Lie groups blend smooth manifolds with group structures, enabling the study of continuous symmetries in mathematics and physics. They provide a powerful framework for analyzing transformations and symmetries in various fields.
Examples of Lie groups include matrix groups like and , as well as transformation groups like the Euclidean and Lorentz groups. These illustrate the diverse applications of theory across different areas of study.
Lie groups and their properties
Definition and essential characteristics
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A Lie group is a mathematical object that combines the structure of a group with the properties of a
The (multiplication) and inversion map in a Lie group are required to be smooth (infinitely differentiable) functions between the underlying manifolds
Lie groups possess a unique , which acts as a neutral element under the group operation
Each element in a Lie group has a unique inverse with respect to the group operation, allowing for the "undoing" of the operation
Compatibility of group and smooth structures
The group operation in a Lie group is compatible with its smooth manifold structure, ensuring that the result of the operation remains within the group
The smoothness property of the group operation and inversion map allows for the application of differential calculus techniques to study the local structure of Lie groups
The compatibility between the group and smooth structures enables the study of symmetries and continuous transformations in various mathematical and physical contexts
Examples of Lie groups
Matrix Lie groups
The general linear group GL(n,R) consists of all invertible n×n real matrices and forms a Lie group under matrix multiplication
The special linear group SL(n,R) is a subgroup of GL(n,R) consisting of matrices with determinant 1 and is also a Lie group
The orthogonal group [O(n)](https://www.fiveableKeyTerm:o(n)) consists of all n×n orthogonal matrices (matrices A satisfying ATA=I) and forms a Lie group under matrix multiplication
The special orthogonal group SO(n) is a subgroup of O(n) consisting of orthogonal matrices with determinant 1 and is also a Lie group
The unitary group [U(n)](https://www.fiveableKeyTerm:u(n)) consists of all n×n unitary matrices (matrices U satisfying U∗U=I, where U∗ is the conjugate transpose) and forms a Lie group under matrix multiplication
Transformation groups
The of isometries of Rn is a Lie group that describes rigid motions (translations and rotations) in n-dimensional Euclidean space
The is a Lie group of isometries of Minkowski spacetime, which is fundamental in the study of special relativity
The , a combination of translations and Lorentz transformations, is a Lie group that describes the symmetries of spacetime in special relativity
The group of of a smooth manifold, denoted as Diff(M), is an infinite-dimensional Lie group that plays a crucial role in the study of smooth dynamical systems and fluid dynamics
Smoothness in Lie groups
Differentiability of group operations
Smoothness in Lie groups refers to the differentiability of the group multiplication and inversion maps
The group operations in a Lie group are required to be smooth functions between the underlying manifolds, meaning they are infinitely differentiable
The smoothness property allows for the application of differential calculus techniques, such as the computation of derivatives and the study of tangent spaces, to analyze the local structure of Lie groups
Smooth maps between Lie groups
A is a smooth map between two Lie groups that preserves both the group structure and the smooth manifold structure
Lie group homomorphisms are essential in studying the relationships between different Lie groups and their representations
The composition of Lie group homomorphisms is again a Lie group , allowing for the construction of categories of Lie groups and their morphisms
The study of smooth maps between Lie groups leads to the development of the theory of Lie group actions on smooth manifolds, which has applications in , topology, and mathematical physics
Group operations in Lie group theory
Properties of the group operation
The group operation in a Lie group, typically denoted as multiplication, combines two elements of the group to produce a third element within the group
The group operation satisfies the axioms of associativity, meaning that (ab)c=a(bc) for any elements a, b, and c in the Lie group
The group operation is compatible with the smooth structure of the Lie group, ensuring that the result of the operation remains within the group and preserves smoothness
Identity element and inverses
A Lie group possesses a unique identity element, often denoted as e, which acts as a neutral element under the group operation, satisfying ae=ea=a for any element a in the group
Each element in a Lie group has a unique inverse with respect to the group operation, denoted as a−1 for an element a, satisfying aa−1=a−1a=e
The existence of inverses allows for the "undoing" of the group operation and is crucial in the study of symmetries and transformations described by Lie groups
Interplay between group operation and smooth structure
The compatibility between the group operation and the smooth manifold structure is a fundamental aspect of Lie group theory
The group operation and the smooth structure work together to enable the study of continuous symmetries and transformations in various mathematical and physical contexts
The interplay between the group operation and smooth structure gives rise to the notion of infinitesimal generators of a Lie group, which are elements of the associated and describe the local behavior of the group
The , a smooth map from the Lie algebra to the Lie group, connects the infinitesimal generators to the global structure of the group and plays a crucial role in the study of one-parameter subgroups and the representation theory of Lie groups