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Article

Equivariant Holomorphic Hermitian Vector Bundles over a Projective Space

by
Indranil Biswas
1,* and
Francois-Xavier Machu
2
1
Department of Mathematics, Shiv Nadar University, NH91, Tehsil Dadri, Greater Noida 201314, Uttar Pradesh, India
2
Ecole Supérieure d’Informatique Électronique Automatique (ESIEA), 74 bis Av. Maurice Thorez, 94200 Ivry-sur-Seine, France
*
Author to whom correspondence should be addressed.
Mathematics 2024, 12(23), 3757; https://doi.org/10.3390/math12233757
Submission received: 9 October 2024 / Revised: 11 November 2024 / Accepted: 27 November 2024 / Published: 28 November 2024
(This article belongs to the Special Issue Advanced Algebraic Geometry and Applications)

Abstract

:
The aim here is to describe all isomorphism classes of SU ( n + 1 ) -equivariant Hermitian holomorphic vector bundles on the complex projective space C P n . If G SU ( n + 1 ) is the isotropy subgroup of a chosen point x 0 C P n , and ρ : G GL ( V ) is a unitary representation, we obtain SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles on C P n . Next, given any v End ( V ρ ) ( T z 0 0 , 1 C P n ) satisfying certain conditions, a new structure of an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on this underlying C holomorphic Hermitian bundle is obtained. It is shown that all SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles on C P n arise this way.

1. Introduction

Take any holomorphic vector bundle E of rank r defined over C P 1 . Then, E holomorphically decomposes as
E = i = 1 r L i ,
where each L i is a holomorphic line bundle on the complex projective line C P 1 [1]. We know that each L i is isomorphic to O C P 1 ( d i ) for some d i Z . Therefore, the above theorem of Grothendieck describes all holomorphic vector bundles on C P 1 .
Here, we consider a special class of holomorphic vector bundles on the complex projective space C P n of dimension n. To explain this class, first note that SU ( n + 1 ) acts transitively on C P n via holomorphic automorphisms. We consider holomorphic Hermitian vector bundles on C P n that are equivariant for the action of SU ( n + 1 ) . More precisely, we take a holomorphic vector bundle E on the complex projective space C P n and assume that E is equipped with a Hermitian structure h; furthermore, let
ρ : SU ( n + 1 ) × E E
be a C action of SU ( n + 1 ) on E such that the following conditions hold:
  • for any g SU ( n + 1 ) , the map v ρ ( g , v ) is a holomorphic automorphism of E over the automorphism of C P n given by the action of g;
  • the above map v ρ ( g , v ) preserves the Hermitian structure h.
Holomorphic Hermitian vector bundles E on C P n equipped with such an action of SU ( n + 1 ) are called SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles.
Our aim here is to describe all the isomorphism classes of SU ( n + 1 ) -equivariant Hermitian holomorphic vector bundles defined over C P n .
Let us take two SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles on C P n , say ( E , h , ρ ) and ( E , h , ρ ) . An isomorphism between ( E , h , ρ ) and ( E , h , ρ ) is a holomorphic isomorphism of vector bundles
Φ : E E
such that
  • h ( v , w ) = h ( Φ ( v ) , Φ ( w ) ) for all v , w E x and all x C P n ,
  • Φ ( ρ ( g , v ) ) = ρ ( g , Φ ( v ) ) for all g SU ( n + 1 ) and v E .
We describe the space of all isomorphism classes of SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles on C P n .
To explain the isomorphism classes of SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles on C P n , we fix a point z 0 C P n . Let G SU ( n + 1 ) be the isotropy subgroup of the point z 0 for the action of SU ( n + 1 ) on C P n . We note that G is isomorphic to the intersection of the subgroup U ( 1 ) × U ( n ) U ( n + 1 ) with the subgroup SU ( n + 1 ) U ( n + 1 ) . Let
Z G G
be the center of G. We note that Z G is identified with U ( 1 ) .
Consider all pairs of the form ( ρ , v ) , where
ρ : G GL ( V ρ )
is a finite dimensional complex representation of the group G SU ( n + 1 ) and
v ( End ( V ρ ) ( T z 0 0 , 1 C P n ) ) Z G End ( V ρ ) ( T z 0 0 , 1 C P n )
is an invariant for the action of Z G on End ( V ρ ) ( T z 0 0 , 1 C P n ) given by the actions of Z G on V ρ and T z 0 0 , 1 C P n . For any such pair ( ρ , v ) ,
[ v , v ] End ( V ρ ) ( T z 0 0 , 2 C P n ) .
Let S denote the space of all pairs ( ρ , v ) of the above type such that [ v , v ] = 0 .
Two elements ( ρ , v ) and ( ρ , v ) of S will be called equivalent if there is a C –linear isomorphism
ψ : V ρ V ρ
such that the following two conditions hold:
  • ψ ρ ( g ) = ρ ( g ) ψ for all g G (note that both ψ ρ ( g ) and ρ ( g ) ψ are homomorphisms from V ρ to V ρ ),
  • v ψ = ( ψ Id ( T z 0 0 , 1 C P n ) ) v (note that both sides are homomorphisms from V ρ to V ρ ( T z 0 0 , 1 C P n ) ).
Let
S
denote the equivalence classes of elements of S .
The following theorem is proved here (see Theorem 2):
Theorem 1.
There is a canonical bijection between S (see (38)) and the space of all isomorphisms classes of SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n .
The very special case of n = 0 was addressed earlier in [2]. Note that that condition in (37) is automatically satisfied when n = 1 , because T 0 , 2 C P 1 = 0 .
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 C P n of dimension n that parametrizes all one-dimensional complex linear subspaces of C n + 1 . There is a natural projection C n + 1 { 0 } C P n that sends any nonzero vector of 0 v C n + 1 to the line C · v in C n + 1 generated by it. Consider the standard action of the special unitary group SU ( n + 1 ) on the complex vector space C n + 1 . This action evidently induces an action of SU ( n + 1 ) on C P n . Let
f : SU ( n + 1 ) Aut ( C P n )
be the morphism that defines the above action of SU ( n + 1 ) on C P n . Clearly, for every U SU ( n + 1 ) , the image f ( U ) is a holomorphic automorphism of the projective space C P n .
Take a holomorphic vector bundle E on the projective space C P n ; assume that E is equipped with a Hermitian structure h.
In the special case where n = 1 , 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 ( E , h ) on C P n is called SU ( n + 1 ) -homogeneous if for each U SU ( n + 1 ) , the pulled-back holomorphic Hermitian vector bundle ( f ( U ) E , f ( U ) h ) is holomorphically isometric to ( E , h ) , where f is the homomorphism in (1).
Two SU ( n + 1 ) -homogeneous vector bundles ( E , h ) and ( E , h ) are called isomorphic if there is a holomorphic isomorphism E E that takes h to h .
Definition 2.
An SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n is a triple ( E , h , ρ ) , where
  • E p C P n is a holomorphic vector bundle on C P n ,
  • h is a Hermitian structure on E,
  • ρ is an action of SU ( n + 1 ) on the total space of E
    ρ : SU ( n + 1 ) × E E
    satisfying the following two conditions:
    1. 
    p ρ ( ( U , v ) ) = f ( U ) ( p ( v ) ) for all ( U , v ) SU ( n + 1 ) × E , where f is the homomorphism in (1) and p is the above projection of E to C P n ,
    2. 
    for each U SU ( n + 1 ) , the action of U on E is a holomorphic isometry of the pulled-back holomorphic Hermitian vector bundle ( f ( U 1 ) E , f ( U 1 ) h ) with ( E , h ) .
Two SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles ( E , h , ρ ) and ( E , h , ρ ) are called isomorphic if there is a holomorphic isometry E E that intertwines the two actions ρ and ρ of SU ( n + 1 ) .
An SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n is evidently SU ( n + 1 ) -homogeneous. The following lemma shows that the converse holds.
In the special case where n = 1 , Lemma 1 reduces to [2] (p. 248, Lemma 2.3).
Lemma 1.
Let ( E , h ) be a SU ( n + 1 ) -homogeneous holomorphic Hermitian vector bundle on C P n . Then, E admits an action ρ of SU ( n + 1 ) such that the triple ( E , h , ρ ) is an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle.
Proof. 
For any U SU ( n + 1 ) , let T ( U ) denote the space of all holomorphic isometries of the holomorphic Hermitian vector bundle ( f ( U 1 ) E , f ( U 1 ) h ) with ( E , h ) , where f is the homomorphism in (1). The union
U E : = U SU ( n + 1 ) T ( U )
has a natural structure of a finite dimensional Lie group. The group operation is defined as follows: for A T ( U ) and A T ( U ) ,
A A = A A T ( U U )
is simply the composition of maps. Since ( E , h ) is SU ( n + 1 ) -homogeneous, the homomorphism from the group U E in (3)
γ : U E SU ( n + 1 ) ,
that sends any A T ( U ) to U, is surjective. Therefore, we have a short exact sequence of groups
e Aut ( ( E , h ) ) U E γ SU ( n + 1 ) e ,
where γ is constructed in (4), and Aut ( ( E , h ) ) is the group of all holomorphic isometries of the holomorphic Hermitian vector bundle ( E , h ) .
The Lie algebra of U E (respectively, Aut ( ( E , h ) ) ) will be denoted by g (respectively, g 0 ). Let
0 g 0 g γ s u ( n + 1 ) e
be the short exact sequence of Lie algebras associated to (5), where γ is the homomorphism of Lie algebras associated to the homomorphism γ in (4).
The Lie algebra s u ( n + 1 ) of SU ( n + 1 ) is simple. Hence, the homomorphism γ in (6) splits (see [12] (p. 91, Corollaire 3)). In other words, there is Lie algebra homomorphism
γ : s u ( n + 1 ) g
such that γ γ = Id s u ( n + 1 ) . Fix a splitting γ as in (7).
Since the Lie group SU ( n + 1 ) is simply connected, there is a unique homomorphism of Lie groups
ρ : SU ( n + 1 ) U E
whose differential, at the identity element, is the homomorphism γ in (7). This homomorphism ρ defines an action of SU ( n + 1 )
ρ : SU ( n + 1 ) × E E
on the total space of E. More precisely, the action of any U SU ( n + 1 ) on E defined by ρ coincides with ρ ( U ) .
Now it is straightforward to verify that ( E , h , ρ ) is an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle, where ρ is constructed in (8) (see the conditions on ρ in (2)). This completes the proof of the lemma. □
Take any point z C P n . Let
z = : S z C n + 1
be the orthogonal complement of the line z in C n + 1 . The group of linear automorphisms of S z preserving the Hermitian structure on it induced by the Hermitian structure on C n + 1 , will be denoted by U ( S z ) . The group of linear automorphisms of the line z in C n + 1 preserving the Hermitian structure on it induced by the Hermitian structure on C n + 1 , will be denoted by U ( z ) . We note that U ( z ) is canonically identified with
U ( 1 ) = { λ C | | λ | = 1 }
The element in U ( z ) corresponding to any λ U ( 1 ) is uniquely determined by the condition that it acts as multiplication by λ on the line in C n + 1 represented by z. Note that U ( z ) × U ( S z ) is a subgroup of U ( n + 1 ) . Let
H z SU ( n + 1 )
be the isotropy subgroup of z for the action of SU ( n + 1 ) on C P n . We note that H z is canonically identified with the subgroup
S ( U ( z ) × U ( S z ) ) = S ( U ( 1 ) × U ( S z ) ) SU ( n + 1 ) ,
where S ( U ( z ) × U ( S z ) ) : = ( U ( z ) × U ( S z ) ) SU ( n + 1 ) U ( n + 1 ) ; note that both U ( z ) × U ( S z ) and SU ( n + 1 ) are subgroups of U ( n + 1 ) .
Take any SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle ( E , h , ρ ) on C P n . For any two points z , z C P n , the action of H z = S ( U ( z ) × U ( S z ) ) on the fiber E z given by ρ can be shown to be a conjugate of the action of H z = S ( U ( z ) × U ( S z ) ) on E z . To see this, take any A SU ( n + 1 ) such that f ( A ) ( z ) = z , where f is the homomorphism in (1); there is such an element A because the action of SU ( n + 1 ) on C P n is transitive. Then, we have H z = A H z A 1 . Let
A ^ : H z H z , g A g A 1
be the isomorphism. Now, the isomorphism
A z : E z E z
given by the action of A on E has the following property:
A z ( ρ ( g , v ) ) = ρ ( A ^ ( g ) , A z ( v ) )
for all v E z and g H z .
Let
Z ( H z ) H z
be the center of the group H z . We note that Z ( H z ) is identified with U ( 1 ) = { λ C | | λ | = 1 } . To see this, for any λ C with | λ | = 1 , consider the automorphism of C n + 1
g λ : = λ n · Id z λ 1 · Id z GL ( n + 1 , C ) ;
so g λ acts on the line in C n + 1 defined by z as multiplication by λ n , and g λ acts on the orthogonal complement of this line as multiplication by λ 1 . It is easy to see that g λ Z ( H z ) , where Z ( H z ) is defined in (11). Now, we have an isomorphism
U ( 1 ) Z ( H z )
that sends any λ U ( 1 ) to g λ Z ( H z ) constructed above from λ .
In the special case where n = 1 , Proposition 1 reduces to [2] (p. 250, Proposition 2.4).
Proposition 1.
Let ( E , h , ρ ) and ( E , h , ρ ) be two SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles on C P n . Fix a point z 0 C P n . Assume that for the action of the center Z ( H z 0 ) = U ( 1 ) (see (11) and (12)) on E z 0 , every λ U ( 1 ) acts as multiplication by λ d for some fixed d. Let
B : E z 0 E z 0
be an isomorphism such that the following two conditions hold:
1. 
h ( v , w ) = h ( B ( v ) , B ( w ) ) for all v , w E z 0 (in other words, B takes the Hermitian structure h z 0 to h z 0 ),
2. 
B ( ρ ( g , v ) ) = ρ ( g , B ( v ) ) for all g H z 0 and v E z 0 .
Then, the SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle ( E , h , ρ ) is isomorphic to ( E , h , ρ ) .
Proof. 
For every U SU ( n + 1 ) , let
B U : E f ( U ) ( z 0 ) E f ( U ) ( z 0 )
be the linear isometry obtained from the isometry B in (13) using the actions of U on E and E , where f is the homomorphism in (1). More precisely,
B U ( ρ ( U , v ) ) = ρ ( U , B ( v ) )
for all v E z 0 . From the second condition in the statement of the proposition, it follows immediately that we have B U = B U if f ( U ) = f ( U ) .
Therefore, all the isometries { B U } U SU ( n + 1 ) patch together to give a C isomorphism
B C ( C P n , E E )
between the C vector bundles which intertwines the actions of SU ( n + 1 ) on E and E . In particular, the section B is left invariant by the action of SU ( n + 1 ) on the vector bundle E E induced by the actions of SU ( n + 1 ) on E and E .
From the construction of B , it follows immediately that B takes the Hermitian structure h on E to h on E .
The holomorphic structures on E and E together define a holomorphic structure on the C vector bundle E E . Let
¯ E , E : C ( C P n , E E ) C ( C P n , Ω C P n 0 , 1 E E ) = C ( C P n , Ω C P n 0 , 1 ( E E ) )
be the Dolbeault operator for the holomorphic structure on the vector bundle E E . So we have
¯ E , E ( B ) C ( C P n , Ω C P n 0 , 1 ( E E ) ) ,
where B is the section in (14).
Consider the action of SU ( n + 1 ) on the vector bundle E E induced by the actions of SU ( n + 1 ) on E and E . Since B is left invariant by the action of SU ( n + 1 ) on E E , we conclude that the ( 0 , 1 ) -form ¯ E , E ( B ) with values in E E (see (15)) is also left invariant by the action of SU ( n + 1 ) on the C vector bundle
( T 0 , 1 C P n ) E E
on C P n ; note that the action of SU ( n + 1 ) on C P n produces an action of SU ( n + 1 ) on ( T 0 , 1 C P n ) , and this action of SU ( n + 1 ) on ( T 0 , 1 C P n ) combines together with the action of SU ( n + 1 ) on E E to produce an action of SU ( n + 1 ) on ( T 0 , 1 C P n ) E E .
Recall that for the action of the center Z ( H z 0 ) = U ( 1 ) (see (11) and (12)) on E z 0 , every λ U ( 1 ) acts as multiplication by λ d for some fixed d. Therefore, from the second condition in the proposition, it follows immediately that for the action of the center Z ( H z 0 ) = U ( 1 ) on E z 0 , every λ U ( 1 ) acts as multiplication by λ d . Consequently, the group Z ( H z 0 ) acts trivially on the fiber ( E E ) z 0 .
On the other hand, the group Z ( H z 0 ) = U ( 1 ) acts on the fiber ( T z 0 0 , 1 C P n ) as follows: any λ U ( 1 ) acts as multiplication with 1 / λ n + 1 . Since the section ¯ E , E ( B ) in (15) is left invariant by the action of SU ( n + 1 ) , in particular, it is left invariant by the action of Z ( H z 0 ) , we now conclude that the section ¯ E , E ( B ) vanishes at z 0 . The section ¯ E , E ( B ) being SU ( n + 1 ) -invariant, it follows that ¯ E , E ( B ) vanishes identically; recall that the action of SU ( n + 1 ) on C P 1 is transitive. Consequently, the C isomorphism B is actually holomorphic.
We already noted that B takes the Hermitian metric h to h , and it also intertwines the actions of SU ( n + 1 ) on E and E . Therefore, B is an isomorphism between the two SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles ( E , h , ρ ) and ( E , h , ρ ) . This completes the proof of the proposition. □

3. An Equivariant Principal Bundle

Fix a point z 0 C P n . Let
G : = H z 0 SU ( n + 1 )
be the corresponding isotropy subgroup (see (9)). Since the action of SU ( n + 1 ) on C P n is transitive, the quotient SU ( n + 1 ) / G , where G is the subgroup in (16), is identified with C P n . This identification is constructed by sending any g SU ( n + 1 ) to f ( g ) ( z 0 ) C P n , where f is the homomorphism in (1). Consider the quotient map
q : SU ( n + 1 ) SU ( n + 1 ) / G = C P n .
It gives a C principal G-bundle on C P n . We will show that this principal G-bundle
P : = ( SU ( n + 1 ) , q )
on C P n has a tautological connection.
To construct the tautological connection on the principal G-bundle P in (18), consider the Lie algebra s u ( n + 1 ) of SU ( n + 1 ) ; the Killing form on it will be denoted by κ . We note that κ is a positive definite inner product on s u ( n + 1 ) . Let
g = Lie ( G ) s u ( n + 1 )
be the Lie subalgebra of the Lie subgroup G in (16). We have the orthogonal complement
W : = g s u ( n + 1 )
of g for the inner product κ on s u ( n + 1 ) . Let
δ : s u ( n + 1 ) g
be the orthogonal projection for the inner product κ on s u ( n + 1 ) . So kernel ( δ ) = W (see (19)). Using the left-translation action of SU ( n + 1 ) on itself, the real tangent bundle T R SU ( n + 1 ) SU ( n + 1 ) is identified with the trivial vector bundle SU ( n + 1 ) × s u ( n + 1 ) SU ( n + 1 ) with fiber s u ( n + 1 ) . Using this identification, the homomorphism δ produces a C g -valued 1-form on SU ( n + 1 ) ; this 1-form is evidently preserved by the left-translation action of SU ( n + 1 ) on itself. Let
ω C ( SU ( n + 1 ) , ( T R SU ( n + 1 ) ) g )
be this SU ( n + 1 ) -invariant g -valued 1-form on SU ( n + 1 ) given by δ . Next, note that the restriction of ω to any fiber of the projection q in (17) coincides with the Maurer–Cartan form on the fiber of the principal G-bundle P on C P n in (18). Moreover, ω is G-equivariant for the right action of G on SU ( n + 1 ) when we equip g with the adjoint action of G. Consequently, ω defines a connection on the principal G-bundle P on C P n ; see [13]. Let
0
be this connection on principal G-bundle P given by ω . We note that the left-translation action of SU ( n + 1 ) on itself preserves the connection 0 in (21) because the 1-form ω is SU ( n + 1 ) -invariant.
The adjoint vector bundle for the principal G-bundle P in (18) will be denoted by ad ( P ) . Let
K ( 0 ) C ( C P n , ad ( P ) 2 ( T R C P n ) )
be the curvature of the connection 0 in (21). Since the left-translation action of SU ( n + 1 ) on itself preserves the connection 0 , we conclude that the section K ( 0 ) in (22) is SU ( n + 1 ) -invariant. Let
K ( 0 ) = K ( 0 ) 2 , 0 K ( 0 ) 1 , 1 K ( 0 ) 0 , 2
be the Hodge type decomposition of the ad ( P ) -valued 2-form K ( 0 ) in (22).
Proposition 2.
In (23),
K ( 0 ) 2 , 0 = 0 = K ( 0 ) 0 , 2 ;
in other words, the equality
K ( 0 ) = K ( 0 ) 1 , 1
holds.
Proof. 
Since K ( 0 ) in (22) is SU ( n + 1 ) -invariant, and the action of each element of SU ( n + 1 ) on C P n preserves the complex structure of C P n , we conclude that K ( 0 ) 2 , 0 , K ( 0 ) 1 , 1 and K ( 0 ) 0 , 2 in (23) are all SU ( n + 1 ) -invariant.
The action of SU ( n + 1 ) on P induces an action of SU ( n + 1 ) on the adjoint vector bundle ad ( P ) .
Now, consider the center Z G : = Z ( H z 0 ) H z 0 = G (see (11) and (16)). The action of SU ( n + 1 ) on P produces an action of the group Z G on the fiber ad ( P ) z 0 of ad ( P ) over the point z 0 . It is easy to see that this action of Z G on ad ( P ) z 0 is the trivial one. On the other hand, as noted in the proof of Proposition 1, for the action of the group Z G = U ( 1 ) (see (12)) on the fiber ( T z 0 0 , 1 C P n ) , any λ Z G = U ( 1 ) acts as multiplication with 1 / λ n + 1 . Therefore, any λ Z G = U ( 1 ) acts on 2 ( T z 0 0 , 1 C P n ) as multiplication with 1 / λ 2 ( n + 1 ) . Hence, any λ Z G acts on ad ( P ) z 0 2 ( T z 0 0 , 1 C P n ) as multiplication with 1 / λ 2 ( n + 1 ) . This implies that no nonzero element of ad ( P ) z 0 2 ( T z 0 0 , 1 C P n ) is fixed by the action of Z G . Since K ( 0 ) 0 , 2 in (23) is SU ( n + 1 ) -invariant, and no nonzero element of ad ( P ) z 0 2 ( T z 0 0 , 1 C P n ) is fixed by the action of Z G , we conclude that
K ( 0 ) 0 , 2 = 0 .
For the action of the group Z G = U ( 1 ) on the fiber ( T z 0 1 , 0 C P n ) , any λ Z G = U ( 1 ) acts as multiplication with λ n + 1 . Therefore, repeating the above argument, we conclude that no nonzero element of ad ( P ) z 0 2 ( T z 0 1 , 0 C P n ) is fixed by the action of Z G . Hence, we have
K ( 0 ) 2 , 0 = 0
as well. This completes the proof. □

4. Equivariant Vector Bundle for a Representation

Consider the subgroup G SU ( n + 1 ) in (16). Let V be a finite dimensional complex vector space and
ρ : G GL ( V )
a homomorphism. Let
E V = P × G V C P n
be the vector bundle associated to the principal G-bundle P (see (18)) for the G-module V in (24). We recall that E V is a quotient P × V where two elements ( y 1 , v 1 ) and ( y 2 , v 2 ) of P × V are identified if there is an element g G such that y 2 = y 1 g and v 2 = ρ ( g 1 ) ( v 1 ) . The action of SU ( n + 1 ) on P produces an action of SU ( n + 1 ) on E V . More precisely, consider the following action of SU ( n + 1 ) on P × V = SU ( n + 1 ) × V : the action of any g SU ( n + 1 ) sends any ( y , v ) P × V to ( g y , v ) . This action of SU ( n + 1 ) on P × V = SU ( n + 1 ) × V produces an action of SU ( n + 1 ) on the quotient space E V .
Since the group G is compact, there is a positive definite Hermitian structure h 0 on V such that the image of the homomorphism ρ in (24) is contained in the subgroup of GL ( V ) consisting of all automorphisms of V that preserve the Hermitian structure h 0 . Now, it can be seen that h 0 produces a Hermitian structure on the vector bundle E V in (25). Indeed, the Hermitian structure h 0 on V produces a Hermitian structure on the trivial vector bundle P × V P with fiber V. Since the action of G on V given by ρ preserves h 0 , this Hermitian structure on the trivial vector bundle P × V P descends to a Hermitian structure on the vector bundle E V over C P n . The Hermitian structure on E V obtained this way will be denoted by h.
The above action of SU ( n + 1 ) on E V clearly preserves the Hermitian structure h on E V .
Next, consider the connection 0 on the principal G-bundle P constructed in (21). It induces a connection on any vector bundle associated to P . In particular, 0 induces a connection on the vector bundle E V in (25). This induced connection on E V will be denoted by V . We note that the action of SU ( n + 1 ) on E V preserves the connection V because the action of SU ( n + 1 ) on P preserves the connection 0 .
The connection V on E V clearly preserves the Hermitian structure h on E V .
Let K ( V ) C ( C P n , End ( E V ) 2 ( T R SU ( n + 1 ) ) ) be the curvature of the connection V . Since the curvature K ( V ) is given by the curvature of 0 , from Proposition 2, we conclude that K ( V ) is of Hodge type ( 1 , 1 ) . From this, it follows that the ( 0 , 1 ) -component of the connection V produces a holomorphic structure on the vector bundle E V (see [14] (p. 9, Prop. 3.5) and [14] (p. 9, Prop. 3.7)).
The action of elements on SU ( n + 1 ) on E V preserves the above holomorphic structure on E V because the action of SU ( n + 1 ) on E V preserves the connection V .
Consequently, ( E V , h ) is an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n .
The following lemma summarizes the above construction.
Lemma 2.
Given a finite dimensional complex vector space V and a homomorphism
ρ : G GL ( V ) ,
there is a naturally associated SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle ( E V , h ) on C P n .

5. Representation for an Equivariant Vector Bundle

Let ( E , h ^ , ρ ^ ) be an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n . As in Section 3, fix a point z 0 C P n . V denotes the fiber E z 0 of E over the point z 0 . Consider the action of the subgroup G SU ( n + 1 ) (see (16)) on E z 0 = V . Let
ρ : G GL ( V )
be the homomorphism given by the action of G on V.
Lemma 2 associates an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle ( E V , h ) to ρ in (26).
Lemma 3.
There is a canonical C isomorphism
ϕ : E V E
such that
1. 
ϕ is SU ( n + 1 ) -equivariant,
2. 
ϕ takes the Hermitian structure h on E V to the Hermitian structure h ^ on E .
Proof. 
Consider the quotient map q in (17). The pulled-back vector bundle q E V SU ( n + 1 ) is canonically identified with the trivial vector bundle
SU ( n + 1 ) × V = P × V SU ( n + 1 ) ;
this follows immediately from the construction of E V from ρ . We will construct an isomorphism
ϕ ˜ : SU ( n + 1 ) × V q E
of vector bundles over SU ( n + 1 ) = P . Take any
( g , v ) SU ( n + 1 ) × V = SU ( n + 1 ) × E z 0 .
The map ϕ ˜ sends ( g , v ) to ( g , ρ ^ ( g , v ) ) q E , where ρ ^ is the map giving the action of SU ( n + 1 ) on E . Recall from Section 4 that E V is a quotient of SU ( n + 1 ) × V . It is easy to see that the isomorphism ϕ ˜ in (27) descends to an isomorphism
ϕ : E V E
of vector bundles over C P n .
From the construction of ϕ , it follows immediately that ϕ is SU ( n + 1 ) -equivariant.
Since the action of SU ( n + 1 ) on E preserves the Hermitian structure h ^ on E , it follows that ϕ takes the Hermitian structure h on E V to the Hermitian structure h ^ on E . □
From Lemma 2, we know that ( E V , h ) is an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle. It should be clarified that the isomorphism ϕ in Lemma 3 need not be holomorphic.
The Dolbeault operators on the holomorphic vector bundles E and E V will be denoted by ¯ E and ¯ E V , respectively (see [14] (p. 10, Prop. 3.9)). We have
θ : = ¯ E ¯ E V C ( C P n , End ( E V ) ( T 0 , 1 C P n ) ) .
Since ¯ E and ¯ E V define holomorphic structures, it follows that
¯ E V θ + [ θ , θ ] = 0
[14] (p. 9, Prop. 3.5).
Proposition 3.
Let
β C ( C P n , End ( E V ) ( T 0 , 1 C P n ) ) SU ( n + 1 ) C ( C P n , End ( E V ) ( T 0 , 1 C P n ) )
be an SU ( n + 1 ) -invariant C ( 0 , 1 ) -form on C P n with values in End ( E V ) . Then,
¯ E V β = 0 ,
where ¯ E V is the Dolbeault operator in (29).
Proof. 
Consider the center
U ( 1 ) = Z G = Z ( H z 0 ) = G SU ( n + 1 )
of G (see (16), (11) and (12)). The action of SU ( n + 1 ) on E V produces an action of U ( 1 ) = Z G on the fiber E z 0 = : V . Let
V = i = 1 V i
be the isotypical decomposition of the U ( 1 ) -module V. For each 1 i , let
ν i Z
be the unique integer satisfying the following condition: The action of any λ U ( 1 ) = Z G on V i sends any v V i to λ ν i · v .
Since U ( 1 ) = Z G is the center of G, the action of G on V, given by the action of SU ( n + 1 ) on E V , preserves the decomposition in (30). In other words, the action of G on V preserves each V i in (30).
Note that Lemma 2 associates to each G-module V i an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n . For each 1 i , let ( E V i , h i ) be the SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n for V i . From (30), we have
( E V , h ) = i = 1 ( E V i , h i ) .
We have the maps
E V i t i E V q i E V i
where t i is the inclusion map and q i is the projection map constructed using the decomposition in (32).
Consider the section β in the proposition. For every 1 i , j , let
β i , j : E V i E V j ( T 0 , 1 C P n )
be the homomorphism given by the following composition of homomorphisms
E V i t i E V β E V ( T 0 , 1 C P n ) q j id E V j ( T 0 , 1 C P n ) ,
where t i and q j are the homomorphisms in (33). Then, we have
β = i , j = 1 β i , j .
Note that each section β i , j is preserved by the action of SU ( n + 1 ) because
  • β is preserved by the action of SU ( n + 1 ) ,
  • the homomorphisms t i and q i in (33) are also preserved by the action of SU ( n + 1 ) .
Recall that for the action of the group Z G = U ( 1 ) on the fiber ( T z 0 0 , 1 C P n ) , any λ Z G = U ( 1 ) acts as multiplication with 1 / λ n + 1 . Therefore, if β i , j 0 , then we have
ν i = ν j n 1
(see (31)).
From (34), it follows that
¯ E V β = i , j = 1 ¯ E V β i , j .
Note that
¯ E V β i , j C ( C P n , Hom ( E V i , E V j ) ( T 0 , 1 C P n ) ) ,
and ¯ E V β i , j is preserved by the action of SU ( n + 1 ) because β i , j is preserved by the action of SU ( n + 1 ) . Since for the action of the group Z G = U ( 1 ) on the fiber ( T z 0 0 , 2 C P n ) , any λ Z G = U ( 1 ) acts as multiplication with 1 / λ 2 n + 2 , it follows that if ¯ E V β i , j 0 ; then, we have
ν i = ν j 2 n 2 .
Comparing this with (35) we conclude that ¯ E V β i , j = 0 if β i , j 0 . Now, the proposition follows from (36). □
Corollary 1.
The term ¯ E V θ in (29) vanishes identically.
Proof. 
The section θ in (28) is preserved by the action of SU ( n + 1 ) because the two Dolbeault operators ¯ E and ¯ E V are both preserved by the action of SU ( n + 1 ) . Hence, from Proposition 3, it follows that ¯ E V θ = 0 . □

6. Equivariant Holomorphic Hermitian Vector Bundles

As before, G : = H z 0 SU ( n + 1 ) .
Consider all pairs of the form ( ρ , v ) , where
ρ : G GL ( V ρ )
is a finite dimensional complex representation of the group G and
v ( End ( V ρ ) ( T z 0 0 , 1 C P n ) ) Z G End ( V ρ ) ( T z 0 0 , 1 C P n ) ,
where Z G = U ( 1 ) G is the center of G. For any such pair ( ρ , v ) , note that we have
[ v , v ] End ( V ρ ) ( T z 0 0 , 2 C P n ) .
Let S denote the space of all pairs ( ρ , v ) of the above type such that
[ v , v ] = 0 .
Two elements ( ρ , v ) and ( ρ , v ) of S will be called equivalent if there is an isomorphism
ψ : V ρ V ρ
such that the following two conditions hold:
  • ψ ρ ( g ) = ρ ( g ) ψ for all g G (note that both ψ ρ ( g ) and ρ ( g ) ψ are homomorphisms from V ρ to V ρ ),
  • v ψ = ( ψ Id ( T z 0 0 , 1 C P n ) ) v (note that both sides are homomorphisms from V ρ to V ρ ( T z 0 0 , 1 C P n ) ).
Let
S
denote the equivalence classes of elements of S .
Theorem 2.
There is a canonical bijection between S (see (38)) and the space of all isomorphisms classes of SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n .
Proof. 
As in Section 5, take any SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle ( E , h ^ ) on C P n .
Consider ρ in (26) and
θ ( z 0 ) End ( E V ) ( T z 0 0 , 1 C P n ) )
constructed in (28). From (29) and Corollary 1, it follows immediately that
[ θ ( z 0 ) , θ ( z 0 ) ] = 0 .
Hence, we have ( ρ , θ ( z 0 ) ) S .
We send ( E , h ^ ) to the element of S given by the pair ( ρ , θ ( z 0 ) ) . This produces a map to S from the space of all isomorphism classes of SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundles on C P n .
For the inverse map, take any ( ρ , v ) S . Using Lemma 2, the homomorphism ρ produces an SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle ( E V ρ , h ) on C P n . Since v is fixed by the action of Z G on End ( V ρ ) ( T z 0 0 , 1 C P n ) , using the actions of SU ( n + 1 ) on E V ρ and C P n , the element v produces a SU ( n + 1 ) -invariant section
θ C ( C P n , End ( E V ρ ) ( T 0 , 1 C P n ) ) SU ( n + 1 ) .
The given condition in (37) that [ v , v ] = 0 implies that
[ θ , θ ] = 0
because θ is preserved by the action of SU ( n + 1 ) and the action of SU ( n + 1 ) is transitive.
Let ¯ E V ρ be the Dolbeault operator for the holomorphic vector bundle E V ρ . Consider the Dolbeault operator ¯ E V ρ + θ on the C vector bundle E V ρ . From (39) and Proposition 3, we conclude that
¯ E V θ + [ θ , θ ] = 0 .
Therefore, ¯ E V ρ + θ defines a holomorphic structure on the C vector bundle E V ρ .
The Hermitian structure h on E V ρ remains unchanged. This new holomorphic Hermitian vector bundle is evidently SU ( n + 1 ) -equivariant. This produces the inverse map from S to the space of all isomorphisms classes of the SU ( n + 1 ) -equivariant holomorphic Hermitian vector bundle on C P n . □

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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Biswas, I.; Machu, F.-X. Equivariant Holomorphic Hermitian Vector Bundles over a Projective Space. Mathematics 2024, 12, 3757. https://doi.org/10.3390/math12233757

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Biswas I, Machu F-X. Equivariant Holomorphic Hermitian Vector Bundles over a Projective Space. Mathematics. 2024; 12(23):3757. https://doi.org/10.3390/math12233757

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Biswas, Indranil, and Francois-Xavier Machu. 2024. "Equivariant Holomorphic Hermitian Vector Bundles over a Projective Space" Mathematics 12, no. 23: 3757. https://doi.org/10.3390/math12233757

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Biswas, I., & Machu, F.-X. (2024). Equivariant Holomorphic Hermitian Vector Bundles over a Projective Space. Mathematics, 12(23), 3757. https://doi.org/10.3390/math12233757

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