Corollary 3.2**.**
If is an order-isomorphism, then maps an extreme half-line with apex onto an extreme half-line with apex .
Proof.
Suppose that is an extreme ray of . Then and satisfies properties (P1)–(P3), as is an order-isomorphism. So by Proposition 3.1 we find that , where is an extreme ray of . ∎
Our next step is to show that order-isomorphisms possess an additive property on extreme half-lines, which was proved in [8, Lemma 1]. For the reader’s convenience we include the proof.
Lemma 3.3**.**
Let and be distinct extreme rays of and be an order-isomorphism. For each , and we have that
[TABLE]
Proof.
The equality in the statement holds trivially if either or equals zero. Assume and . Then for are three distinct parallel extreme half-lines. Due to Corollary 3.2, their images are extreme half-lines in and they are distinct as is injective. For each , the set is an extreme half-line that intersects for each , so, by Corollary 3.2, is an extreme half-line and
[TABLE]
We obtain that is not parallel to any of the , as and are distinct and is injective.
We aim to show that , , and are parallel. We do so in two steps. As a first step we show that if two of them are parallel, then all three of them are parallel. Indeed, assume that and are parallel, with , . Since and are distinct parallel half-lines, it follows from (3.2) that the half-line is in their affine span for every . Then the half-line with is in that affine span, too, as it intersects for two distinct values of . Thus, , , and are three extreme half-lines in the affine plane spanned by and . By Lemma 2.1, it follows that at least two of the half-lines , , and must be parallel, which yields that and must be parallel. Thus, , , and are parallel.
As a second step we argue by contradiction that at least two of the half-lines , , and are parallel. For , take such that
[TABLE]
Suppose that no two of the three extreme half-lines , , and are parallel. After translation they correspond to three distinct extremal rays, so that Lemma 2.1 yields that , , and are linearly independent. Define
[TABLE]
f(x+S)$$\bullet$$f(x)$$\bullet$$f(x+s)$$\bullet$$f(x+2s)$$f(R_{0})$$f(R_{1})$$f(R_{2})
We observe that and are parallel and distinct planes. Moreover, , and . The affine span of and is three dimensional and contains . Indeed, for every there is with , and by (3.2), contains the half-line . This shows that , and hence . Since is linearly independent of and , we conclude that intersects and .
We proceed by showing that the half-line intersects or . Loosely speaking, the point on lies between and and, therefore, the points where intersects and cannot be both at the same side of . To make this idea precise, let be such that
[TABLE]
Observe that , as . Then
[TABLE]
As , there are such that . By linear independence of , and , we have . Consider the case . Then intersects , so there is a such that . As , it follows that the half-line contains two distinct points of , so that . Therefore , which is a contradiction. Otherwise, in case , then intersects , and we similarly arrive at a contradiction. Hence at least two of the half-lines , , and are parallel, so by the first step all three of them are parallel.
Now we complete the proof. As and are parallel, we have that the vectors and have the same direction. By interchanging the roles of and we obtain that the vectors and have the same direction. Thus, , , , and are the consecutive corners of a parallellogram, which concludes the proof. ∎
It is interesting to note that the proof of Lemma 3.3 does not work if the domain of the order-isomorphism is bounded. In fact, there exist examples of order-isomorphisms on bounded order intervals for which equation (3.1) does not hold, see for example [12] where order-isomorphisms on order intervals in are studied.
The following observation is a simple consequence of the previous lemma.
Corollary 3.4**.**
Suppose are extreme vectors with for all and is an order-isomorphism. If is such that then
[TABLE]
Proof.
We only discuss the proof for the case and , and leave the other two remaining cases to the reader, as they are proved in a similar way. By writing , we get
[TABLE]
by Lemma 3.3. ∎
Using this corollary we now show the following lemma.
Lemma 3.5**.**
Let be an order-isomorphism. Suppose are extreme vectors such that for all and . If , then
[TABLE]
Proof.
By relabelling we may assume that there exists such that for all and for all . Then and for . By Corollary 3.4 we have
[TABLE]
Repeating this argument yields the desired conclusion. ∎
We can use Lemma 3.5 to get the following identity.
Lemma 3.6**.**
Let be an order-isomorphism. Suppose and are extreme vectors in such that for all and , , and for all , then
[TABLE]
Proof.
By relabelling we may assume that there exists such that for all and for all . Then for . Using a telesoping sum and Lemma 3.5 we obtain
[TABLE]
∎
Let denote the collection of all extreme rays in , and define
[TABLE]
Lemma 3.7**.**
Let be an order-isomorphism and . Suppose that , where is an extreme vector for . If is an extreme vector with for all and , and , then
[TABLE]
Proof.
Note that
[TABLE]
by Lemma 3.5.∎
In the setting of Lemma 3.7, if for some and , and where , then one could replace by a linear combination of extreme vectors not contained in and thus obtain with for all and . Then the conclusion of Lemma 3.7 still holds. This motivates the following definition due to [8] .
Definition 3.8**.**
Let be a collection of rays in a cone in a vector space . A ray is called engaged (in ) whenever
[TABLE]
holds, and is called disengaged (in ) otherwise.
It can be shown that an extreme ray of a finite dimensional cone is disengaged (in the set of extreme rays) if and only if the cone equals the Cartesian product of the ray and another subcone. Cones that do not allow such a decomposition are considered in [2].
Recall that denotes the collection of all extreme rays of . We denote the collection of all engaged extreme rays in by and the collection of all disengaged extreme rays in by . We remark that being an engaged ray is relative to the collection it is viewed in. Nevertheless, we have that the elements of are again engaged in . For simplicity we say that an extreme vector is engaged if .
Lemma 3.9**.**
If is an extreme vector, then the following assertions hold:
- (i)
* is a scalar multiple of for every and such that ;* 2. (ii)
If is engaged and and , then
[TABLE]
Proof.
Assertion (i) follows from Corollary 3.2. Remark that if is engaged then there exist extreme vectors with such that for all and . So (ii) follows from Lemma 3.7. ∎
The following result is an extension of [8, Theorem A]. Recall that denotes the collection of engaged extreme rays in . We define
[TABLE]
Theorem 3.10**.**
If is an order-isomorphism, then is affine on .
Proof.
Let be an engaged extreme ray of and fix . Let and take such that . Then . So, by Lemma 3.9(i), there exists a unique such that
[TABLE]
As is engaged, it follows from Lemma 3.9(ii) that does not depend on . Thus there exists a unique function such that for every and with we have
[TABLE]
Clearly, and is a monotone increasing function. For there exists an such that , , and . Moreover
[TABLE]
Since is engaged, Lemma 3.9(ii) gives
[TABLE]
Note that , as and is injective, and hence
[TABLE]
As is monotone increasing, additive, and , a result by Darboux (see [1, Theorem 1 in Section 2.1]) yields that for all .
To show that is affine it suffices to show that is convex-linear on , let and . Then and where each is an engaged extreme vector and for all and . Moreover, and for all . Put . As for all , we can apply Lemma 3.6 to get
[TABLE]
where we have used (3.4) and the fact that each is engaged in the forth and sixth equality, and Lemma 3.6 in the seventh one. This completes the proof. ∎
Remark 3.11**.**
It is interesting to note that in the proof of Theorem 3.10 we have only used the assumption that is an engaged extreme vector to show that the map satisfying (3.3) is independent of and additive. However, if is a disengaged extreme vector, then (3.3) still holds. In Section 5 we will exploit this observation. Moreover, we remark that it is necessary to work with the positive linear span of engaged extreme vectors, . Indeed, to apply Lemma 3.6 we need for each that is in the domain of .
Let us now see how we can use Theorem 3.10 to generalise [8, Theorem A]. Suppose and exists. If is an order-isomorphisms, then . Likewise order-isomorphisms preserve infima. These basic observations motivate the following definition.
Definition 3.12**.**
Given the inf-sup hull of is the set
[TABLE]
where and are arbitrary index sets.
Note that if and and are in the inf-sup hull of , then and , with all and in , and hence for all we have that
[TABLE]
which shows that is also in the inf-sup hull. In particular we see that the inf-sup hull of a convex subset of is again a convex set.
Lemma 3.13**.**
Let be an order-isomorphism and let be convex. If is affine on , then is affine on the inf-sup hull of .
Proof.
Suppose and are such that . Then is an upper bound of in . Moreover, if is another upper bound of , then is an upper bound of , since is order preserving. As we deduce that , so that . This implies that in . In the same way it can be shown that if and are such that , then in .
To complete the proof it suffices to show that is convex-linear on the inf-sup hull of . Indeed, the inf-sup hull of is a convex set by (3.6). Suppose that and are in the inf-sup hull of and . Write and , with for all and .
By repeatedly using the fact that preserves infima and suprema and Theorem 3.10 we get
[TABLE]
∎
Combination of Theorem 3.10 and Lemma 3.13 yields the next conclusion.
Proposition 3.14**.**
Every order-isomorphism is affine on the inf-sup hull of .
We can now prove our main result Theorem 1.1.
Proof of Theorem 1.1.
Let be given. As is the inf-sup hull of , we get that the interval equals the inf-sup hull of . So it follows from Proposition 3.14 that is affine on . As is directed the cone is generating, and hence . This implies that there exists a unique affine map such that restricted to coincides with .
In the same way we find that for any the map is affine on . Using that is directed, we know there exists such that . We remark that the intersection contains the interval . Therefore, and coincide on for all . Since , we conclude that coincides with on , which completes the proof. ∎
Theorem 1.1 is a generalisation of [8, Theorem A] by Noll and Schäffer. It would be interesting to have a complete characterisation of the (infinite dimensional) directed Archimedean partially ordered vector spaces for which every order-isomorphism is linear. To our knowledge, Theorem 1.1 is the most general result at present. It can, however, not be applied in a variety of settings such as the space with cone . In this space the cone has exactly two disengaged extreme rays: and , where for all , but it has no engaged extreme rays. We believe, however, that each order-isomorphism on the cone is linear in this space.
We end this section with a simple observation concerning direct sums. Let and be directed Archimedean partially ordered vector spaces. Then the direct sum is a directed Archimedean partially ordered vector space with cone . Moreover is an (engaged) extreme vector if and only if is an (engaged) extreme vector and , or, is an (engaged) extreme vector and . It is straightforward to infer that if and satisfy the conditions on in Theorem 1.1, then so does .
4 Self-adjoint operators on a Hilbert space
Let be a Hilbert space and be the space of bounded self-adjoint operators on , ordered by the cone of positive semi-definite operators. In this section we show that satisfies the conditions of Theorem 1.1.
It is easy to show that the extreme rays of are the rays spanned by rank-one projections. We will denote the collection of all extreme rays of by . Furthermore, for a closed subspace of we denote the orthogonal projection onto by by , and for we write .
Theorem 4.1**.**
If is a Hilbert space, with , and are upper sets, then every order-isomorphism is affine.
Proof.
We verify that satisfies the conditions of Theorem 1.1. Evidently, is directed and Archimedean. We first show that all extreme rays of are engaged. So, suppose . Then there exists an such that . As we can find non-zero such that and are orthogonal and lie in a two-dimensional subspace . Then , so that
[TABLE]
where . We conclude that can be written as a linear combination of rank-one projections different from and, hence, the ray spanned by is engaged in .
Note that the positive linear span of the extreme rays equals the set of positive finite rank operators, which will be denoted . To verify the condition in Theorem 1.1 it suffices to show that the inf-sup hull of equals , as the inf-sup hull is closed under positive sums by (3.6).
We start by showing that the identity belongs to the inf-sup hull of . Note that for all . Suppose that is an upper bound of for all . Then we have for any that
[TABLE]
Therefore, holds and we conclude that Note that it follows from (4.1) that for each with we have that
[TABLE]
as for all there exists a with and .
Now suppose that is invertible. Let be given by . Then is a linear order-isomorphism, so that
[TABLE]
As is a bijection from onto itself, we get that .
Finally, suppose . Remark that is invertible. For , with we let . Then , from which it follows that . Thus,
[TABLE]
This shows that is the inf-sup hull of the positive linear span of its extreme rays, and hence Theorem 1.1 yields the desired result. ∎
We remark that Theorem 4.1 was first proved, using different arguments, by Molnár [6] and does not follow from [8, Theorem A].
5 Order-isomorphisms in related problems
In this section we proceed the discussion of Section 3 and relate to results by Artstein-Avidan and Slomka and Schäffer in settings somewhat different than in Theorem 1.1. We obtain three results. First, we present a “diagonalization formula” for order-isomorphisms between cones, see (5.1) below. Second, we apply the results of Section 3 to positively homogeneous order-isomorphisms between cones and obtain that they must be linear if one of the cones equals the inf-sup hull of the positive span of its extreme rays. Third, we consider separable complete order unit spaces where in one of them the inf-sup hull of the positive linear span of the engaged extreme rays is big enough to intersect the interior of the cone. In that case we derive from Theorem 1.1 that every order-isomorphism between upper sets must be affine.
We begin with the following infinite dimensional analogue of a result by Artstein-Avidan and Slomka [5, Theorem 1.7].
Proposition 5.1**.**
Let and be Archimedean partially ordered vector spaces and suppose that is an order-isomorphism. Let be a collection of linearly independent extreme vectors in . Then there exist corresponding monotone increasing bijections , for , such that for all and we have
[TABLE]
Proof.
Note that . Let be an extreme vector. According to Corollary 3.2, maps the extreme ray through bijectively onto the extreme ray through . Hence there exists a nonnegative scalar such that , for all . Moreover, the function is a monotone increasing bijection. Equation (5.1) now follows from Lemma 3.6. ∎
In [5, Theorem 1.7], also the finite dimensional cases and are considered. In the situation of Proposition 5.1, if is an order-isomorphism from to and , then one can easily verify that the maps are actually defined on and that (5.1) holds for all . The infinite dimensional version of the case where is not so strong. Indeed, if and are infinite dimensional order unit spaces, then one can adapt the proof of Proposition 5.1 to show that for each order-isomorphism and each collection of linearly independent extreme vectors of , there are linearly independent extreme vectors of and monotone increasing bijections , , such that for all and we have (5.1) where is replaced by , provided that . However, in general infinite dimensional order unit spaces most elements of the interior of the cone cannot be written as a positive linear combination of finitely many positive extreme vectors and, thus, the use of this result is limited.
Let us next consider positively homogeneous order-isomorphisms. If and are such that and for every , , and , then a map is called positively homogeneous if for every and . If and are generating Archimedean cones, then this condition implies that , which yields the more common definition that includes . The definition given here also applies to maps on interiors of cones.
In [11, Theorem B], Schäffer provides the next result.
Theorem 5.2** (Schäffer).**
Let and be order unit spaces. Then every positively homogeneous order-isomorphism is linear.
The results of Section 3 yield the following alternative statement, in which the requirement of an order unit is replaced by a condition involving extreme rays.
Theorem 5.3**.**
Let and be Archimedean partially ordered vector spaces such that is directed and equals the inf-sup hull of . Then every positively homogeneous order-isomorphism is linear.
Proof.
We first show that is additive on . Let be extreme vectors in . It suffices to show that . In order to apply Lemma 3.6, we combine terms of that lie on the same ray. Indeed, for , let be disjoint with such that for every we have for some if and only if there exists with . Denote and for every let be such that . Then for . With the aid of Lemma 3.6 and the positive homogeneity of we obtain
[TABLE]
As is positively homogeneous, it follows that is linear on . Due to Lemma 3.13 we obtain that is linear on the inf-sup hull of , which equals . ∎
If in Theorem 5.3 is an order-isomorphism from to and is homogeneous instead of only positively homogeneous, then it can be shown along similar lines that is affine.
It is useful to compare Theorem 5.2 and Theorem 5.3 and identify the differences. Let and be order unit spaces. Suppose that is a positively homogeneous order-isomorphism. Then straightforward verification yields . Hence it follows by Theorem 5.2 that is linear on . As is the inf hull of the convex set , it follows from Lemma 3.13 that is linear on . Thus, any homogeneous order-isomorphism between cones of order unit spaces is linear. Theorem 5.3 provides a condition, alternative to having an order unit, that yields the same conclusion. For example, the space for with coordinate-wise order satisfies the conditions of Theorem 5.3 but fails to have an order unit. Hence Schäffer’s Theorem 5.2 does not imply our Theorem 5.3.
Our third interest in this section is an intermediate result by Schäffer, which has a milder homogeneity condition than Theorem 5.2. In [11, Corollary A1] Schäffer shows for order unit spaces and , where either or is separable and complete, that any order-isomorphism is linear, provided there exists a such that for all . Compared to [11, Theorem B], the positively homogeneous condition of is weakened to only being positively homogeneous on a ray through the interior of the cone, at the cost of one of the order unit spaces being separable and complete. In conjunction with Theorem 1.1 this yields the following.
Theorem 5.4**.**
Let and be order unit spaces, and and be upper sets. Suppose that the inf-sup hull of has a non-empty intersection with , and that either or is separable and complete. Then every order-isomorphism is affine.
Proof.
Firstly, we consider the case and . Let denote the inf-sup hull of the positive linear span of the engaged extreme rays of . By assumption there exists . We recall that an order unit space is directed and Archimedean. Hence, Proposition 3.14 says that is affine on . As is an order-isomorphism mapping onto , it is straightforward to infer that is in fact linear on . In particular, for all . Now [11, Corollary A1] yields that is linear on .
Next we consider the case and . Just as in the previous paragraph, there exists an such that for all . We infer that . Indeed, let . As there exists such that . This yields that . Therefore, is an order unit in and hence . Now let . Then there exists such that . We get . In particular, is an order unit and we conclude that . Hence . We remark that for all we have , in other words is positively homogeneous along the ray through . Therefore, the previous steps applied to instead of yield the converse inclusion . By the first part of the proof we obtain that is linear on . Since is the inf hull of the convex set , it follows from Lemma 3.13 that is linear on .
Suppose and are such that and . The order-isomorphism defined by maps to . By the previously considered case is linear, and hence is affine.
The general case where and are upper sets follows by arguments similar to those made in the proof of Theorem 1.1. Indeed, for every , is an order-isomorphism from to , so that is affine on by the previous case. Then extends to a unique affine map , which is independent of , as is directed.∎
To conclude the paper we provide an example to which Theorem 5.4 applies, but not Theorem 1.1. Consider the order unit space consisting of the real vector space , the Archimedean cone
[TABLE]
and the order unit . Then is complete and separable. The unit ball
[TABLE]
has four extreme points: and , where and denote the indicator functions of and , respectively. Therefore, has four extreme rays, namely the rays through and . As
[TABLE]
all four extreme rays are engaged, and which lies in is contained in the positive linear span of the engaged extreme rays. We conclude that the order unit space satisfies the conditions of Theorem 5.4. However, the inf-sup hull of the sum of the engaged extreme rays consist only of elements of the form , with and , and hence does not satisfy the conditions of Theorem 1.1.
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