Abstract
The aim here is to describe all isomorphism classes of -equivariant Hermitian holomorphic vector bundles on the complex projective space . If is the isotropy subgroup of a chosen point , and is a unitary representation, we obtain -equivariant holomorphic Hermitian vector bundles on . Next, given any satisfying certain conditions, a new structure of an -equivariant holomorphic Hermitian vector bundle on this underlying holomorphic Hermitian bundle is obtained. It is shown that all -equivariant holomorphic Hermitian vector bundles on arise this way.
MSC:
53B35; 14F05
1. Introduction
Take any holomorphic vector bundle E of rank r defined over . Then, E holomorphically decomposes as
where each is a holomorphic line bundle on the complex projective line [1]. We know that each is isomorphic to for some . Therefore, the above theorem of Grothendieck describes all holomorphic vector bundles on .
Here, we consider a special class of holomorphic vector bundles on the complex projective space of dimension n. To explain this class, first note that acts transitively on via holomorphic automorphisms. We consider holomorphic Hermitian vector bundles on that are equivariant for the action of . More precisely, we take a holomorphic vector bundle E on the complex projective space and assume that E is equipped with a Hermitian structure h; furthermore, let
be a action of on E such that the following conditions hold:
- for any , the map is a holomorphic automorphism of E over the automorphism of given by the action of g;
- the above map preserves the Hermitian structure h.
Holomorphic Hermitian vector bundles E on equipped with such an action of are called -equivariant holomorphic Hermitian vector bundles.
Our aim here is to describe all the isomorphism classes of -equivariant Hermitian holomorphic vector bundles defined over .
Let us take two -equivariant holomorphic Hermitian vector bundles on , say and . An isomorphism between and is a holomorphic isomorphism of vector bundles
such that
- for all and all ,
- for all and .
We describe the space of all isomorphism classes of -equivariant holomorphic Hermitian vector bundles on .
To explain the isomorphism classes of -equivariant holomorphic Hermitian vector bundles on , we fix a point . Let be the isotropy subgroup of the point for the action of on . We note that G is isomorphic to the intersection of the subgroup with the subgroup . Let
be the center of G. We note that is identified with .
Consider all pairs of the form , where
is a finite dimensional complex representation of the group and
is an invariant for the action of on given by the actions of on and . For any such pair ,
Let denote the space of all pairs of the above type such that .
Two elements and of will be called equivalent if there is a –linear isomorphism
such that the following two conditions hold:
- for all (note that both and are homomorphisms from to ),
- (note that both sides are homomorphisms from to ).
Let
denote the equivalence classes of elements of .
The following theorem is proved here (see Theorem 2):
Theorem 1.
There is a canonical bijection between (see (38)) and the space of all isomorphisms classes of -equivariant holomorphic Hermitian vector bundle on .
The very special case of was addressed earlier in [2]. Note that that condition in (37) is automatically satisfied when , because .
See [3,4,5,6,7,8,9,10,11] for results on related topics.
2. Properties of Equivariant Vector Bundles on Projective Space
Consider the complex projective space of dimension n that parametrizes all one-dimensional complex linear subspaces of . There is a natural projection that sends any nonzero vector of to the line in generated by it. Consider the standard action of the special unitary group on the complex vector space . This action evidently induces an action of on . Let
be the morphism that defines the above action of on . Clearly, for every , the image is a holomorphic automorphism of the projective space .
Take a holomorphic vector bundle E on the projective space ; assume that E is equipped with a Hermitian structure h.
In the special case where , Definitions 1 and 2 coincide with [2] (p. 248, Definition 2.1) and [2] (p. 248, Definition 2.2), respectively.
Definition 1.
The holomorphic Hermitian vector bundle on is called -homogeneous if for each , the pulled-back holomorphic Hermitian vector bundle is holomorphically isometric to , where f is the homomorphism in (1).
Two -homogeneous vector bundles and are called isomorphic if there is a holomorphic isomorphism that takes h to .
Definition 2.
An -equivariant holomorphic Hermitian vector bundle on is a triple , where
- is a holomorphic vector bundle on ,
- h is a Hermitian structure on E,
- ρ is an action of on the total space of Esatisfying the following two conditions:
- 1.
- for all , where f is the homomorphism in (1) and p is the above projection of E to ,
- 2.
- for each , the action of U on E is a holomorphic isometry of the pulled-back holomorphic Hermitian vector bundle with .
Two -equivariant holomorphic Hermitian vector bundles and are called isomorphic if there is a holomorphic isometry that intertwines the two actions ρ and of .
An -equivariant holomorphic Hermitian vector bundle on is evidently -homogeneous. The following lemma shows that the converse holds.
In the special case where , Lemma 1 reduces to [2] (p. 248, Lemma 2.3).
Lemma 1.
Let be a -homogeneous holomorphic Hermitian vector bundle on . Then, E admits an action ρ of such that the triple is an -equivariant holomorphic Hermitian vector bundle.
Proof.
For any , let denote the space of all holomorphic isometries of the holomorphic Hermitian vector bundle with , where f is the homomorphism in (1). The union
has a natural structure of a finite dimensional Lie group. The group operation is defined as follows: for and ,
is simply the composition of maps. Since is -homogeneous, the homomorphism from the group in (3)
that sends any to U, is surjective. Therefore, we have a short exact sequence of groups
where is constructed in (4), and is the group of all holomorphic isometries of the holomorphic Hermitian vector bundle .
The Lie algebra of (respectively, ) will be denoted by (respectively, ). Let
be the short exact sequence of Lie algebras associated to (5), where is the homomorphism of Lie algebras associated to the homomorphism in (4).
The Lie algebra of is simple. Hence, the homomorphism in (6) splits (see [12] (p. 91, Corollaire 3)). In other words, there is Lie algebra homomorphism
such that . Fix a splitting as in (7).
Since the Lie group is simply connected, there is a unique homomorphism of Lie groups
whose differential, at the identity element, is the homomorphism in (7). This homomorphism defines an action of
on the total space of E. More precisely, the action of any on E defined by coincides with .
Take any point . Let
be the orthogonal complement of the line z in . The group of linear automorphisms of preserving the Hermitian structure on it induced by the Hermitian structure on , will be denoted by . The group of linear automorphisms of the line z in preserving the Hermitian structure on it induced by the Hermitian structure on , will be denoted by . We note that is canonically identified with
The element in corresponding to any is uniquely determined by the condition that it acts as multiplication by on the line in represented by z. Note that is a subgroup of . Let
be the isotropy subgroup of z for the action of on . We note that is canonically identified with the subgroup
where ; note that both and are subgroups of .
Take any -equivariant holomorphic Hermitian vector bundle on . For any two points , the action of on the fiber given by can be shown to be a conjugate of the action of on . To see this, take any such that , where f is the homomorphism in (1); there is such an element A because the action of on is transitive. Then, we have . Let
be the isomorphism. Now, the isomorphism
given by the action of A on E has the following property:
for all and .
Let
be the center of the group . We note that is identified with . To see this, for any with , consider the automorphism of
so acts on the line in defined by z as multiplication by , and acts on the orthogonal complement of this line as multiplication by . It is easy to see that , where is defined in (11). Now, we have an isomorphism
that sends any to constructed above from .
In the special case where , Proposition 1 reduces to [2] (p. 250, Proposition 2.4).
Proposition 1.
Let and be two -equivariant holomorphic Hermitian vector bundles on . Fix a point . Assume that for the action of the center (see (11) and (12)) on , every acts as multiplication by for some fixed d. Let
be an isomorphism such that the following two conditions hold:
- 1.
- for all (in other words, B takes the Hermitian structure to ),
- 2.
- for all and .
Then, the -equivariant holomorphic Hermitian vector bundle is isomorphic to .
Proof.
For every , let
be the linear isometry obtained from the isometry B in (13) using the actions of U on E and , where f is the homomorphism in (1). More precisely,
for all . From the second condition in the statement of the proposition, it follows immediately that we have if .
Therefore, all the isometries patch together to give a isomorphism
between the vector bundles which intertwines the actions of on E and . In particular, the section is left invariant by the action of on the vector bundle induced by the actions of on E and .
From the construction of , it follows immediately that takes the Hermitian structure h on E to on .
The holomorphic structures on E and together define a holomorphic structure on the vector bundle . Let
be the Dolbeault operator for the holomorphic structure on the vector bundle . So we have
where is the section in (14).
Consider the action of on the vector bundle induced by the actions of on E and . Since is left invariant by the action of on , we conclude that the -form with values in (see (15)) is also left invariant by the action of on the vector bundle
on ; note that the action of on produces an action of on , and this action of on combines together with the action of on to produce an action of on .
Recall that for the action of the center (see (11) and (12)) on , every acts as multiplication by for some fixed d. Therefore, from the second condition in the proposition, it follows immediately that for the action of the center on , every acts as multiplication by . Consequently, the group acts trivially on the fiber .
On the other hand, the group acts on the fiber as follows: any acts as multiplication with . Since the section in (15) is left invariant by the action of , in particular, it is left invariant by the action of , we now conclude that the section vanishes at . The section being -invariant, it follows that vanishes identically; recall that the action of on is transitive. Consequently, the isomorphism is actually holomorphic.
We already noted that takes the Hermitian metric h to , and it also intertwines the actions of on E and . Therefore, is an isomorphism between the two -equivariant holomorphic Hermitian vector bundles and . This completes the proof of the proposition. □
3. An Equivariant Principal Bundle
Fix a point . Let
be the corresponding isotropy subgroup (see (9)). Since the action of on is transitive, the quotient , where G is the subgroup in (16), is identified with . This identification is constructed by sending any to , where f is the homomorphism in (1). Consider the quotient map
It gives a principal G-bundle on . We will show that this principal G-bundle
on has a tautological connection.
To construct the tautological connection on the principal G-bundle in (18), consider the Lie algebra of ; the Killing form on it will be denoted by . We note that is a positive definite inner product on . Let
be the Lie subalgebra of the Lie subgroup G in (16). We have the orthogonal complement
of for the inner product on . Let
be the orthogonal projection for the inner product on . So (see (19)). Using the left-translation action of on itself, the real tangent bundle is identified with the trivial vector bundle with fiber . Using this identification, the homomorphism produces a -valued 1-form on ; this 1-form is evidently preserved by the left-translation action of on itself. Let
be this -invariant -valued 1-form on given by . Next, note that the restriction of to any fiber of the projection q in (17) coincides with the Maurer–Cartan form on the fiber of the principal G-bundle on in (18). Moreover, is G-equivariant for the right action of G on when we equip with the adjoint action of G. Consequently, defines a connection on the principal G-bundle on ; see [13]. Let
be this connection on principal G-bundle given by . We note that the left-translation action of on itself preserves the connection in (21) because the 1-form is -invariant.
The adjoint vector bundle for the principal G-bundle in (18) will be denoted by . Let
be the curvature of the connection in (21). Since the left-translation action of on itself preserves the connection , we conclude that the section in (22) is -invariant. Let
be the Hodge type decomposition of the -valued 2-form in (22).
Proposition 2.
Proof.
Since in (22) is -invariant, and the action of each element of on preserves the complex structure of , we conclude that , and in (23) are all -invariant.
The action of on induces an action of on the adjoint vector bundle .
Now, consider the center (see (11) and (16)). The action of on produces an action of the group on the fiber of over the point . It is easy to see that this action of on is the trivial one. On the other hand, as noted in the proof of Proposition 1, for the action of the group (see (12)) on the fiber , any acts as multiplication with . Therefore, any acts on as multiplication with . Hence, any acts on as multiplication with . This implies that no nonzero element of is fixed by the action of . Since in (23) is -invariant, and no nonzero element of is fixed by the action of , we conclude that
For the action of the group on the fiber , any acts as multiplication with . Therefore, repeating the above argument, we conclude that no nonzero element of is fixed by the action of . Hence, we have
as well. This completes the proof. □
4. Equivariant Vector Bundle for a Representation
Consider the subgroup in (16). Let V be a finite dimensional complex vector space and
a homomorphism. Let
be the vector bundle associated to the principal G-bundle (see (18)) for the G-module V in (24). We recall that is a quotient where two elements and of are identified if there is an element such that and . The action of on produces an action of on . More precisely, consider the following action of on : the action of any sends any to . This action of on produces an action of on the quotient space .
Since the group G is compact, there is a positive definite Hermitian structure on V such that the image of the homomorphism in (24) is contained in the subgroup of consisting of all automorphisms of V that preserve the Hermitian structure . Now, it can be seen that produces a Hermitian structure on the vector bundle in (25). Indeed, the Hermitian structure on V produces a Hermitian structure on the trivial vector bundle with fiber V. Since the action of G on V given by preserves , this Hermitian structure on the trivial vector bundle descends to a Hermitian structure on the vector bundle over . The Hermitian structure on obtained this way will be denoted by h.
The above action of on clearly preserves the Hermitian structure h on .
Next, consider the connection on the principal G-bundle constructed in (21). It induces a connection on any vector bundle associated to . In particular, induces a connection on the vector bundle in (25). This induced connection on will be denoted by . We note that the action of on preserves the connection because the action of on preserves the connection .
The connection on clearly preserves the Hermitian structure h on .
Let be the curvature of the connection . Since the curvature is given by the curvature of , from Proposition 2, we conclude that is of Hodge type . From this, it follows that the -component of the connection produces a holomorphic structure on the vector bundle (see [14] (p. 9, Prop. 3.5) and [14] (p. 9, Prop. 3.7)).
The action of elements on on preserves the above holomorphic structure on because the action of on preserves the connection .
Consequently, is an -equivariant holomorphic Hermitian vector bundle on .
The following lemma summarizes the above construction.
Lemma 2.
Given a finite dimensional complex vector space V and a homomorphism
there is a naturally associated -equivariant holomorphic Hermitian vector bundle on .
5. Representation for an Equivariant Vector Bundle
Let be an -equivariant holomorphic Hermitian vector bundle on . As in Section 3, fix a point . V denotes the fiber of over the point . Consider the action of the subgroup (see (16)) on . Let
be the homomorphism given by the action of G on V.
Lemma 2 associates an -equivariant holomorphic Hermitian vector bundle to in (26).
Lemma 3.
There is a canonical isomorphism
such that
- 1.
- ϕ is -equivariant,
- 2.
- ϕ takes the Hermitian structure h on to the Hermitian structure on .
Proof.
Consider the quotient map q in (17). The pulled-back vector bundle is canonically identified with the trivial vector bundle
this follows immediately from the construction of from . We will construct an isomorphism
of vector bundles over . Take any
The map sends to , where is the map giving the action of on . Recall from Section 4 that is a quotient of . It is easy to see that the isomorphism in (27) descends to an isomorphism
of vector bundles over .
From the construction of , it follows immediately that is -equivariant.
Since the action of on preserves the Hermitian structure on , it follows that takes the Hermitian structure h on to the Hermitian structure on . □
From Lemma 2, we know that is an -equivariant holomorphic Hermitian vector bundle. It should be clarified that the isomorphism in Lemma 3 need not be holomorphic.
The Dolbeault operators on the holomorphic vector bundles and will be denoted by and , respectively (see [14] (p. 10, Prop. 3.9)). We have
Since and define holomorphic structures, it follows that
[14] (p. 9, Prop. 3.5).
Proposition 3.
Proof.
Consider the center
of G (see (16), (11) and (12)). The action of on produces an action of on the fiber . Let
be the isotypical decomposition of the -module V. For each , let
be the unique integer satisfying the following condition: The action of any on sends any to .
Since is the center of G, the action of G on V, given by the action of on , preserves the decomposition in (30). In other words, the action of G on V preserves each in (30).
Note that Lemma 2 associates to each G-module an -equivariant holomorphic Hermitian vector bundle on . For each , let be the -equivariant holomorphic Hermitian vector bundle on for . From (30), we have
We have the maps
where is the inclusion map and is the projection map constructed using the decomposition in (32).
Consider the section in the proposition. For every , let
be the homomorphism given by the following composition of homomorphisms
where and are the homomorphisms in (33). Then, we have
Note that each section is preserved by the action of because
- is preserved by the action of ,
- the homomorphisms and in (33) are also preserved by the action of .
Recall that for the action of the group on the fiber , any acts as multiplication with . Therefore, if , then we have
(see (31)).
From (34), it follows that
Note that
and is preserved by the action of because is preserved by the action of . Since for the action of the group on the fiber , any acts as multiplication with , it follows that if ; then, we have
Comparing this with (35) we conclude that if . Now, the proposition follows from (36). □
Corollary 1.
The term in (29) vanishes identically.
Proof.
The section in (28) is preserved by the action of because the two Dolbeault operators and are both preserved by the action of . Hence, from Proposition 3, it follows that . □
6. Equivariant Holomorphic Hermitian Vector Bundles
As before, .
Consider all pairs of the form , where
is a finite dimensional complex representation of the group G and
where is the center of G. For any such pair , note that we have
Let denote the space of all pairs of the above type such that
Two elements and of will be called equivalent if there is an isomorphism
such that the following two conditions hold:
- for all (note that both and are homomorphisms from to ),
- (note that both sides are homomorphisms from to ).
Let
denote the equivalence classes of elements of .
Theorem 2.
There is a canonical bijection between (see (38)) and the space of all isomorphisms classes of -equivariant holomorphic Hermitian vector bundle on .
Proof.
As in Section 5, take any -equivariant holomorphic Hermitian vector bundle on .
Consider in (26) and
constructed in (28). From (29) and Corollary 1, it follows immediately that
Hence, we have .
We send to the element of given by the pair . This produces a map to from the space of all isomorphism classes of -equivariant holomorphic Hermitian vector bundles on .
For the inverse map, take any . Using Lemma 2, the homomorphism produces an -equivariant holomorphic Hermitian vector bundle on . Since v is fixed by the action of on , using the actions of on and , the element v produces a -invariant section
The given condition in (37) that implies that
because is preserved by the action of and the action of is transitive.
Let be the Dolbeault operator for the holomorphic vector bundle . Consider the Dolbeault operator on the vector bundle . From (39) and Proposition 3, we conclude that
Therefore, defines a holomorphic structure on the vector bundle .
The Hermitian structure h on remains unchanged. This new holomorphic Hermitian vector bundle is evidently -equivariant. This produces the inverse map from to the space of all isomorphisms classes of the -equivariant holomorphic Hermitian vector bundle on . □
Author Contributions
Conceptualization, I.B. and F.-X.M. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Data Availability Statement
No new data were created or analyzed in this study.
Conflicts of Interest
The authors declare no conflicts of interest.
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