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Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
Modes of Standing Waves - I01:03

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A close look at earthquakes provides evidence for the conditions appropriate for resonance, standing waves, and constructive and destructive interference. A building may vibrate for several seconds with a driving frequency matching the building's natural frequency of vibration; this produces a resonance that results in one building collapsing while the neighboring buildings do not. Often, buildings of a certain height are devastated, while other taller buildings remain intact. This phenomenon...
Modes of Standing Waves: II01:04

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The starting point for expressing the modes of standing waves is understanding the boundary conditions that the waves must follow. The boundary conditions are derived from the physical understanding of how the standing waves are sustained, that is, how the vibrating particles of the medium behave at the boundaries imposed on them.
For a tube open at one end and closed at the other filled with air, the modes are such that there is always an antinode at the open end and a node at the closed end.
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The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in the...
Interference and Diffraction02:18

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Interference is a characteristic phenomenon exhibited by waves. When two electromagnetic waves interact with their peaks and troughs coinciding, a resulting wave with enhanced amplitude is produced. This is known as constructive interference. In this case, the two waves interacting are in phase with each other.
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Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...

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Related Experiment Video

Updated: Jun 19, 2026

Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators
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Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators

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Conical third-harmonic generation in normally dispersive media.

Virgilijus Vaicaitis1, Vygandas Jarutis, Dionysios Pentaris

  • 1Laser Research Center, Vilnius University, Sauletekio 10, Vilnius LT-10223, Lithuania. virgilijus.vaicaitis@ff.vu.lt

Physical Review Letters
|October 2, 2009
PubMed
Summary

Third harmonic generation in normally dispersive media under tight-focusing occurs via six-wave mixing, not third-order frequency tripling. This study explores the resulting complex beam patterns and validates findings with sodium nonlinear susceptibility simulations.

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Area of Science:

  • Nonlinear optics
  • Quantum optics
  • Laser physics

Background:

  • Third harmonic generation (THG) is typically a third-order nonlinear optical process.
  • Tight-focusing conditions can alter nonlinear optical phenomena.
  • Understanding nonlinear interactions is crucial for laser technology and material science.

Purpose of the Study:

  • To investigate the mechanism of third harmonic generation under tight-focusing in normally dispersive media.
  • To analyze the far-field patterns of the generated third harmonic.
  • To compare theoretical models with experimental results for nonlinear susceptibilities.

Main Methods:

  • Theoretical modeling of nonlinear optical processes.
  • Experimental investigation of third harmonic generation.
  • Numerical simulations of wave mixing and beam propagation.
  • Characterization of nonlinear susceptibilities (third- and fifth-order) in sodium.

Main Results:

  • Third harmonic generation is predominantly driven by six-wave mixing, not third-order frequency tripling, under the studied conditions.
  • The far-field pattern of the third harmonic typically forms an axially symmetric ring.
  • Complex beam patterns can emerge under specific mismatch and focusing conditions.
  • Simulations align qualitatively with experimental data for sodium's nonlinear susceptibilities.

Conclusions:

  • Six-wave mixing is the dominant mechanism for third harmonic generation in normally dispersive media with tight focusing.
  • The study provides a more accurate model for THG under these specific conditions.
  • Experimental validation confirms the theoretical predictions and highlights the role of nonlinear susceptibilities.