The connects representation theory to geometry. It shows how irreducible representations of compact Lie groups relate to cohomology of vector bundles on flag manifolds. This deep result bridges algebra and topology.
Understanding this theorem is key for grasping representation theory of Lie groups. It provides a powerful tool for constructing and analyzing representations, with applications in math physics and algebraic geometry.
Borel-Weil-Bott Theorem Statement
Geometric Realization of Irreducible Representations
Top images from around the web for Geometric Realization of Irreducible Representations
Representation Theory [The Physics Travel Guide] View original
Is this image relevant?
1 of 3
The Borel-Weil-Bott theorem provides a geometric realization of the irreducible representations of a compact, connected Lie group G in terms of the cohomology of certain homogeneous vector bundles over the flag manifold G/B, where B is a Borel subgroup of G
For a dominant integral weight λ, the theorem states that the irreducible representation of G with λ can be realized as the space of global sections of a certain line bundle Lλ over G/B
The theorem establishes a deep connection between the representation theory of Lie groups and the geometry and topology of flag manifolds
The flag manifold G/B is an example of a homogeneous space, i.e., a manifold on which a Lie group acts transitively
Cohomology and Vanishing Results
The theorem provides a vanishing result for the higher cohomology groups of Lλ when λ is dominant
In this case, the representation is completely determined by the space of global sections H0(G/B,Lλ)
For non-dominant weights, the theorem gives a precise description of the cohomology in terms of certain "dot actions" of the Weyl group on the weight lattice
The dot action is defined as w⋅λ=w(λ+ρ)−ρ, where ρ is half the sum of the positive roots
The cohomology group Hi(G/B,Lλ) is isomorphic to the irreducible representation with highest weight w⋅λ, where w is an element of the Weyl group with length i
The study of the cohomology of homogeneous spaces is a rich and active area of research in algebraic geometry and representation theory, with connections to other fields such as number theory and mathematical physics
Representations of Compact Lie Groups
Constructing Irreducible Representations
To apply the Borel-Weil-Bott theorem, one must first identify the dominant integral weights of the Lie group G, which correspond to the irreducible representations
For each dominant integral weight λ, construct the associated line bundle Lλ over the flag manifold G/B using the Borel-Weil construction
The space of global sections of Lλ, denoted H0(G/B,Lλ), is an irreducible representation of G with highest weight λ
When λ is dominant, the higher cohomology groups Hi(G/B,Lλ) vanish for i>0, and the representation is completely determined by H0(G/B,Lλ)
Understanding Dominant Integral Weights
To apply the Borel-Weil-Bott theorem effectively, one must be able to identify the dominant integral weights of a given compact Lie group and understand their relationship to the root system and Weyl group
Dominant integral weights are weights that lie in the fundamental Weyl chamber, which is determined by the choice of a set of positive roots
The dominant integral weights are in one-to-one correspondence with the irreducible representations of the Lie group G
Examples of dominant integral weights for classical Lie groups:
For SU(n), the dominant integral weights are n-tuples of integers (λ1,…,λn) satisfying λ1≥λ2≥⋯≥λn
For SO(2n+1), the dominant integral weights are n-tuples of integers or half-integers (λ1,…,λn) satisfying λ1≥λ2≥⋯≥λn≥0
Borel-Weil-Bott Theorem vs Cohomology
Cohomology of Homogeneous Vector Bundles
The Borel-Weil-Bott theorem relates the representation theory of G to the cohomology of certain vector bundles over the homogeneous space G/B
The theorem can be generalized to other homogeneous spaces, such as generalized flag manifolds G/P, where P is a parabolic subgroup of G
The cohomology of homogeneous vector bundles over G/P can be used to construct and study representations of G, analogous to the case of G/B
Examples of generalized flag manifolds:
Grassmannians Gr(k,n), which parametrize k-dimensional subspaces of an n-dimensional vector space
Orthogonal Grassmannians OG(n,2n), which parametrize n-dimensional isotropic subspaces of a 2n-dimensional vector space with a non-degenerate symmetric bilinear form
Geometric Context and Applications
Familiarity with the structure and properties of flag manifolds and their generalization to other homogeneous spaces is crucial for understanding the geometric context of the Borel-Weil-Bott theorem
The theorem has important applications in various areas of mathematics, such as algebraic geometry, complex analysis, and mathematical physics
In algebraic geometry, the Borel-Weil-Bott theorem is used to study the cohomology of vector bundles over flag varieties and their generalizations, which play a central role in the classification of algebraic varieties
In complex analysis, the theorem provides a way to construct and study certain spaces of holomorphic functions on complex manifolds, such as the Bergman and Hardy spaces
In mathematical physics, the Borel-Weil-Bott theorem is used to analyze the representation theory of Lie groups that arise in the study of symmetries in physical systems, such as gauge theories and conformal field theories
Representation Theory Applications
Classical Lie Groups
The ability to apply the Borel-Weil-Bott theorem to concrete examples, such as the classical Lie groups (e.g., SU(n), SO(n), Sp(n)), is important for developing a deep understanding of the representation theory of compact Lie groups
For the special unitary group SU(n), the theorem can be used to construct and study the irreducible representations corresponding to the dominant integral weights, which are given by Young diagrams or partitions
For the special orthogonal group SO(n), the theorem provides a way to realize the irreducible representations in terms of the cohomology of certain vector bundles over the orthogonal flag manifold SO(n)/T, where T is a maximal torus
For the symplectic group Sp(n), the Borel-Weil-Bott theorem can be applied to study the irreducible representations in terms of the cohomology of vector bundles over the symplectic flag manifold Sp(n)/T
Interdisciplinary Connections
Recognizing the connections between the Borel-Weil-Bott theorem and other areas of mathematics can lead to new insights and applications of the theorem
In number theory, the Borel-Weil-Bott theorem has been used to study the cohomology of certain arithmetic groups and their representations, which play a role in the Langlands program
In mathematical physics, the theorem has been applied to the study of the representation theory of infinite-dimensional Lie groups, such as loop groups and affine Kac-Moody groups, which arise in the context of conformal field theory and integrable systems
The Borel-Weil-Bott theorem has also found applications in the study of the geometry and topology of certain moduli spaces, such as the moduli space of stable vector bundles over a Riemann surface, which is related to the geometric Langlands correspondence