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Related Concept Videos

Hyperbolas01:30

Hyperbolas

A hyperbola is a conic section produced when a double-napped cone is intersected by a plane at an angle steeper than the slope of the cone, such that it cuts through both nappes. This intersection yields two separate, mirror-image curves known as branches, which open away from each other along the transverse axis. The nearest points on each branch to the hyperbola’s center are termed vertices, and the distance from the center to a vertex is denoted by a. Perpendicular to the transverse axis is...
Hyperbolic and Inverse Hyperbolic Functions: Problem Solving01:30

Hyperbolic and Inverse Hyperbolic Functions: Problem Solving

An arched gate can be effectively modeled using a hyperbolic cosine profile because this type of function is smooth and symmetric about the vertical axis. When the arch is centered at the origin, its maximum height occurs at the center point. This symmetry ensures that any height below the crown of the arch is reached at two horizontal positions that are equal in distance from the centerline but lie on opposite sides.To determine where the gate reaches a height of five meters, the height of the...
Hyperbolic Functions01:26

Hyperbolic Functions

A flexible cable suspended between two points at the same height naturally forms a curve known as a catenary. This shape results from the balance between the cable’s weight and the tension acting along its length, representing a state of mechanical equilibrium. Unlike simpler approximations, the true shape of a hanging cable is described using hyperbolic functions.Hyperbolic functions are closely related to exponential functions and are named for their connection to the geometry of the...
Geometry of Hyperbolas01:30

Geometry of Hyperbolas

A hyperbola consists of all points where the absolute difference of distances to two fixed points, called foci, remains constant. The standard equation isEach branch extends infinitely and approaches two asymptotes, which guide the curve’s behavior. The parameters a and b define key features: a measures the distance from the center to each vertex along the transverse axis, while b influences the slopes of the asymptotes. The asymptotes have equationsA rectangle centered at the origin with...
Polar Curves01:19

Polar Curves

The spirograph is a versatile tool for visualizing the relationship between geometry and mathematical representation. In particular, it demonstrates how polar coordinates offer an alternative framework for describing curves in comparison to Cartesian coordinates. Instead of specifying a point by its horizontal and vertical displacements (x, y), polar coordinates use a radius r, the distance from the origin, and an angle θ, measured counterclockwise from the polar axis. This system is...
Inverse Hyperbolic Functions and Their Derivatives01:25

Inverse Hyperbolic Functions and Their Derivatives

The shape of a suspension bridge cable hanging under its own weight is described by a catenary curve, which is modeled using the hyperbolic cosine function. This mathematical model accurately captures the balance between gravity and tension acting along the cable. When a particular vertical position on the cable is known, the corresponding horizontal position can be determined using the inverse hyperbolic cosine function, allowing for a detailed analysis of the cable's geometry.Inverse...

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Demonstration of a Hyperlens-integrated Microscope and Super-resolution Imaging
10:01

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Published on: September 8, 2017

Experimental demonstration of hyperbolic patterns.

Stanis Kolpakov1, Adolfo Esteban-Martín, Fernando Silva

  • 1Departament d'Optica, Universitat de València, Dr. Moliner 50, 46100 Burjassot, Spain.

Physical Review Letters
|December 31, 2008
PubMed
Summary
This summary is machine-generated.

Researchers experimentally observed novel hyperbolic patterns in nonlinear optical resonators. These 2D dissipative structures differ from typical elliptic patterns by mode distribution along hyperbolas, not rings.

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Area of Science:

  • Nonlinear optics
  • Dissipative systems
  • Pattern formation

Background:

  • Nonlinear optical resonators can exhibit complex transverse patterns.
  • Existing patterns, like elliptic ones, show mode distributions along rings in the wave-vector domain.
  • Understanding new pattern types can reveal fundamental physics of light-matter interaction.

Purpose of the Study:

  • To experimentally demonstrate the existence of hyperbolic patterns in a nonlinear optical resonator.
  • To characterize these hyperbolic patterns as a new class of 2D dissipative structures.
  • To theoretically investigate these patterns using Swift-Hohenberg models.

Main Methods:

  • Utilizing a nonlinear optical resonator.
  • Manipulating intra-cavity diffraction using cylindrical lenses to induce hyperbolic patterns.
  • Theoretical analysis employing Swift-Hohenberg models.

Main Results:

  • Experimental evidence of hyperbolic transverse patterns was obtained.
  • These patterns exhibit active mode distributions along hyperbolas in the transverse wave-vector space.
  • Theoretical models confirm the formation of hyperbolic patterns under specific conditions.

Conclusions:

  • Hyperbolic patterns represent a novel type of 2D dissipative structure in nonlinear optics.
  • The formation of these patterns is controllable via manipulation of diffraction.
  • This discovery opens new avenues for studying pattern formation in nonlinear systems.