1. Introduction
The octonions
form the largest of the four normed division algebras over the real numbers, following the real numbers
themselves, the complex numbers
, and the quaternions
. In contrast to these algebras, the octonions are neither commutative nor associative, but they satisfy a weaker form of associativity known as alternativity, meaning that every subalgebra generated by two elements is associative [
1]. The complexified octonions
inherit this non-associative algebraic structure while gaining the rich analytic properties of complex manifolds. The automorphism group of
is the simple complex Lie group of exceptional type
, which is a 14-dimensional complex group and the complexification of the compact exceptional Lie group
[
1,
2,
3]. More precisely, the group
can be characterized as the subgroup of
that preserves the octonionic multiplication and the standard inner product [
1]. The Lie algebra
of
can be realized as the derivations of
that preserve the octonionic multiplication:
Let X be a compact Riemann surface of genus . The main object of interest in this paper is the moduli space of octonionic bundles over X. An octonionic bundle E over X can be viewed as a holomorphic fiber bundle with fiber and structure group . This can be equivalently understood as a principal -bundle E together with the associated bundle construction , where acts on through its natural action as the automorphism group. Thus, an octonionic bundle can be equivalently viewed as a principal -bundle over X, allowing us to apply the theory of principal bundles and the geometry of to study octonionic structures.
Through this identification, suitable notions of stability and polystability for octonionic bundles are derived from those of principal bundles, as provided by Ramanathan [
4,
5,
6] for any reductive complex Lie structure group. Thus the moduli space
of octonionic bundles over
X is a complex algebraic variety parametrizing isomorphism classes of polystable octonionic bundles, which can be identified with the moduli space
of principal
-bundles over
X. This identification reflects the fact that every octonionic bundle corresponds to a unique principal
-bundle.
The non-associative nature of the octonions is linked to exceptional structures in geometry, with
-holonomy in seven-dimensional manifolds being a particularly interesting and deeply studied topic [
7]. The geometric study of the moduli space of principal
-bundles over curves and related structures, such as
-Higgs bundles, has attracted recent attention in algebraic geometry [
7,
8,
9,
10]. A fruitful line of research analyzes how the moduli space
embeds into larger moduli spaces, from which topological and geometric properties arise [
11]. This aligns with work on moduli spaces of bundles with exceptional structure groups, yielding geometric and physical consequences [
12,
13].
In the study of moduli spaces of principal bundles, understanding the geometric structure of embeddings between these spaces provides valuable insights. The main objective of this paper is to rigorously establish and analyze the embedding of the moduli space of octonionic bundles into the moduli space of principal
-bundles. The group
is naturally embedded into the simple complex Lie group
[
3], and this Lie group inclusion induces a forgetful map from
to the moduli space
, which sends each octonionic bundle with underlying principal
-bundle
E to the principal
-bundle
.
Our first main result, proved in Theorem 1, establishes that this forgetful map is a closed embedding, showing that the moduli space of octonionic bundles can be viewed as a closed subvariety of the moduli space of principal
-bundles. The proof proceeds in three steps. First, we establish set-theoretic injectivity by showing that the forgetful map is injective on points and that semistability is preserved under the embedding. This requires a technical result describing how parabolic subgroups and their characters behave under the embedding
, developed in Proposition 1. Second, we prove in Proposition 2 that the differential of the embedding is injective at smooth points corresponding to stable bundles. This uses deformation theory and a cohomological analysis involving the exact sequence
where
is the orthogonal complement of
in
, isomorphic to the seven-dimensional fundamental representation of
. Third, in Proposition 3, we extend the injectivity of the differential to singular points of the moduli space using Luna’s étale slice theorem. This has not been addressed in previous work on similar embeddings. At singular points corresponding to strictly semistable bundles, we use the local description of the moduli space as a quotient of an affine slice by a reductive stabilizer group, and show that the differential remains injective by analyzing the equivariant structure. Finally, the properness of the embedding follows from the valuative criterion: from the result of Balaji–Seshadri [
14], semistable families extend over DVR base changes, and the
-reduction extends uniquely from the result of Drinfeld–Simpson [
15], using the fact that
is an affine variety and
X has a cohomological dimension of one.
The second main result of the paper, established in Theorem 2, analyzes the normal bundle to this embedding. We show that at a smooth point corresponding to a stable octonionic bundle, the fiber of the normal bundle is canonically isomorphic to , and in particular the normal bundle has rank . This result establishes that the embedding has codimension in the ambient space, as confirmed in Corollary 1, which can be verified both by dimensional considerations ( and ) and by analyzing the tangent spaces using the cohomological long exact sequence.
We further develop applications of the above main results to deformation theory. Specifically, Proposition 4 shows that for a stable octonionic bundle E, the tangent space is canonically isomorphic to and has dimension . Moreover, the differential of the embedding identifies this tangent space with a -dimensional subspace of the -dimensional tangent space . This provides an explicit cohomological framework for understanding infinitesimal deformations of octonionic bundles and how they relate to deformations of the underlying -structure. The injectivity of the differential reflects the geometric fact that the -structure is more rigid than the underlying -structure, meaning that every infinitesimal deformation of a -bundle induces a unique infinitesimal deformation of the associated -bundle, but not every infinitesimal deformation of an -bundle preserves the -structure.
Some consequences of the embedding are also derived as applications of the main results. Thus, Proposition 5 establishes that the image of
is a closed irreducible subvariety of
that intersects the smooth locus in a dense open subset and is not contained in the singular locus. Proposition 6 shows that the embedding gives rise to an exact sequence of holomorphic vector bundles
over the smooth locus
, where
T is the tangent bundle of
,
is the pullback of the ambient tangent bundle, and
N is the normal bundle. The Whitney sum formula then yields the identity
in
, providing a structural constraint relating the characteristic classes of
, the normal bundle, and the ambient moduli space. In particular, the first Chern class of the normal bundle satisfies
expressing the anticanonical class of
in terms of the pullback of the anticanonical class of the ambient space and
.
The structure of this paper is as follows.
Section 2 introduces octonionic bundles and establishes their equivalence with principal
-bundles, including the crucial result that all such bundles are topologically trivial.
Section 3 contains the proof of the closed embedding theorem, beginning with the analysis of parabolic subgroups and characters, establishing set-theoretic injectivity and preservation of semistability, proving differential injectivity at smooth points, extending to singular points using Luna’s theorem, and completing the proof using the valuative criterion. The analysis of the normal bundle is developed in
Section 4 by computing its rank and providing the cohomological description of fibers. The applications to deformation theory, consisting on the explicit computation of the tangent spaces and the analysis of how infinitesimal deformations of octonionic bundles relate to deformations of
-bundles, are given in
Section 5. In
Section 6, the main geometric consequences of the embedding are derived, establishing irreducibility of the image and the Whitney formula relating the characteristic classes of the tangent bundle, the normal bundle, and the pullback of the ambient tangent bundle. Finally,
Section 7 summarizes our main results and discusses open questions for future research.
2. Octonionic Bundles over a Riemann Surface
Throughout the paper, X will be a compact Riemann surface of genus and, for a principal G-bundle P over X and a representation , we denote by the associated vector bundle with fiber V. In particular, for the adjoint representation , we write for the adjoint bundle. When the group G needs to be specified, we may write to emphasize the structure group.
In this section, the notion of octonionic bundle is formally recalled, and octonionic bundles are related to principal -bundles over X.
Definition 1. An octonionic bundle E over the compact Riemann surface X is a fiber bundle whose fiber is the algebra of complex octonions and whose structure group is .
The structure group of an octonionic bundle over
X can be identified with the simple complex Lie group of exceptional type
, which acts on the fiber
via automorphisms. Indeed, the complex octonions
form an eight-dimensional non-associative algebra over
, and the automorphism group of
, which preserves the algebra structure, including the non-associative multiplication, is
, the complex form of the exceptional Lie group
[
2,
3,
7]. This isomorphism can be explicitly constructed by noting that
is the subgroup of
that preserves a particular three-form, which corresponds to the structure constants of the octonion multiplication. Thus, the structure group of an octonionic bundle is
. Consequently, giving an octonionic bundle over
X is equivalent to giving a principal
-bundle over
X.
Lemma 1. Let X be a compact Riemann surface of genus . Then, the topological classification of octonionic bundles over X is given by elements of the cohomology . Moreover, since is simply connected, all octonionic bundles over X are topologically trivial.
Proof. For a principal
G-bundle
P over a surface
X, the topological classification is given by elements of
[
16]. Since
is simply connected, i.e.,
[
2,
3], it follows that
. Thus, all octonionic bundles over
X are topologically trivial, distinguished only by their holomorphic structures. □
The moduli space of octonionic bundles over
X, which will be denoted by
, parametrizes isomorphism classes of polystable octonionic bundles. Two octonionic bundles are isomorphic as principal
-bundles over
X if there exists a
-equivariant bundle isomorphism between them covering the identity on
X. The moduli space is defined as
the moduli space of polystable principal
-bundles over
X, with the stability notion established by Ramanathan [
4,
5,
6]. This space is a complex variety of dimension
. Reduced notions of
-bundles have also been provided in the preceding literature [
8].
4. The Normal Bundle Structure
Given a closed embedding of complex varieties
, the normal bundle
is defined at each smooth point
as the cokernel of the differential [
24]:
Understanding the normal bundle provides geometric information about how
Y sits inside
Z.
We study the normal bundle of the embedding
established in Theorem 1.
Theorem 2. Let X be a compact Riemann surface of genus . At a smooth point corresponding to a stable -bundle E, the fiber of the normal bundle to the embedding is canonically isomorphic towhere is the orthogonal complement of in with respect to the Killing form, isomorphic as a -representation to the irreducible seven-dimensional fundamental representation. In particular, the normal bundle has rank .
Proof. At a smooth point
where
E is stable, both moduli spaces are smooth, and the tangent spaces are given by
where
is the adjoint bundle and
.
The Lie algebra decomposition
, where
is the orthogonal complement of
with respect to the Killing form of
(stable under the adjoint action of
and isomorphic to the irreducible seven-dimensional fundamental representation of
[
3,
20]), induces the short exact sequence of vector bundles over
X established in (
3).
Taking the long exact sequence in cohomology induced by the short exact sequence (
3) and using that
(established in the proof of Proposition 2), we obtain
where the sequence terminates at zero because
for every locally free sheaf
on a compact Riemann surface
X, which has complex dimension 1 and hence cohomological dimension 1 according to Serre duality.
Since the differential
is injective according to Theorem 1, the fiber of the normal bundle at
is
To compute the rank of the normal bundle, we apply the Riemann–Roch theorem. The vector bundle has rank seven and degree zero. The degree is zero because both adjoint bundles and have trivial determinants (being adjoint bundles of topologically trivial principal bundles for semisimple groups, according to Lemma 1), and therefore from the exact sequence we deduce that .
According to Riemann–Roch, for a rank seven bundle of degree zero over a curve of genus
g:
Since
, we obtain
Therefore, the normal bundle has rank . □
Remark 2. The rank established in Theorem 2 is consistent with the global dimension count: the closed embedding maps a variety of dimension into a variety of dimension , so the expected codimension isThe normal bundle computation thus provides an independent, infinitesimal confirmation of this codimension, showing that the cokernel of the differential has constant dimension at every smooth point, which implies that the embedding is regular (in the sense that the codimension equals the rank of the normal bundle everywhere on the stable locus). Corollary 1. Let X be a compact Riemann surface of genus . The image of the map forms a subvariety of of codimension .
Proof. The dimension of is , since . The dimension of is , since . Since is a closed embedding according to Theorem 1, the codimension of the image is , which equals the rank of the normal bundle computed in Theorem 2. □
Remark 3. The computation of the codimension can also be verified using infinitesimal deformation theory. The tangent space to at a point coming from a -bundle is , while the tangent space to at is . The exact sequenceinduces a long exact sequence in cohomology. Applying the Riemann–Roch theorem shows that and , confirming that the codimension equals . Remark 4. The smooth locus of is dense. A stable -bundle E gives a smooth point of the moduli space if and only if , which is equivalent to E having no non-trivial automorphisms.
For generic stable bundles over curves of genus , we have since the adjoint representation of is irreducible. The locus wherehas a codimension of at least one according to the semicontinuity of cohomology dimensions. Therefore, all results of this section apply to a dense open subset of the moduli space .
5. Deformation Theory and Tangent Spaces
The closed embedding established in Theorem 1 allows us to analyze the tangent spaces and deformation theory of octonionic bundles by exploiting the known structure of the moduli space .
Proposition 4. Let X be a compact Riemann surface of genus , and let be a point corresponding to a stable octonionic bundle E over X. Then
- 1.
The tangent space is canonically isomorphic to , where is the adjoint bundle.
- 2.
We have .
- 3.
The differential of the embeddingis injective, and the image is a -dimensional subspace of the -dimensional space .
Proof. First, we establish Part (1). According to Ramanathan’s deformation theory for moduli spaces of principal bundles [
5], the tangent space to the moduli space
at a point
corresponding to a stable principal
G-bundle
P is canonically isomorphic to
, where
is the adjoint bundle.
Since
and
E is a stable
-bundle, we have
where
.
To compute the dimension stated in Part (2), we apply the Riemann–Roch theorem. Since has dimension 14, the vector bundle has rank 14. According to Lemma 1, all octonionic bundles over X are topologically trivial, which implies that has degree zero (the degree of an associated bundle depends only on the topology of the principal bundle and the representation, and the adjoint representation of a semisimple group has a trivial determinant).
The Riemann–Roch theorem gives
For a stable principal
-bundle
E over a curve of genus
, we have
. To see this, note that
is the Lie algebra of infinitesimal automorphisms of
E. For a stable bundle, the automorphism group is finite [
5], so its Lie algebra is zero-dimensional, giving
.
For the embedding assertion, consider the map
defined by
. According to Theorem 1, this is a closed embedding, so the differential
is injective at every point
.
The tangent space at
is canonically isomorphic to
where
.
Now, there is a natural isomorphism
of vector bundles over
X. This follows from the fact that
, so
where the last isomorphism uses the natural
-equivariant identification
.
The embedding of Lie algebras
induces an inclusion of vector bundles
This inclusion is
-equivariant: for any
and
, we have
where
denotes the adjoint action of
restricted to
, and
denotes the adjoint action of
.
Considering cohomology, we obtain an injective linear map
According to the functoriality of Ramanathan’s construction of tangent spaces, this cohomological map is precisely the differential .
According to the same Riemann–Roch computation as in part (2), the vector bundle
has rank 21 and degree zero, and therefore
Therefore, embeds as a -dimensional subspace of the -dimensional space . □
Corollary 2. At any smooth point of corresponding to a stable bundle, the codimension of the image of in equals the difference in tangent space dimensions, which is .
Proof. From Proposition 4, at a smooth point
where
E is stable, we have
Since
is a closed embedding according to Theorem 1, at smooth points the codimension equals the difference in tangent space dimensions:
This confirms the global codimension computed in Corollary 1. □
Remark 5. The results of this section apply to the open dense subset of consisting of stable bundles. For stable bundles, the automorphism group is finite [5], the moduli space is smooth at the corresponding point, and the tangent space identification is classical. For strictly semistable bundles, the moduli space may have singularities, and the Zariski tangent space may be larger than . However, according to Theorem 1, the differential of ι remains injective even at these singular points, as proved in Section 3. Remark 6. The tangent space computation provides a cohomological interpretation of infinitesimal deformations. A class corresponds to an infinitesimal deformation of the -bundle structure on E, while its image corresponds to the induced infinitesimal deformation of the associated -bundle.
The fact that this map is injective reflects that the -structure is more rigid than the underlying -structure, in the sense that every infinitesimal deformation of a -bundle induces a unique infinitesimal deformation of the associated -bundle, but not every infinitesimal deformation of an -bundle preserves the -structure.
6. Consequences of the Embedding
The closed embedding
established in Theorem 1 has geometric consequences for the position of the moduli space of octonionic bundles within the ambient space and for the characteristic classes of its tangent bundle. For any reductive group
H, we write
for the open dense subvariety parametrizing stable bundles, and
as shorthand for
when the target group is clear from context. Throughout this section we denote by
and
the open dense subsets parametrizing stable bundles, on which both moduli spaces are smooth [
5,
6].
Proposition 5. Let X be a compact Riemann surface of genus . The image is a closed irreducible subvariety of of codimension . Moreover, the image intersects the smooth locus in a dense open subset of the image, and in particular is not contained in the singular locus of .
Proof. Since
is a closed embedding according to Theorem 1, the image is a closed subvariety of
isomorphic to
as an algebraic variety. According to Ramanathan’s construction of the moduli space [
5,
6], the moduli space
is irreducible; since
and the image is isomorphic to it as an algebraic variety, the image is irreducible. The codimension statement follows from Corollary 1.
For the second assertion, we show that the image of
under
is contained in
. Let
E be a stable
-bundle. Since
acts irreducibly on
[
20], the group
is not contained in any proper parabolic subgroup of
. Therefore, as shown in
Section 3, every reduction in structure of
to a proper parabolic
induces a reduction in
E to a proper parabolic of
. Since
E is stable, this induced reduction has strictly negative associated degree, and therefore the associated degree of the original reduction in
to
Q is also strictly negative, since according to the character analysis of
Section 3 that degree is a positive integer multiple of the degree of the induced reduction in
E. According to Ramanathan’s criterion [
5],
is therefore stable.
Therefore . Since is dense in the ambient space and is an isomorphism onto its image as algebraic varieties, the image of is a dense open subset of the image of , contained in the smooth locus of . In particular the image is not contained in the singular locus. □
Proposition 6. Let X be a compact Riemann surface of genus . Denote by T the tangent bundle of , by the pullback of the tangent bundle of to , and by N the normal bundle of the embedding over the smooth locus. Then
- 1.
There is an exact sequence of holomorphic vector bundles over : - 2.
The total Chern classes satisfyin . In particular:
Proof. (1) Since is a closed embedding and and are both smooth, the differential of the embedding at each point gives an injective linear map . The cokernel of this map is by definition the fiber of the normal bundle . Since the differential of is a morphism of holomorphic vector bundles over , and the cokernel has constant rank at every point according to Theorem 2, the cokernel is itself a holomorphic vector bundle, and the exact sequence of holomorphic vector bundles over follows.
(2) The relation
is the Whitney sum formula for the exact sequence of part (1), which holds for any short exact sequence of complex vector bundles [
25]. Expanding the product
and equating graded components in
and
respectively yields the stated formulas for
and
. □
Remark 7. The Whitney formula provides a constraint that any future computation of the characteristic classes of or of the normal bundle must satisfy. In particular, the first Chern class of the normal bundle is completely determined by those of T and :in . Sinceis the pullback to of the anticanonical class of the ambient space, the formula expresses —the anticanonical class of —as the difference between this pullback and . 7. Conclusions and Open Questions
In this paper, we have established that the natural Lie group inclusion
induces a closed embedding
of the moduli space of octonionic bundles as a closed irreducible subvariety of codimension
in the moduli space of
-bundles over a compact Riemann surface
X of genus
. The significance of this result is threefold: it provides a concrete algebro-geometric realization of the exceptional symmetry encoded according to
within the classical orthogonal moduli theory; it yields an explicit cohomological description of the normal bundle and the tangent spaces; and it produces structural constraints on the Chern classes of
via the Whitney formula
. The proofs combine Ramanathan’s stability theory, the theorem of Ramanan–Ramanathan on associated bundles, Luna’s étale slice theorem, and the valuative criterion via Balaji–Seshadri and Drinfeld–Simpson.
Several natural directions for further investigation remain. Although the Whitney formula establishes relations among and of the tangent bundle, the pullback of the ambient tangent bundle, and the normal bundle, a complete determination of the individual Chern classes requires a more refined understanding of the global geometry. In particular, the global structure of the normal bundle is not yet fully understood, including the existence of a canonical splitting as a direct sum of simpler bundles, the determination of its degree as a vector bundle over , and its possible semistability or polystability. Addressing these structural properties requires further analysis of the variation of the cohomology groups as E ranges over the moduli space.
Second, further study of the infinitesimal neighborhoods of within using formal deformation theory would be interesting, as it could provide insights into the structure of the formal completion of the ambient space along the subvariety, the obstruction groups controlling higher-order deformations, and the relationship between deformations that preserve the -structure and those that only preserve the -structure.
It would also be illuminating to compare the results of the present paper with similar embeddings for other exceptional groups, such as (which is covered by the preceding literature), to understand whether the phenomena we observe are specific to or represent general features.
From the perspective of mathematical physics, the moduli space of -bundles appears naturally in string theory and M-theory, particularly in compactifications on seven-dimensional manifolds with holonomy. Understanding the embedding into -bundles may help analyze the effective physics of these compactifications and could have implications for understanding moduli stabilization and the landscape of string vacua.
Finally, several open problems remain to be addressed. These include the concrete computation of the cohomology groups in specific examples, the determination of explicit equations defining as a subvariety of , and the construction of explicit examples that realize the embedding in cases of low genus.