Abstract
A gyrogroup, an algebraic structure that generalizes groups, is modeled on the bounded symmetric space of relativistically admissible velocities endowed with Einstein’s addition. Given a gyrogroup G, we offer a new way to construct a gyrogroup such that contains a gyro-isomorphic copy of G. We then prove that every strongly topological gyrogroup G can be embedded as a closed subgyrogroup of the path-connected and locally path-connected topological gyrogroup . We also study several properties shared by G and , including gyrocommutativity, first countability and metrizability. As an application of these results, we prove that being a quasitopological gyrogroup is equivalent to being a strongly topological gyrogroup in the class of normed gyrogroups.
Keywords:
topological gyrogroup; embedding of gyrogroup; normed gyrogroup; gyrogroup extension; quasitopological gyrogroup MSC:
Primary 22A30; Secondary 22A22, 20N05, 54H99
1. Introduction
The three-dimensional Einstein gyrogroup consists of the open c-ball in ,
where c is a positive constant representing the speed of light in vacuum and is the usual Euclidean norm, together with Einstein’s addition given by
In Equation (2), is the Lorentz factor given by and is the usual Euclidean inner product. The Einstein gyrogroup arises as a prominent example of a gyrogroup and motivates studying the general theory of gyrogroups. It is rich in structure and satisfies several sets of axioms. For instance, once suitable scalar multiplication is defined, it becomes a gyrovector space that provides a model for studying analytic hyperbolic geometry [1]. With the Euclidean topology, the Einstein gyrogroup forms a topological gyrogroup (cf. Example 3 of [2]). Indeed, it is a strongly topological gyrogroup, as mentioned in the remark after Example 3.1 of [3]. Assuming , the Einstein gyrogroup admits the gyronorm defined by and becomes a normed gyrogroup (cf. Theorem 2 of [4]). In fact, this gyronorm induces the rapidity metric (which turns out to be the Cayley–Klein metric) given by for all (cf. Theorem 3.9 of [5]). The presence of Einstein’s addition enables us to construct a point-reflection symmetry of the open unit ball in a convenient way. More precisely, for each point , there exists a point reflection of corresponding to —that is, is an isometry of such that is the identity transformation of and is the unique fixed point of . Indeed, , where is defined by and is the left gyrotranslation defined by for all (cf. Theorem 7 of [6]). Recent studies on Einstein gyrogroups can be found, for instance, in [6,7,8,9,10,11,12,13].
W. Atiponrat initiates the study of topological gyrogroups as a generalization of topological groups in [2] and then topological gyrogroups have been studied in some detail; see, for instance [3,4,14,15,16]. In particular, J. Wattanapan et al. prove that every locally compact Hausdorff topological gyrogroup can be embedded in a completely regular topological group as a twisted subset (cf. Theorem 3.9 of [16]). This inspires us to continue studying topological embedding of a generic topological gyrogroup. It is known in the literature that every topological group can be embedded in a path-connected and locally path-connected topological group (cf. Theorem 3.8.3 of [17]). In this article, we generalize this result to the case of strongly topological gyrogroups. We also investigate some algebraic and topological properties shared by the topological gyrogroup under consideration and its extension. We then give some applications of these results to examine normed gyrogroups.
2. Preliminaries
In this section, we collect relevant definitions in gyrogroup theory; for more details, see [1,18]. Standard terminology and notation in topology used throughout the article are defined as usual. All topologies mentioned in this article are assumed to be .
Let G be a nonempty set equipped with a binary operation ⊕ on G and let be the group of automorphisms of .
Definition 1
(Definition 2.7, [1]). A nonempty set G, together with a binary operation ⊕ on G, is called a gyrogroup if it satisfies the following axioms:
- (G1)
- There exists an element such that for all .
- (G2)
- For each , there exists an element such that .
- (G3)
- For all a, , there is an automorphism such thatfor all .
- (G4)
- For all a, , . (left loop property)
It can be proved that any gyrogroup has a unique two-sided identity, denoted by e, and that an element a of the gyrogroup has a unique two-sided inverse, denoted by . The automorphism is called the gyroautomorphism generated by a and b. The gyrogroup cooperation (cf. Definition 2.9, [1]) of a gyrogroup G, denoted by ⊞, is defined by
Let G be a gyrogroup. Define and for all . For each , the left gyrotranslation by a, denoted by , is defined by for all and the right gyrotranslation by a, denoted by , is defined by for all . Subgyrogroups, L-subgyrogroups and gyrogroup homomorphisms are defined in [18].
Definition 2
(Definition 3.17, [1]). A gyrogroup G is gyrocommutative if for all .
Definition 3
(Definition 3.32, [1]). Let G be a gyrogroup. An element is a two-torsion element if . If the only two-torsion element in G is e, we say that G is two-torsion-free.
Definition 4
(Definition 3.33, [1]). A gyrogroup G is two-divisible if for each element , there is an element such that .
Definition 5
(Definition 7, [18]). Let G be a gyrogroup. An element is said to have finite order if there is a number such that . If for all , a is said to have infinite order. The order of a is the least positive integer k (if any) such that , denoted by . In the case when a has infinite order, we write .
Definition 6
(Definition 1, [2]). A gyrogroup endowed with a topology is called a topological gyrogroup if the following statements hold:
- (T1)
- The binary operation is continuous. Here, is equipped with the product topology.
- (T2)
- The operation of taking inverses, , called the inversion function, is continuous.
3. Extended Gyrogroups and Their Properties
We follow the construction of S. Hartman and J. Mycielski (see, for instance, Section 3.8 in [17]) to construct an extension of an arbitrary gyrogroup G, which is also a gyrogroup containing an isomorphic copy of G. This gyrogroup will be a primary object studied in the next section when a certain topology is imposed. In this section, we focus on several algebraic properties that shared by G and .
Let G be a gyrogroup with identity e and let . A function is a step function if there are real numbers such that and f is constant on for all . Henceforward, when we say that is a partition of J, we include the condition that . Denote by the set of all step functions. Define an operation ⊕ on by
for all . Let . Note that is again a step function. Indeed, there are partitions and of J such that f and g are constant on and , respectively, for all and for all . Then, is another partition of J that refines both A and B. It follows that both f and g are constant on each subinterval partitioned by , and so is . Hence, is a step function.
Theorem 1.
forms a gyrogroup under the operation defined by Equation (4).
Proof.
Let be the function from J to G defined by for all . Then, acts as an identity of . Given , define a function by for all . Then, acts as an inverse of f in . For , define a function by
for all . It can be verified that belongs to and that the gyroassociative law and the left loop property hold in . ☐
Next, we show that G appears in as the subgyrogroup of constant functions. Let G be a gyrogroup. For each , define a function by for all . Clearly, .
Proposition 1.
The function defined by
is a gyrogroup monomorphism. Consequently, forms a subgyrogroup of that is isomorphic to G as gyrogroups.
Proof.
The proof that is a gyrogroup monomorphism is straightforward. By Proposition 24 of [19], is a subgyrogroup of . Furthermore, defines a gyrogroup isomorphism from G to so that . ☐
We list a few algebraic properties that shared by G and in Theorem 2. We show that any gyrogroup homomorphism from G to H can be naturally extended to a homomorphism from to in Theorem 3. We show that any pseudometric (respectively, metric) on G can be extended to a pseudometric (respectively, metric) on in such a way that the property of being (left) invariant is preserved in Theorem 4.
Theorem 2.
Let G be a gyrogroup. Then, G has one of the following properties if and only if has the same property:
- (i)
- being gyrocommutative;
- (ii)
- being two-torsion-free;
- (iii)
- being two-divisible;
- (iv)
- all elements having finite order.
Proof.
- (i)
- Suppose that G is gyrocommutative. Let and let . Then,Thus, , and so is gyrocommutative. The converse holds since G is isomorphic to a subgyrogroup of .
- (ii)
- Suppose that G is two-torsion-free. Let . Then, there is a number such that . It follows that . Thus, . This proves that is two-torsion-free. Conversely, assume that is two-torsion-free. Let . Then, , and so . It follows that . This proves that G is two-torsion-free.
- (iii)
- Suppose that G is two-divisible. Let and let . By assumption, for each , there is an element such that . Define a function by for for all . Clearly, . By definition of g, for all . Thus, is two-divisible. Conversely, assume that is two-divisible. Let . By assumption, there is a function such that . Thus, . Hence, G is two-divisible.
- (iv)
- Suppose that all the elements of G have finite order. Let and let . Since , all the elements of have finite order. The converse holds since G is isomorphic to a subgyrogroup of . ☐
Theorem 3.
Let G and H be gyrogroups and let be a gyrogroup homomorphism. Then, there exists a homomorphism extension of φ in the sense that . Furthermore, φ is injective (respectively, surjective) if and only if is injective (respectively, surjective).
Proof.
The homomorphism extension is defined by
for all . Suppose that is surjective. Let . Then, there is a partition of J such that h is constant on each interval . Since is surjective, there are elements such that for all . Define a function by , where . Clearly, and . Thus, is surjective. Conversely, suppose that is surjective. Let . By surjectivity, there is a function such that . Since , we obtain that is surjective. The remaining parts can be proved straightforwardly. ☐
Theorem 3 states that any gyrogroup homomorphism from G to H can be lifted to a gyrogroup homomorphism from and such that the following diagram commutes.
Theorem 4.
Let G be a gyrogroup. If d is a pseudometric (respectively, metric) on G, then d admits an extension to a pseudometric (respectively, metric) on . Furthermore, if d is (left) invariant or bounded, then has the same property.
Proof.
Let d be a pseudometric on G. Let . Then, there is a partition of J such that both f and g are constant on each interval . Define
Let . Then, for some and is a partition of J such that both f and g are constant on each subinterval. Note that
Hence, . By mathematical induction, if is a finite set, then . Now, let be another partition of J such that both f and g are constant on each subinterval. Then, is a partition of J such that both f and g are constant on each subinterval. Since and is a finite subset of ,
Similarly, , and so . This proves that does not depend on A.
Next, define a function by
where A is a partition of J as in the previous paragraph, for all . The argument above shows that is well defined. Clearly, and for all . Note also that
for all . Next, we show that is a pseudometric. If , then
and so . Let . Then, there is a partition of J such that and h are constant on each interval . Direct computation shows that
Thus, is a pseudometric on .
Next, suppose that d is a metric on G. Let with . Then, there is a partition of J such that f and g are constant on each interval . Since , we have for some . Then,
Thus, is a metric on . Clearly, if d is bounded, then so is .
Suppose that d is left invariant. Let . Then, there is a partition of J such that and h are constant on each interval . Direct computation shows that
This proves that is left invariant. Similar arguments apply to the case when d is invariant. ☐
4. Embedding of Strongly Topological Gyrogroups
In this section, we focus on topological properties of G and . In particular, we show that if a gyrogroup G has a certain nice family of its subsets, then G can be topologized. With this result, we can topologize the extended gyrogroup , when G is a strongly topological gyrogroup, in such a way that contains a homeomorphic copy of G. We begin with proving Theorem 5, which is an extension of the first part of Theorem 1.3.12 of [17] to topological gyrogroups. However, in order to obtain the converse of Theorem 1.3.12 of [17] for the case of gyrogroups, we need to impose an additional gyro-condition. This condition seems to be natural and is introduced by M. Bao and F. Lin in [3]. The converse of Theorem 1.3.12 of [17] is generalized to the case of gyrogroups in Theorem 6.
Theorem 5.
Let G be a topological gyrogroup and let be an open base at the identity e of G. Then, the following hold:
- (i)
- for every , there is a set such that ;
- (ii)
- for all , there is a set such that ;
- (iii)
- for all , there is a set such that ;
- (iv)
- for all , there is a set such that , , and ;
- (v)
- for all , there is a set such that ;
- (vi)
- .
Proof.
- (i)
- Let . Since the operation ⊕ is continuous and , there are sets such that . Since is an open base at e, there is a set such that . Hence, .
- (ii)
- Let and let . Since G is a topological gyrogroup, the function is continuous. Note that . By the continuity of , there is a set such that .
- (iii)
- Let and let . Then, is an open neighborhood of e for is open. Since is an open base at e, there is a set such that . Thus, .
- (iv)
- Let and let . Since G is a topological gyrogroup, the function is continuous. Note that for all . Note also that is an open neighborhood of . Since , there is a set such that . Similarly, one can show that there are sets such that and . Since is an open base at e, there is a set such that , and the assertion follows.
- (v)
- The assertion follows directly from the definition of an open base.
- (vi)
- Clearly, . Let . Since G is , there is a set such that . Thus, . This shows that . ☐
Definition 7
(p. 5116, [3]). A topological gyrogroup G is strong if there exists an open base at the identity e of G such that for all . In this case, we say that G is a strongly topological gyrogroup with open base at e.
The property of being invariant under gyroautomorphisms mentioned in the previous definition arises naturally when one tries to extend theorems for topological groups to topological gyrogroups. Furthermore, several well-known gyrogroups in the literature, including Einstein, Möbius and Proper Velocity gyrogroups, are indeed strongly topological gyrogroups. We prove basic properties of strongly topological gyrogroups in Propositions 2 and 3 and extend the converse of Theorem 1.3.12 of [17] to Theorem 6.
Proposition 2.
Let G be a strongly topological gyrogroup with open base at e and let H be a subgyrogroup of G. Then, H is a strongly topological gyrogroup with open base at e.
Proof.
Clearly, H is a topological gyrogroup and the family is an open base for H at e. Let and let . Then, . Therefore, H is a strongly topological gyrogroup with open base at e. ☐
Proposition 3.
Let G be a strongly topological gyrogroup with open base at e. If , then is a strongly topological gyrogroup.
Proof.
By Theorem 4.7 of [20], is a topological gyrogroup. By Proposition 35 of [18], H is an L-subgyrogroup of G. It follows from Theorem 3.7 of [3] that the canonical homomorphism is continuous and open. Hence, the family is an open base for at . Let , let , and let . Then,
Thus, for all . It follows from Proposition 24 of [18] that for all . Hence, is a strongly topological gyrogroup. ☐
The following theorem provides one way to topologize a gyrogroup based on Theorem 5.
Theorem 6.
Let G be a gyrogroup and let be a family of subsets of G that satisfies the following properties:
- (i)
- for every , there is a set such that ;
- (ii)
- for all , there is a set such that ;
- (iii)
- for all , there is a set such that ;
- (iv)
- for all , there is a set such that , , and ;
- (v)
- for all , there is a set such that ;
- (vi)
- ;
- (vii)
- for all , .
Then, the family forms a base for a -topology on G. With this topology, G is a topological gyrogroup, and the family is a base for the same topology on G.
Proof.
Let U be a family of subsets of G such that items (i) through (vii) hold. Define
Claim 1.
is a topology on G.
Clearly, ∅ and G are in . Let be a subfamily of and let . Then, for some and there is a set such that . Hence, , and so . Let and be in . If , then there are sets and in such that and . By item (v), there is a set such that and hence . Therefore, . This proves that is a topology on G.
Claim 2.
for all .
Let . Then, . By item (iii), there is a set such that . It follows from the left gyroassociative law and item (vii) that
Thus, .
Claim 3.
The family is a base for .
The claim follows directly from the definition of and Claim 2.
Claim 4.
The multiplication in G is jointly continuous with respect to .
Let and let with . Then, there is a set such that . By item (i), there is a set such that . By item (iv), there is a set such that . By Claim 2, . Direct computation shows that
This proves the claim.
Claim 5.
for all .
Let . Then, and there is a set such that . By item (iv), there is a set such that . This implies that .
Claim 6.
The function ⊖ from G to itself given by is continuous with respect to .
Let and let . Then, there is a set such that . By item (ii), there is a set such that . Note that by Claim 5. Thus, . This proves that the inversion function is continuous.
Finally, G is since for all . If and , then there is a set such that by item (iv). This implies that . Therefore, the family is also a base for . ☐
Corollary 1.
If G is a gyrogroup that fits Theorem 6, then G becomes a strongly topological gyrogroup with respect to the topology defined by Equation (8).
Proof.
The family in Theorem 6 is an open base at e satisfying Definition 7. ☐
Using Theorem 6, we can topologize the extended gyrogroup in the case when G is a strongly topological gyrogroup, as shown in the following theorem. Let G be a topological gyrogroup. Given an open neighborhood V of e in G and a real number , define
where is the Lebesgue measure on the real line.
Theorem 7.
Let G be a strongly topological gyrogroup with open base at e. Then, the family
forms a base of a Hausdorff topology on , and becomes a strongly topological gyrogroup.
Proof.
It suffices to show that the family satisfies Theorem 6.
- (i)
- Let . Then, there is a set such that . Let . Note that Hence,This shows that .
- (ii)
- Let and let . Then, there is a partition of J such that f is constant on each interval . By item (ii) of Theorem 5, for each , there is a set such that . By item (v) of Theorem 5, there is a set such that . Thus, for all . Let . Then,It follows that , and so . This shows that .
- (iii)
- Let . Then, there is a partition of J such that f is constant on each interval . SetBy item (iii) of Theorem 5, for each , there is a set such that . By item (v) of Theorem 5, there is a set such that . Thus, whenever . Put . If , thenIt follows thatThus, . This proves that .
- (iv)
- Let and let . Then, there is a partition of J such that both f and g are constant on each interval . By item (iv) of Theorem 5, for each , there is a set such thatBy item (v) of Theorem 5, there is a set such that . Furthermore,for all . Let . Then,Hence, . It follows that , and so . This shows that . Similarly, one can show that and that .
- (v)
- Let , let , and let . Note that if , thenTherefore, . Note that if , then implies . This shows that . Let . By item (v) of Theorem 5, there is a set such that . Put . The arguments above show that .
- (vi)
- Clearly, for all . Let . Then, there exists a subinterval such that f is constant on and . By item (vi) of Theorem 5, there is a set such that . Then, . It follows that . Thus, . This shows that .
- (vii)
- Let , let , and let . It follows from the assumption thatThus, , which implies . This proves that .
Therefore, the family forms a base of a -topology on . By Corollary 1, is strong and by Theorem 3 of [2], is Hausdorff. In addition, the family
is also a base for the same topology. ☐
Remark 1.
From the definition of the topology on , if , then
individually, form open bases for at f.
Next, we prove several topological properties shared by G and , where G is a strongly topological gyrogroup. Proposition 4 shows that any two open bases of G at the gyrogroup identity generate the same topology on . Theorem 8 shows that is always path-connected and locally path-connected. Theorems 9 and 10 show that being first countable and being metrizable are preserved under the process of taking •, respectively.
Proposition 4.
Let G be a strongly topological gyrogroup with open bases and at e. Then, the two bases
and
generate the same topology on .
Proof.
Let and let . Then, there is a set such that . Hence, . This shows that . By the sake of symmetry, . ☐
Theorem 8.
is path-connected and locally path-connected for any strongly topological gyrogroup G.
Proof.
Note that if is path-connected for all , then is locally path-connected since every topological gyrogroup is a homogeneous space (cf. Proposition 3 of [2]).
Let and let . Then, there is a partition of J such that f is constant on each interval . Given and , put . Note that for all . Let . Define a function as follows. ; ; for , note that if , then for some k, so we define by
for all . Clearly, for all . Furthermore, we have
and so for all . Define a function by for all . To show that is continuous, let and let be an open neighborhood of . Let . Then, . Since
it follows that . Hence, , and so . This shows that is continuous. Therefore, is path-connected, and so is locally path-connected. In particular, if , then . It follows that is path-connected. ☐
Theorem 9.
Let G be a strongly topological gyrogroup with open base at e. If G is first countable, then so is .
Proof.
Suppose that G is first countable. Then, there is a countable open base . Thus, the family is a countable open base at . Therefore, is first countable. ☐
Theorem 10.
Let G be a strongly topological gyrogroup. If G is metrizable, then so is .
Proof.
Recall that is Hausdorff. Suppose that G is metrizable. Then, G is first countable. By Theorem 9, is first countable. By Theorem 2.3 of [14], is metrizable. ☐
The next proposition shows that every strongly topological gyrogroup can be topologically embedded in a path-connected and locally path-connected topological gyrogroup. As every group is a strongly topological gyrogroup, this result extends a known result in the theory of topological groups. See, for instance, Section 3.8 of [17].
Proposition 5.
For any strongly topological gyrogroup G, the function defined in Proposition 1 is a topological embedding. Furthermore, forms a closed subgyrogroup of .
Proof.
By Proposition 1, is a monomorphism and is a subgyrogroup of . Next, we show that the function and its inverse are continuous.
Let . Note that for all ,
Let . Then, for each , we have . Thus, is continuous at x.
Next, let . Then, for each , we have . Thus, is continuous at . This proves that is a topological embedding.
The remaining part is to show that is a closed subset of . Let . Then, there are numbers and satisfying such that f is constant on and with . Since , there is an open set such that . Put . We claim that . Suppose that for some . Then, . We have
Thus, . Since f is constant on ,
Similarly, . This means that if , then . Hence, and . Thus, , a contradiction. Hence, . ☐
The following theorem is a topological version of Theorem 4. This theorem proves useful in studying normed gyrogroups, as illustrated in Section 5.
Theorem 11.
Let G be a strongly topological gyrogroup with open base at e. If d is a bounded pseudometric (respectively, metric) on G, then d admits an extension to a bounded pseudometric (respectively, metric) on such that
- (i)
- if d is continuous, then so is ;
- (ii)
- if d is a metric generating the topology of G, then also generates the topology of .
Proof.
The first part of the theorem follows from Theorem 4. Next, suppose that d is continuous. Without loss of generality, we may assume that d is bounded by 1. To prove the continuity of , we need to show that for all , there are a set and a number such that
Suppose that . For each , because d is continuous and , there is an open neighborhood of with . In particular, for all . Since is an open neighborhood of , we have is an open neighborhood of e, and so there is a set such that . If and , we have . It follows that
for all and . We claim that —that is, if . Let . Then, there is a partition of J such that f and g are constant on each interval . For each , let and be the values of f and g on , respectively. Note that . Set and . Note that if , then and that if , then . Furthermore, we have , and so . By definition of ,
Therefore, . Let and let . Then, there are basic open sets and such that and If and , then
On the other hand,
This shows that , and so is in . Hence, is continuous at .
Finally, suppose that d is a metric on G generating the topology of G. Let and let be a basic open neighborhood of f in . Suppose that . Then, there exists a number such that for all . Note that if and , then . Put . We claim that . Let . Then, there exists a partition of J such that f and g are constant on each interval . For each , let and be the values of f and g on , respectively. Note that . Set
If , then , and so . It follows that
Hence, . Recall that . We have
Hence, . This shows that , and so . Hence, . Let be the topology on induced by and let , which is a base for . Hence, each basic open set is a union of elements in . Let be the topology on . Since is continuous with respect to , for each , the function defined by for all is continuous (being the restriction of to ). It follows that is open with respect to . Hence, . ☐
In view of Theorem 11, one might wonder whether is complete in the case when is a complete metric space. The following example shows that the answer is negative.
Example 1.
Consider the group equipped with the discrete metric d. Clearly, is a complete strongly topological gyrogroup and the discrete metric d is bounded. For each , define a function by
Obviously, for all . Next, define ; if , define
Note that for all . Note also that for each ,
Moreover, for each , we have . Thus, is a Cauchy sequence in . Suppose that . Since , there is a number such that f is constant on . By definition of the sequence , there is an integer such that . It follows that for all , a contradiction. Therefore, is not complete.
Following the proof of Theorem 4, we prove that any continuous real-valued bounded function on a strongly topological gyrogroup G can be extended to a continuous real-valued bounded function on .
Theorem 12.
Let F be a continuous real-valued bounded function on a strongly topological gyrogroup G. Then, F admits an extension to a continuous real-valued bounded function on .
Proof.
Let G be a strongly topological gyrogroup with open base at e and let be a continuous function. Without loss of generality, we may assume that F is bounded by 1. For each , there is a partition of J such that g is constant on each interval . Define a function by
It is not difficult to see that is well defined and bounded by 1. Let and let . Suppose that . Since F is continuous, there is a set such that for all . In other words, there is a set such that
for all . We claim that —that is, for all . Let . Then, there is a partition of J such that both g and f are constant on each interval . Set . It follows that . Since , . Now, consider
Thus, is continuous at g. Since g is arbitrary, is continuous on . ☐
We close this section with a topological version of Theorem 3.
Theorem 13.
Let G and H be strongly topological gyrogroups. If is a continuous homomorphism, then the function , defined by for all , is a continuous homomorphism that extends φ in the sense that . Furthermore, if φ is open and surjective, then so is .
Proof.
By Theorem 3, is a homomorphism that extends . To show that is continuous, let and let be a basic open neighborhood of in . Since is continuous, there is a set such that . Let . Then,
It follows that . Thus, . Hence, if , then . This shows that is continuous.
Suppose that is open and surjective. By Theorem 3, is surjective. To show that is open, let be a basic open neighborhood at and let . Note that
Thus, . Hence, . This shows that . Let . Then, there is a partition of J such that h is constant on each interval . Set . If , then there is an element such that . If , then there is an element such that . Define a function by
Clearly, . It follows that . By definition of L, . Hence, . Since , we have . Thus, . Let . Then, for some k and . This shows that , and so . Let . We show that . Since is surjective, there are elements such that and . Let . By Proposition 23 (3) of [19], . Thus, for all . It follows from Proposition 4 that is open. ☐
5. An Application to Normed Gyrogroups
In this section, we present an application of results in Section 4 to normed gyrogroups. The notion of a normed gyrogroup is introduced in [4]; we recall its definition as follows.
Definition 8
(Definition 2, [4]). A real-valued function on a gyrogroup G is called a gyronorm if it satisfies the following properties:
- 1.
- for all and if and only if ;
- 2.
- for all ;
- 3.
- for all ;
- 4.
- for all .
The pair is called a normed gyrogroup.
According to Theorem 1 of [4], any gyronorm on G induces a metric, called the gyronorm metric, given by
for all so that forms a metric space. Throughout this section, let denote the topology on a normed gyrogroup generated by , called the gyronorm topology. We remark that a normed gyrogroup endowed with the gyronorm topology need not be a topological gyrogroup. However, we obtain a sufficient condition for a normed gyrogroup to be a topological gyrogroup with respect to the gyronorm topology as an application of Theorem 6. We begin with proving basic properties of normed gyrogroups in Propositions 6 through 8.
Proposition 6.
Let G be a normed gyrogroup. If
for all , then the inversion function ⊖ is continuous.
Proof.
By assumption, for all . This shows that ⊖ is an isometry of G, and so ⊖ is continuous. ☐
Corollary 2.
The inversion function of any gyrocommutative normed gyrogroup is continuous.
Proof.
The corollary follows since . ☐
Proposition 7.
Let G be a normed gyrogroup. If the inversion function and all the right gyrotranslations are continuous, then every right gyrotranslation is a homeomorphism.
Proof.
It suffices to show that every right gyrotranslation has the continuous inverse. Let . Note that for all . Define a function by for all . Note that
for all . Thus, , and so is continuous. By Theorem 2.38 of [1], for all . Hence, for all . It follows that , and so is continuous. ☐
Remark 2.
It should be emphasized that Proposition 7 is valid for any gyrogroup with a topology such that all the left gyrotranslations are continuous.
Proposition 8.
Let G be a normed gyrogroup. If is a topological gyrogroup, then is a strongly topological gyrogroup.
Proof.
Let denote the open ball in G centered at z with radius . It is clear that the family is an open base for G at e. Let and let . For each ,
This shows that . Therefore, G is a strongly topological gyrogroup with respect to . ☐
Like several theorems in Section 4, any gyronorm on a gyrogroup G can be extended to a gyronorm on in a natural way, as shown in the following theorem.
Theorem 14.
Any gyronorm on a gyrogroup G induces a gyronorm on such that for all . Furthermore, if is a strongly topological gyrogroup and is bounded, then is a strongly topological gyrogroup and is bounded, where is the gyronorm topology associated to the extended metric .
Proof.
Let be a gyronorm on G. Then, induces the left-invariant gyronorm metric on G by Theorems 1 and 9 of [4]. By Theorem 4, can be extended to the left-invariant metric on . By Theorem 9 of [4], the function defined on by is a gyronorm on that generates the same metric. Note that for all . Next, suppose that is a strongly topological gyrogroup and that is bounded. Hence, is bounded. By Theorem 11, is bounded and generates the topology of described in the proof of Theorem 7. Therefore, is a strongly topological gyrogroup on which is bounded. ☐
As proved in Theorem 10 of [4], if G is a normed gyrogroup, then the following conditions are equivalent:
(Right-gyrotranslation inequality) for all ;
(Klee’s condition) for all .
These are some sufficient conditions for a normed gyrogroup to be a topological gyrogroup with respect to the gyronorm topology; see Theorem 11 of [4].
Proposition 9.
Let G be a normed gyrogroup. If satisfies one of the conditions mentioned previously, then so does .
Proof.
Suppose that satisfies the right-gyrotranslation inequality. Let . Then, there is a partition of J such that and h are constant on each interval . Direct computation shows that
Thus, satisfies the right-gyrotranslation inequality. ☐
We are now in a position to prove the main result of this section, which gives another sufficient condition for a normed gyrogroup to be a topological gyrogroup. This shows a nice application of Theorem 6. We start with the following lemma, demonstrating that the left gyrotranslation of any open ball in a normed gyrogroup is again an open ball with the same radius.
Lemma 1.
Let G be a normed gyrogroup. Then, for all .
Proof.
Let and let . Since is left invariant, we obtain
which completes the proof. ☐
Theorem 15.
Let G be a normed gyrogroup. If every right gyrotranslation and the inversion function are continuous, then G is a topological gyrogroup with respect to the gyronorm topology.
Proof.
Suppose that every right gyrotranslation and the inversion function are continuous. Let . We show that fits Theorem 6.
- (i)
- Let . If , thenThus, .
- (ii)
- Let and let . By assumption, the function is continuous and there is a number such that . Thus, .
- (iii)
- Let and let . Put . If , thenTherefore, .
- (iv)
- Let and let . By Proposition 7, the function , given by for all , is continuous. Note that . Since is continuous, there is a number such thatSimilarly, there are numbers such that and . Put . Then, the ball does the job.
- (v)
- Let . Then, , where .
- (vi)
- Let . Then, .
- (vii)
- Let and let . If , thenThus, .
It follows from Theorem 6 that G is a topological gyrogroup with respect to the topology generated by the base . By Lemma 1,
Since the family on the right hand side is a base for the gyronorm topology, it follows that G becomes a topological gyrogroup with respect to the gyronorm topology. ☐
Following terminology in the literature, we introduce the notion of a quasitopological gyrogroup as follows.
Definition 9.
Suppose that G is a gyrogroup with a topology. We say that G is a quasitopological gyrogroup if all the left gyrotranslations, all the right gyrotranslations and the inversion function are continuous.
Definition 9 extends the usual definition of a quasitopological group since every group can be viewed as a gyrogroup with trivial gyroautomorphisms. It should be emphasized that there exists a quasitopological gyrogroup that is not a topological gyrogroup. In fact, any infinite group K with the cofinite topology (that is, X is open in K if and only if or is finite) is a quasitopological group that is not a topological group; see Example 1.2.5 (b) of [17]. However, in light of Theorem 15, we obtain a remarkable result that being a quasitopological gyrogroup is equivalent to being a strongly topological gyrogroup in the class of normed gyrogroups, as shown in the following theorem.
Theorem 16.
Let G be a normed gyrogroup. Then, the following are equivalent:
- (i)
- is a quasitopological gyrogroup;
- (ii)
- is a topological gyrogroup;
- (iii)
- is a strongly topological gyrogroup.
Proof.
The theorem is a consequence of Theorem 15 and Proposition 8. ☐
We close this section with the remark that the Einstein gyrogroup provides a concrete example of Theorem 16. In fact, in addition to the gyronorm , the Euclidean norm is a gyronorm on the Einstein gyrogroup (cf. [4] p. 534) that generates the same topology as does. It can be shown that the Euclidean gyronorm generates the Euclidean topology on the Einstein gyrogroup. Therefore, is a normed gyrogroup that fits Theorem 16. This also implies that the Einstein gyrogroup forms a topological gyrogroup with respect to the gyronorm topology associated to . It seems to be difficult to have a direct proof of this result because of complication of Einstein’s addition formula.
Author Contributions
Conceptualization, W.A. and T.S.; methodology, J.W., W.A. and T.S.; validation, W.A. and T.S.; investigation, J.W., W.A. and T.S.; writing—original draft preparation, J.W. and T.S.; writing—review and editing, W.A. and T.S.; visualization, T.S.; supervision, W.A. and T.S.; project administration, T.S. All authors have read and agreed to the published version of the manuscript.
Funding
Part of this research was supported by the Research Center in Mathematics and Applied Mathematics, Chiang Mai University.
Conflicts of Interest
The authors declare no conflict of interest.
References
- Ungar, A.A. Analytic Hyperbolic Geometry and Albert Einstein’s Special Theory of Relativity; World Scientific: Hackensack, NJ, USA, 2008. [Google Scholar]
- Atiponrat, W. Topological gyrogroups: Generalization of topological groups. Topol. Appl. 2017, 224, 73–82. [Google Scholar] [CrossRef]
- Bao, M.; Lin, F. Feathered gyrogroups and gyrogroups with countable pseudocharacter. Filomat 2019, 33, 5113–5124. [Google Scholar] [CrossRef]
- Suksumran, T. On metric structures of normed gyrogroups. In Mathematical Analysis and Applications; Volume 154: Springer Optimization and Its Applications; Rassias, T.M., Pardalos, P.M., Eds.; Springer: Cham, Switzerland, 2019; pp. 529–542. [Google Scholar]
- Kim, S.; Lawson, J. Unit balls, Lorentz boosts, and hyperbolic geometry. Results Math. 2013, 63, 1225–1242. [Google Scholar] [CrossRef]
- Suksumran, T. The isometry group of n-dimensional Einstein gyrogroup. In Computational Mathematics and Variational Analysis; Volume 159: Springer Optimization and Its Applications; Daras, N.J., Rassias, T.M., Eds.; Springer: Cham, Switzerland, 2020; pp. 505–512. [Google Scholar]
- Honma, T.; Hatori, O. A gyrogeometric mean in the Einstein gyrogroup. Symmetry 2020, 12, 1333. [Google Scholar] [CrossRef]
- Barabanov, N.E.; Ungar, A.A. Differential geometry and binary operations. Symmetry 2020, 12, 1525. [Google Scholar] [CrossRef]
- Friedman, Y.; Scarr, T. Symmetry and special relativity. Symmetry 2019, 11, 1235. [Google Scholar] [CrossRef]
- Ferreira, M.; Suksumran, T. Orthogonal gyrodecompositions of real inner product gyrogroups. Symmetry 2020, 12, 941. [Google Scholar] [CrossRef]
- Molnár, L.; Virosztek, D. On algebraic endomorphisms of the Einstein gyrogroup. J. Math. Phys. 2015, 56, 082302. [Google Scholar] [CrossRef]
- Frenkel, P.E. On endomorphisms of the Einstein gyrogroup in arbitrary dimension. J. Math. Phys. 2016, 57, 032301. [Google Scholar] [CrossRef]
- Barabanov, N.E.; Ungar, A.A. Binary operations in the unit ball: A differential geometry approach. Symmetry 2020, 12, 1178. [Google Scholar] [CrossRef]
- Cai, Z.; Lin, S.; He, W. A note on paratopological loops. Bull. Malays. Math. Sci. Soc. 2019, 42, 2535–2547. [Google Scholar] [CrossRef]
- Atiponrat, W.; Maungchang, R. Complete regularity of paratopological gyrogroups. Topol. Appl. 2020, 270, 106951. [Google Scholar] [CrossRef]
- Wattanapan, J.; Atiponrat, W.; Suksumran, T. Embedding of locally compact Hausdorff topological gyrogroups in topological groups. Topol. Appl. 2020, 273, 107102. [Google Scholar] [CrossRef]
- Arhangel’skii, A.; Tkachenko, M. Topological Groups and Related Structures; Volume 1, Atlantis Studies in Mathematics; Atlantis Press: Paris, France; World Scientific: Hackensack, NJ, USA, 2008. [Google Scholar]
- Suksumran, T. The algebra of gyrogroups: Cayley’s theorem, Lagrange’s theorem, and isomorphism theorems. In Essays in Mathematics and Its Applications; Rassias, T.M., Pardalos, P.M., Eds.; Springer: Cham, Switzerland, 2016; pp. 369–437. [Google Scholar]
- Suksumran, T.; Wiboonton, K. Isomorphism theorems for gyrogroups and L-subgyrogroups. J. Geom. Symmetry Phys. 2015, 37, 67–83. [Google Scholar]
- Atiponrat, W.; Maungchang, R. Continuous homomorphisms, the left-gyroaddition action and topological quotient gyrogroups. Quasigroups Relat. Syst. 2020, 28, 17–28. [Google Scholar]
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations. |
© 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).