Equivariant index theorem 1970-01-01
The Equivariant Index Theorem is a significant result in mathematics that generalizes the classical index theorem in the context of equivariant topology, particularly in the presence of group actions. It relates the index of an elliptic differential operator on a manifold equipped with a group action to topological invariants associated with the manifold and the group.
Essential manifold 1970-01-01
An **essential manifold** is a concept used in topology and differential geometry, particularly in the study of manifolds and their embeddings. While the term may not have a universally accepted definition, it generally refers to certain properties of manifolds that distinguish them from other types of topological spaces. In broader terms, a manifold is a topological space that locally resembles Euclidean space and is characterized by its dimensional structure.
Euler characteristic of an orbifold 1970-01-01
The Euler characteristic of an orbifold is a generalization of the concept of the Euler characteristic of a manifold, adapted to account for the singularities and local symmetries present in orbifolds. An orbifold can be thought of as a space that locally looks like a quotient of a Euclidean space by a finite group of symmetries.
Evolute 1970-01-01
"Evolute" can refer to different concepts depending on the context. Here are a few possibilities: 1. **Mathematics**: In mathematics, particularly in differential geometry, an evolute is the locus of the centers of curvature of a given curve. It captures the idea of how the curvature of the original curve behaves and represents the "envelope" of the normals to that curve. 2. **Business/Technology**: Evolute may refer to companies or products that carry the name.
Exponential map (Riemannian geometry) 1970-01-01
In Riemannian geometry, the exponential map is a crucial concept that connects the local geometric properties of a Riemannian manifold to its global structure. Specifically, it describes how to move along geodesics (the generalization of straight lines to curved spaces) starting from a given point on the manifold.
Exterior covariant derivative 1970-01-01
The exterior covariant derivative is a concept that arises in differential geometry, particularly in the context of differential forms on a manifold. It generalizes the idea of a standard exterior derivative, which is a way to differentiate differential forms, by incorporating the notion of a connection (or a covariant derivative) to account for possible curvature in the underlying manifold. ### Key Concepts: 1. **Differential Forms**: - Differential forms are objects in a manifold that can be integrated over submanifolds.
Fibered manifold 1970-01-01
A fibered manifold is a type of manifold that is structured in such a way that it can be viewed as a "fiber bundle" over another manifold. More formally, a fibered manifold can be described in terms of a fibration, which is a particular kind of mapping between manifolds. To clarify, let’s break down the concept: 1. **Base Manifold**: A manifold \( B \) that serves as the "base" space for the fibration.
Filling area conjecture 1970-01-01
The Filling Area Conjecture is a concept from the field of geometric topology, particularly in the study of three-dimensional manifolds. It concerns the relationship between the topological properties of a surface and its geometric properties, specifically focusing on the area of certain types of surfaces. The conjecture originates from the study of isotopy classes of simple curves on surfaces.
Filling radius 1970-01-01
Filling radius is a concept in the field of mathematics, particularly in metric spaces and topology. It is often associated with the properties of sets, particularly in the context of potential theory, geometric measure theory, or dynamical systems. The filling radius of a set can be thought of as a measure of how "thick" or "full" a set is.
Finsler manifold 1970-01-01
A **Finsler manifold** is a generalization of a Riemannian manifold that allows for the length of tangent vectors to be defined in a more flexible way. While Riemannian geometry is based on a positive-definite inner product that varies smoothly from point to point, Finsler geometry introduces a more general function, referred to as the **Finsler metric**, which defines the length of tangent vectors.
First fundamental form 1970-01-01
The First Fundamental Form is a mathematical concept in differential geometry, which provides a way to measure distances and angles on a surface. It essentially encodes the geometric properties of a surface in terms of its intrinsic metrics. For a surface described by a parametric representation, the First Fundamental Form can be constructed from the parameters of that representation.
Flat map 1970-01-01
Frankel conjecture 1970-01-01
The Frankel conjecture is a hypothesis in differential geometry, specifically related to the topology of certain kinds of manifolds. It was proposed by Theodore Frankel in the 1950s and pertains to Kähler manifolds, which are complex manifolds that have a hermitian metric whose imaginary part is a closed differential form. The conjecture states that if a Kähler manifold has a Kähler class that is ample, then any morphism from the manifold to a projective space is surjective.
Frenet–Serret formulas 1970-01-01
The Frenet–Serret formulas are a set of differential equations that describe the intrinsic geometry of a space curve in three-dimensional space. They provide a way to relate the curvature and torsion of a curve to the behavior of its tangent vector, normal vector, and binormal vector. The formulas are fundamental in the study of curves in differential geometry and are named after the mathematicians Jean Frédéric Frenet and Joseph Alain Serret.
Frölicher–Nijenhuis bracket 1970-01-01
The Frölicher–Nijenhuis bracket is a mathematical construct that comes from the field of differential geometry and differential algebra. It is a generalization of the Lie bracket, which is typically defined for vector fields. The Frölicher–Nijenhuis bracket allows us to define a bracket operation for arbitrary differential forms and multilinear maps.
G-fibration 1970-01-01
A **G-fibration** is a concept in the field of algebraic topology, particularly in relation to homotopy theory and the study of fiber spaces. It is a generalization of the notion of a fibration, and it is typically associated with certain kinds of structured spaces and diagrams. In a broad sense, a G-fibration is a fibration where the fibers are not just sets but are equipped with a group action, typically from a topological group \( G \).
G-structure on a manifold 1970-01-01
In differential geometry, a \( G \)-structure on a manifold is a mathematical framework that generalizes the structure of a manifold by introducing additional geometric or algebraic properties. More specifically, a \( G \)-structure allows you to define a way to "view" or "furnish" the manifold with additional structure that can be treated similarly to how one treats vector spaces or tangent spaces.
G2-structure 1970-01-01
A G2-structure is a mathematical concept within the field of differential geometry, particularly in the study of special types of manifolds. More specifically, G2-structures are related to the notion of "exceptional" symmetries and are associated with the G2 group, which is one of the five exceptional Lie groups.
G2 manifold 1970-01-01
A \( G_2 \) manifold is a specific type of differentiable manifold that admits a particular geometric structure characterized by a special kind of 3-form, which leads to a unique relationship between its differential geometry and algebraic topology. More technically, \( G_2 \) can be understood in the context of the theory of connections and holonomy groups.
Gauge covariant derivative 1970-01-01
The gauge covariant derivative is a fundamental concept in the framework of gauge theories, which are essential for describing fundamental interactions in particle physics, most notably in the Standard Model. It is a modification of the ordinary derivative that accounts for the presence of gauge symmetry and the associated gauge fields. ### Definition and Purpose In a gauge theory, the fundamental fields are often associated with certain symmetry groups, such as U(1) for electromagnetism or SU(2) for weak interactions.