Nadirashvili surface
The Nadirashvili surface is a notable example of a minimal surface, which is a surface that locally minimizes area. More specifically, it is a type of mathematical surface that is defined in terms of its geometric properties and is studied in differential geometry. The Nadirashvili surface is particularly interesting due to its unique characteristics: it is a complete minimal surface that has finitely many singular points, yet it is not embedded, meaning that it intersects itself.
Natural bundle
In mathematics, particularly in differential geometry and theoretical physics, a **natural bundle** refers to a type of fiber bundle that has certain structures and properties derived from a manifold in a way that is "natural" or invariant under changes of coordinate systems.
Natural pseudodistance
Natural pseudodistance is a concept used in mathematical biology and ecology, particularly in the study of population genetics and evolutionary theory. It is typically used to quantify the genetic differences or relationships between populations or individuals based on genetic data. In general, a pseudodistance is a metric that measures how "far apart" two entities are within a particular space or context, but it may not fulfill all the properties of a true distance metric (such as the triangle inequality).
Nearly Kähler manifold
A Nearly Kähler manifold is a specific type of almost Kähler manifold, which is a manifold equipped with a Riemannian metric and a compatible almost complex structure. More formally, if \( M \) is a manifold, it is said to be nearly Kähler if it possesses the following structures: 1. **Riemannian Metric**: A Riemannian metric \( g \) on \( M \), which provides a way to measure distances and angles.
Negative pedal curve
A negative pedal curve is a type of curve in mathematics, specifically in the context of polar coordinates. In polar coordinates, a point is represented by its distance from the origin and the angle it makes with a reference direction. The concept of pedal curves relates to how a point moves along a given curve (called the base curve) while maintaining a specific distance from that curve, typically along a line that is perpendicular (normal) to the base curve.
Neovius surface
The Neovius surface refers to a specific type of mathematical surface that has properties useful in the study of differential geometry and topology. It is named after the Finnish mathematician A.F. Neovius, who studied the surface and its properties. The Neovius surface is typically characterized by its complex structure, including features like cusps and self-intersections, making it interesting from the perspectives of both geometry and mathematical physics.
Noncommutative geometry
Noncommutative geometry is a branch of mathematics that generalizes geometric concepts to settings where the usual notion of points, coordinates, and commutativity does not apply. In traditional geometry, the coordinates of spaces are commutative—meaning the order of multiplication does not affect the result. However, in noncommutative geometry, the coordinates do not necessarily commute, which leads to a richer and more complex structure.
Nonholonomic system
A nonholonomic system refers to a type of dynamical system that is subject to constraints which are not integrable, meaning that the constraints cannot be expressed purely in terms of the coordinates and time. These constraints typically involve the velocities of the system, leading to a situation where the motion cannot be fully described by a potential function alone.
A nonlinear partial differential equation (PDE) is a type of equation that relates a function of multiple variables to its partial derivatives, where the relationship involves nonlinear terms. In contrast to linear PDEs, where the solution can be combined using superposition due to linearity, nonlinear PDEs can exhibit more complex behavior and often require different analytical and numerical methods for their solution.
Nonmetricity tensor
The nonmetricity tensor is a mathematical object used in the context of a generalization of the theory of gravity, particularly in modifications of general relativity, such as in theories of metric-affine geometry. In differential geometry, the notion of nonmetricity is concerned with the way lengths and angles change under parallel transport. In the context of a connection on a manifold, the nonmetricity tensor is defined as the tensor that measures the failure of the connection to preserve the metric tensor during parallel transport.
Normal bundle
In differential geometry, the **normal bundle** is a specific construction associated with an embedded submanifold of a differentiable manifold. It provides a way to understand how the submanifold sits inside the ambient manifold by considering directions that are orthogonal (normal) to the submanifold. ### Definition Let \( M \) be a smooth manifold, and let \( N \subset M \) be a smooth embedded submanifold.
Novikov–Shubin invariant
The Novikov–Shubin invariants are a set of topological invariants associated with certain types of elliptic operators, particularly in the context of non-compact manifolds or manifolds with boundaries. They arise in the study of the heat equation and index theory, particularly in connection with the theory of elliptic partial differential operators and noncommutative geometry. These invariants can be thought of as a generalization of classical numerical invariants associated with the index of elliptic operators.
Osculating circle
An osculating circle is a circle that best approximates a curve at a given point. It is defined as the circle that has the same tangent and curvature as the curve at that point. In other words, the osculating circle touches the curve at that point and shares the same slope and curvature in a local neighborhood around that point.
Osculating plane
In differential geometry, the **osculating plane** is a concept related to curves in three-dimensional space. Specifically, the osculating plane at a given point on a curve is the plane that best approximates the curve near that point. The osculating plane can be defined using the following components: 1. **Tangent Vector**: At any point on a smooth curve, the tangent vector represents the direction in which the curve is moving.
Paneitz operator
The Paneitz operator is a mathematical object that arises in the context of differential geometry, particularly in the study of Riemannian manifolds and the analysis of conformal geometry. Named after the mathematician S. Paneitz, the operator is a fourth-order differential operator defined on a Riemannian manifold.
Parabolic geometry is a branch of differential geometry that studies geometric structures that are modeled on a special class of homogeneous spaces known as parabolic geometries. These structures relate to the study of certain types of manifolds and their associated symmetries, particularly those that arise from a specific class of Lie groups and their actions. ### Key Features of Parabolic Geometry: 1. **Parabolic Structures**: Parabolic geometries are associated with parabolic subalgebras of Lie algebras.
Parallel curve
A parallel curve is a concept used in geometry and differential geometry. It involves the creation of a new curve that maintains a constant distance from a given original curve at all points. This new curve can be thought of as being "offset" from the original curve by a specific distance, which can be positive (creating a curve that is outward from the original) or negative (creating a curve that is inward).
Parallelization (mathematics)
In mathematics, particularly in the context of computation and numerical methods, "parallelization" refers to the process of dividing a problem into smaller, independent sub-problems that can be solved simultaneously across multiple processors or computing units. This approach is used to improve computational efficiency and reduce the time required to obtain results. ### Key Concepts of Parallelization in Mathematics: 1. **Decomposition**: The original problem is broken down into smaller tasks.
Pedal curve
A pedal curve is a type of curve in mathematics that is generated from a given curve known as the "directrix" and a fixed point called the "pedal point" or "focus." The pedal curve is formed by tracing the perpendiculars from the pedal point to the tangents of the directrix.
Petrov classification
The Petrov classification is a system used to categorize solutions to the Einstein field equations in general relativity based on the properties of their curvature tensors, specifically the Riemann curvature tensor. It is named after the Russian physicist A. Z. Petrov, who introduced it in the 1950s. The classification divides spacetimes into different types based on the algebraic properties of the Riemann tensor.