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Closed-subgroup theorem

The closed-subgroup theorem, also known as Cartan's closed subgroup theorem, asserts that every closed of a is itself a , inheriting a manifold from the ambient group and thus forming an embedded submanifold. This result ensures that such subgroups possess a compatible and , preserving the differentiable essential for analyzing continuous symmetries. Proved in its general form by in 1930, the theorem built upon John von Neumann's 1929 demonstration of the result specifically for the general linear group GL(n, ℝ). Cartan's proof leverages the from the to the group, showing that the subgroup is generated by a Lie subalgebra and is closed under the group operations, thereby confirming its smooth embedding via the and local diffeomorphisms. The theorem holds profound significance in , as it guarantees that closed subgroups—such as the O(n) or special orthogonal group SO(n)—are themselves Lie groups, facilitating their study in applications ranging from to and . Without this result, distinguishing abstract subgroups from those with smooth structure would complicate the of groups, particularly in finite-dimensional settings over the reals or complexes. It also underpins corollaries, like the fact that all closed subgroups of GL(n, ℂ) are Lie groups, underscoring the theorem's role in bridging algebraic, topological, and analytic aspects of Lie groups.

Introduction

Theorem Statement

The closed-subgroup theorem, a fundamental result in the theory of s, asserts that every closed H of a G is itself a of G. More formally, let G be a over \mathbb{R} or \mathbb{C}, equipped with its manifold , and let H be a of G that is closed as a in this . Then H admits a unique smooth manifold structure making the inclusion H \hookrightarrow G a smooth homomorphism, with the group multiplication and inversion on H inherited from G, and H is an embedded submanifold of G. The \mathfrak{h} of H is then given by \mathfrak{h} = \{ X \in \mathfrak{g} \mid \exp(tX) \in H \text{ for all sufficiently small } t \in \mathbb{R} \}, where \mathfrak{g} denotes the of G and \exp: \mathfrak{g} \to G is the . This theorem establishes a direct correspondence between closed subgroups and Lie subalgebras via the , thereby connecting the topological condition of closure to the differential structure of groups. The result was originally proved for the special case of closed subgroups of the general linear group by in 1929, and extended to arbitrary groups by in 1930.

Historical Development

The closed-subgroup theorem traces its origins to the foundational ideas of in the late , where he developed the theory of continuous transformation groups as a means to study symmetries in equations, establishing the framework for what would become theory. A pivotal early result came in 1929 from , who proved that any closed subgroup of the general linear group in a finite-dimensional real or complex is itself a , thereby linking topological closure directly to the smooth structure of such s. This work addressed linear cases and highlighted the importance of closure in preserving the properties. The modern formulation of the theorem for arbitrary s is attributed to in , who demonstrated that every closed of a inherits a structure as an embedded , with the smooth topology agreeing with the ; this precise statement appeared in his treatise on s around 1937. contributed to the broader context of theory during this period through his work on representations and classical groups, which influenced the understanding of structures. In the , the played a central role in resolving , with Andrew Gleason, Deane Montgomery, and Leo Zippin proving that topological groups locally homeomorphic to spaces are groups, and emphasizing how closed subgroups ensure the compatibility of analytic structures in such settings; their seminal 1955 monograph formalized these connections. While the finite-dimensional case solidified during this era, later developments by in the 1980s extended aspects of theory, including subgroup considerations, to infinite-dimensional settings, though the core remains focused on finite dimensions.

Background Concepts

Lie Groups and Subgroups

A is a that combines the algebraic properties of a group with the geometric properties of a manifold. Specifically, it is a group G equipped with a manifold structure such that the group multiplication map G \times G \to G, (g, h) \mapsto gh, and the inversion map G \to G, g \mapsto g^{-1}, are maps. This framework allows for the study of continuous symmetries in and physics, where the smoothness ensures compatibility between infinitesimal and global structures. Subgroups of a G are subsets H \subseteq G that form groups under the restriction of the multiplication and inversion operations from G. These algebraic s need not be closed in the topological sense nor endowed with a manifold inherited from G. In contrast, a arises when H is itself a with the induced , typically requiring the H \to G to be . Central to the local structure of Lie groups is the associated , which captures the behavior near the . The \mathfrak{g} of [G](/page/G) is the at the T_e G, viewed as a over \mathbb{R} or \mathbb{C}, equipped with a [X, Y] defined as the of the left-invariant vector fields on G corresponding to tangent vectors X, Y \in \mathfrak{g}. This bracket satisfies bilinearity, antisymmetry, and the , providing a linear approximation to the nonlinear group operations. For smooth subgroups, a key distinction lies between immersed and embedded realizations. An immersed subgroup H of G has an inclusion map that is a smooth immersion—locally a diffeomorphism onto its image—but the image may be dense or fail to be a proper submanifold globally. An embedded subgroup, however, is a smooth submanifold of G, where the inclusion is both an immersion and a topological embedding, with the image being a closed submanifold of G.

Topological Closure in Lie Groups

In the context of Lie groups, the underlying topological structure ensures that the group operations—multiplication and inversion—are continuous maps with respect to the manifold topology, making every a . This continuity is fundamental, as it allows the to interact seamlessly with the geometric properties of the manifold, enabling the study of limits and convergence within the group. A subgroup H of a Lie group G is defined as closed if it forms a closed of G in the topological sense, meaning the complement G \setminus H is open. In contrast, dense subgroups, whose topological closure equals the entire group G, serve as counterexamples illustrating that arbitrary subgroups do not automatically possess a structure, even if the ambient group does. Such dense subgroups highlight the necessity of closure for inheriting the manifold properties and associated structure, like the . Lie groups are standardly assumed to be Hausdorff topological spaces, which guarantees the uniqueness of limits for convergent sequences and nets, preventing pathological behaviors in the topology. This Hausdorff condition is crucial for the well-definedness of the manifold structure and ensures that the group topology supports the required separation properties for analytic continuations. Finite-dimensional Lie groups over the real numbers \mathbb{R} are equipped with a natural uniform structure derived from their complete metric topology, rendering them Polish groups—separable topological groups that are completely metrizable. As Polish spaces, these Lie groups satisfy the , which asserts that they cannot be expressed as countable unions of nowhere dense sets, providing a topological foundation for genericity arguments and structural theorems in the theory.

Illustrative Examples

Examples of Closed Subgroups

The special orthogonal group SO(n) provides a fundamental example of a closed subgroup within the general linear group GL(n, \mathbb{R}). It comprises all n \times n real matrices A that satisfy A^T A = I_n and \det A = 1, where I_n denotes the n \times n ; these algebraic conditions ensure SO(n) is a closed subset of GL(n, \mathbb{R}) under its standard topology induced from the space of all real matrices. The Lie algebra of SO(n), denoted \mathfrak{so}(n), consists precisely of the n \times n skew-symmetric real matrices, that is, matrices X fulfilling X^T = -X. Another illustrative case is the torus represented by the circle group U(1), which embeds as a closed of GL(2, \mathbb{R}) through the parametrization of rotation matrices: \begin{pmatrix} \cos \theta & -\sin \theta \\ \sin \theta & \cos \theta \end{pmatrix}, where \theta ranges over [0, 2\pi). This subgroup is compact, rendering it closed in the Hausdorff topological space GL(2, \mathbb{R}). Discrete subgroups offer further examples, particularly finite groups such as cyclic groups \mathbb{Z}/k\mathbb{Z} embedded pointwise into a like GL(n, \mathbb{R}) via faithful representations (e.g., permutation matrices for suitable n \geq k). Such embeddings yield closed subgroups because finite sets are compact and thus closed in any , including Lie groups. In each of these instances, the smoothness of the subgroups as groups is verified through explicit manifold charts that align with the of the ambient , consistent with the closed-subgroup theorem's assurance of an induced manifold structure.

Examples of Non-Closed Subgroups

One prominent example of a non-closed subgroup arises in the 2-torus T^2 = \mathbb{R}^2 / \mathbb{Z}^2, considered as a compact under componentwise addition modulo 1. Consider the subgroup H generated by the element (\alpha, \beta) \in T^2, where \alpha / \beta is irrational (more precisely, where 1, \alpha, \beta are linearly independent over \mathbb{Q}). This subgroup is the image of the embedding \mathbb{R} \to T^2 given by t \mapsto (t \alpha \mod 1, t \beta \mod 1), which is an immersed 1-dimensional submanifold diffeomorphic to \mathbb{R}. However, H is dense in T^2 and thus not closed, as its closure is the entire . A similar phenomenon occurs in the Lie group \mathrm{SL}(2, \mathbb{R}). The maximal compact subgroup \mathrm{SO}(2) consists of rotation matrices \begin{pmatrix} \cos \theta & -\sin \theta \\ \sin \theta & \cos \theta \end{pmatrix} for \theta \in [0, 2\pi). The subgroup K generated by rotations through angles that are integer multiples of $2\pi \alpha, where \alpha is irrational, is \{ \begin{pmatrix} \cos (2\pi n \alpha) & -\sin (2\pi n \alpha) \\ \sin (2\pi n \alpha) & \cos (2\pi n \alpha) \end{pmatrix} \mid n \in \mathbb{Z} \}. This discrete subgroup is dense in \mathrm{SO}(2) and hence not closed in \mathrm{SL}(2, \mathbb{R}), since \mathrm{SO}(2) itself is closed but K fails to contain isolated points outside its closure. Such non-closed subgroups illustrate the necessity of the closure assumption in the closed-subgroup theorem, as they are immersed subgroups but not submanifolds. Consequently, they lack the smooth manifold structure required to be subgroups in the standard sense, preventing the formation of a well-defined or at every point that aligns with the ambient group's . The density of these subgroups can be visualized through Weyl's : for irrational \alpha, the sequence n \alpha \mod 1 is equidistributed (and thus dense) in [0,1), implying that the orbit under repeated addition fills the torus uniformly without gaps. In contrast, closed subgroups embed as submanifolds.

Properties and Extensions

Conditions for Subgroup Closure

In Lie groups, analytic subgroups—those generated by one-parameter subgroups via the from a subalgebra—are always topologically closed. This follows from the fact that such subgroups inherit a smooth manifold structure compatible with the group operations and the ambient , ensuring no accumulation points outside the subgroup itself. Compact subgroups of Lie groups are necessarily closed. Since Lie groups are Hausdorff topological spaces, any compact subset is closed in the relative , and prevents the subgroup from having points exterior to itself. This property extends the Heine-Borel from spaces to the more general locally compact setting of Lie groups. Finitely generated subgroups of nilpotent Lie groups need not be closed; dense examples exist, generated by elements whose orbits fill the group without forming a closed set. However, discrete subgroups within these groups are always closed, as the discrete topology induced on them implies no accumulation points in the ambient space. Such discrete subgroups are closed regardless of index, though those of finite covolume (lattices) play a prominent role in homogeneous space constructions. A general for of a H in a G is that H intersects every compact subset of G in a compact set. In the \sigma-compact, locally compact framework of s, this ensures that H has no limit points outside itself, as intersections with compacta capture the topological behavior exhaustively. Equivalently, H is closed the G/H is Hausdorff, since the projection map identifies closedness with the separation of distinct cosets in the topology.

Converse Results

A fundamental converse to the closed-subgroup theorem asserts that every of a is closed in the ambient topology. This equivalence—namely, that a is if and only if it is closed—holds generally for finite-dimensional and ensures that the smooth structure induced from the embedding aligns with the intrinsic group topology. For smooth immersed , the situation differs: such subgroups need not be closed, even when the ambient is connected. A classic counterexample is the irrational winding subgroup on the 2-torus \mathbb{T}^2 = \mathbb{R}^2 / \mathbb{Z}^2, generated by the one-parameter flow t \mapsto (t \mod 1, \alpha t \mod 1) where \alpha is irrational; this yields a connected immersed submanifold diffeomorphic to \mathbb{R} that is dense (hence non-closed) in \mathbb{T}^2. However, in disconnected , additional pathologies arise, such as immersed subgroups that fail to be closed due to dense components interacting with discrete parts, exacerbating the non-closure issue beyond the connected case. A related refinement concerns analytic subgroups, defined as subgroups that are real-analytic submanifolds of the ambient . The Montgomery–Zippin theorem, building on , implies that every analytic subgroup of a finite-dimensional Lie group is closed, as such subgroups inherit a unique Lie group structure compatible with the ambient topology and must coincide with their topological closure. This result underscores the stronger regularity provided by analyticity over mere smoothness. These converses fail in the infinite-dimensional setting without supplementary topological assumptions, such as completeness of the model space (e.g., Banach or Fréchet groups). For instance, in separable Hilbert groups, there exist closed that are not subgroups, and conversely, immersed subgroups that remain non-closed despite satisfying finite-dimensional analogs of conditions. Additional structure, like the interaction of the with the , is required to recover closure properties.

Applications

In Representation Theory

In the context of unitary representations of compact s, the closed-subgroup theorem guarantees that any closed inherits the smooth structure of a , enabling the Peter-Weyl theorem to decompose unitary representations into orthogonal direct sums of finite-dimensional irreducible components. This decomposition is essential for analyzing how representations of the ambient group restrict to closed s, preserving irreducibility or allowing controlled branching rules. For instance, the representation ring of a closed H of a compact G embeds into that of G via , facilitating the classification of representations through data. The theorem also plays a pivotal role in the construction of induced representations. For a closed subgroup H of a Lie group G and a smooth representation \pi of H, the induced representation \operatorname{Ind}_G^H \pi is smooth, ensuring that the resulting action on functions over the quotient space G/H is continuous and differentiable. This smoothness property is critical for extending representation-theoretic techniques from subgroups to the full group, particularly in non-compact settings where topological closure prevents pathological behaviors. Mackey theory provides a deeper connection, where the closed-subgroup theorem underpins the generalization of Frobenius reciprocity to s. In this framework, closedness of H ensures that the intertwining number between \operatorname{Ind}_G^H \pi and a representation of G equals the dimension of invariants under \pi, allowing reciprocity between induction from H and restriction to H. This result extends classical finite-group reciprocity, relying on the Lie group structure afforded by closure. A illustration arises in the \operatorname{SU}(2), where the U(1) of diagonal matrices forms a . Inducing characters of U(1) to \operatorname{SU}(2) produces all finite-dimensional irreducible representations of \operatorname{SU}(2), each of odd dimension $2\ell + 1 for \ell \in \mathbb{N}_0, highlighting how enables explicit construction via highest weights.

In Homogeneous Spaces

In the context of Lie groups, the closed-subgroup theorem ensures that if H is a closed of a G, then the quotient space G/H inherits a natural manifold structure, with dimension equal to \dim G - \dim H. This structure arises because the canonical projection \pi: G \to G/H becomes a submersion, allowing G/H to be endowed with a compatible with the . Moreover, the existence of this facilitates the of functions on G/H using the on G, as the measure class on the quotient is well-defined precisely when H is closed, enabling disintegration theorems and invariant measures on homogeneous spaces. The closedness of H also guarantees that the projection \pi: G \to G/H is a principal H-bundle, ensuring local triviality in associated fiber bundle constructions. Specifically, the left action of H on G by multiplication is free and proper when H is closed, making \pi: G \to G/H a principal H-bundle with smooth total space and base. This property underpins the smooth structure of associated vector bundles and connections over G/H, which are crucial for geometric analysis on these spaces. Symmetric spaces provide a key application where closed subgroups play a central role. A Riemannian symmetric space can be realized as G/H, where G is a acting by isometries, and H is the closed centralizer of an involutive automorphism \sigma of G (i.e., \sigma^2 = \mathrm{id} and \sigma \neq \mathrm{id}). The fixed-point subgroup H = \{g \in G \mid \sigma(g) = g\} is closed (as the fixed points of a continuous ), and hence a by the closed-subgroup theorem, ensuring G/H is a smooth manifold equipped with a G-invariant Riemannian metric for which the geodesic symmetries are isometries. A canonical example is the space of positive definite matrices \mathrm{SL}(n,\mathbb{R})/\mathrm{SO}(n), which models and arises from the involution transposing matrices. In the study of actions on manifolds, the closed-subgroup theorem implies that stabilizers of points under actions are closed subgroups, leading to structures. For a of G on a manifold M, the \mathrm{Stab}_G(x) of a point x \in M is closed, hence a subgroup, and the G \cdot x is diffeomorphic to G / \mathrm{Stab}_G(x), inheriting a immersed structure. When the is proper, closed stabilizers further ensure that orbits are submanifolds, classifying them as components in the orbit decomposition of M. This classification is essential for understanding foliations and reduction in on such spaces.

Proof Outline

Key Technical Lemma

A central component in establishing the closed-subgroup theorem is a lemma describing the local behavior of a closed subgroup H near the identity element e of the ambient G. Let \mathfrak{g} denote the of G and \mathfrak{h} the of H, defined as \mathfrak{h} = \{ X \in \mathfrak{g} \mid \exp(tX) \in H \ \forall t \in \mathbb{R} \}. The lemma asserts that there exists a neighborhood U of e in G such that H \cap U = \exp(\mathfrak{h}) \cap U, where \exp: \mathfrak{g} \to G is the . The \exp: \mathfrak{g} \to G is smooth, and its at the d\exp_0: \mathfrak{g} \to T_e G \cong \mathfrak{g} is the isomorphism. By the , \exp is a : there are neighborhoods W of $0 in \mathfrak{g} and V of e in G such that \exp restricts to a W \to V. Moreover, \exp is surjective onto a neighborhood of e within the of the in G. The proof of the lemma relies on a tubular neighborhood construction or slice theorem via a direct sum decomposition \mathfrak{g} = \mathfrak{h} \oplus \mathfrak{m}, where \mathfrak{m} is a complementary subspace. Define \Phi: \mathfrak{g} \to G by \Phi(X + Y) = \exp(X) \exp(Y) for X \in \mathfrak{h}, Y \in \mathfrak{m}; this map is a diffeomorphism onto its image near e, with d\Phi_0 the identity. To show the equality, assume for contradiction a sequence g_n \in H \cap V with g_n \to e but g_n \notin \exp(\mathfrak{h}). Writing g_n = \exp(X_n) \exp(Y_n) with Y_n \in \mathfrak{m} \setminus \{0\} and X_n + Y_n \to 0, then \exp(-X_n) g_n = \exp(Y_n) \in H. For large n, Y_n is small, so Y_n = \log(\exp(Y_n)) \in \mathfrak{h}, contradicting \mathfrak{h} \cap \mathfrak{m} = \{0\}. Thus, near e, elements of H arise solely from \exp(\mathfrak{h}). This local equality, combined with the diffeomorphism property of \exp restricted to \mathfrak{h}, yields the desired result.

Core Proof Argument

The core proof of the closed-subgroup theorem proceeds by establishing that a closed subgroup H of a Lie group G with Lie algebra \mathfrak{g} inherits a smooth manifold structure and Lie group operations from G, building on a local technical lemma that provides a neighborhood of the identity in H diffeomorphic to an open subset of a vector space. To show the global structure, the local diffeomorphism near the identity—given by the exponential map restricted to a subspace—is extended across H using left translations by elements of H. Specifically, for any h \in H, the left translation \lambda_h: G \to G given by \lambda_h(g) = h g maps the local chart neighborhood in H to a neighborhood of h, yielding an atlas of charts that covers H and renders the inclusion H \hookrightarrow G a smooth embedding of submanifolds. This construction ensures H is a smooth submanifold of G of dimension equal to that of the local model. The Lie algebra \mathfrak{h} of H is identified as the subspace \mathfrak{h} = \{ X \in \mathfrak{g} \mid \exp(tX) \in H \ \forall t \in \mathbb{R} \text{ sufficiently small} \}, where \exp: \mathfrak{g} \to G is the exponential map. This set \mathfrak{h} is a vector subspace of \mathfrak{g} and is closed under the Lie bracket [\cdot, \cdot], as the one-parameter subgroups generated by [X, Y] for X, Y \in \mathfrak{h} remain in H by the Baker-Campbell-Hausdorff formula up to higher-order terms. The group operations on H are smooth as restrictions of those on G: the multiplication map m: H \times H \to H, m(h_1, h_2) = h_1 h_2, is the restriction of G's smooth , and similarly for the inverse map i: H \to H, i(h) = h^{-1}, which inherits smoothness from G's inversion. These restrictions are smooth because H is a smooth embedded in G. For the connected case, the proof first establishes the structure on the identity component H_0 using the above local-global extension, then handles the full H by noting that its connected components are the cosets K H_0 for finitely many coset representatives K (since H is second countable), each of which inherits smoothness as a translate of the submanifold H_0, forming a smooth . Finally, the adjoint action of G preserves \mathfrak{h}, as conjugation by g \in G maps one-parameter subgroups in H to those in H: specifically, \exp(t \operatorname{Ad}_g X) = g \exp(t X) g^{-1} \in H for X \in \mathfrak{h}, implying \operatorname{Ad}_g X \in \mathfrak{h}. This confirms the compatibility of \mathfrak{h} with G's structure.

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    ### Summary of Core Proof from ClosedLie.pdf
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    ### Summary of Core Proof Steps for Closed Subgroup Theorem (Rutgers Notes)