Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
Interference and Diffraction02:18

Interference and Diffraction

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.
The de Broglie Wavelength02:32

The de Broglie Wavelength

In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
Entropy02:39

Entropy

Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
Carrier Transport01:21

Carrier Transport

The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra. Schrödinger...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Comb Model in Periodic Potential.

Entropy (Basel, Switzerland)·2026
Same author

Shear-driven finite-velocity diffusion and its generalization.

Chaos (Woodbury, N.Y.)·2026
Same author

Subordination approach to Lyapunov exponents in random systems with memory.

Chaos (Woodbury, N.Y.)·2025
Same author

Screening and localization in the nonlinear Anderson problem.

Physical review. E·2025
Same author

Turbulence spreading and anomalous diffusion on combs.

Physical review. E·2025
Same author

Non-Markovian quantum mechanics on comb.

Chaos (Woodbury, N.Y.)·2024

Related Experiment Video

Updated: Jun 14, 2026

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level
06:55

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level

Published on: September 26, 2016

Subdiffusion in the nonlinear Schrödinger equation with disorder.

Alexander Iomin1

  • 1Department of Physics, Technion, Haifa, Israel.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|April 7, 2010
PubMed
Summary

Disordered nonlinear Schrödinger equation dynamics reveal subdiffusive wave packet spreading. A continuous time random walk model explains this phenomenon, yielding a transport exponent of 2/5 for subdiffusion.

Area of Science:

  • Physics
  • Nonlinear Dynamics
  • Condensed Matter Physics

Background:

  • The nonlinear Schrödinger equation (NLSE) models various wave phenomena.
  • Disorder introduces complex behavior in wave packet dynamics.
  • Understanding wave packet spreading is crucial in many physical systems.

Purpose of the Study:

  • To investigate the dynamics of wave packets in a disordered nonlinear Schrödinger equation.
  • To explain the observed subdiffusive spreading mechanism.
  • To develop a probabilistic framework for subdiffusion.

Main Methods:

  • Analysis of the nonlinear Schrödinger equation with disorder.
  • Study of initially localized wave packet evolution.
  • Application of the continuous time random walk (CTRW) model.

More Related Videos

Measurement of Particle Size Distribution in Turbid Solutions by Dynamic Light Scattering Microscopy
09:16

Measurement of Particle Size Distribution in Turbid Solutions by Dynamic Light Scattering Microscopy

Published on: January 9, 2017

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light
09:19

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light

Published on: July 29, 2013

Related Experiment Videos

Last Updated: Jun 14, 2026

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level
06:55

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level

Published on: September 26, 2016

Measurement of Particle Size Distribution in Turbid Solutions by Dynamic Light Scattering Microscopy
09:16

Measurement of Particle Size Distribution in Turbid Solutions by Dynamic Light Scattering Microscopy

Published on: January 9, 2017

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light
09:19

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light

Published on: July 29, 2013

  • Derivation of a probabilistic description for subdiffusion.
  • Main Results:

    • Observed subdiffusive spreading of the wave packet.
    • Successful explanation of subdiffusion using the CTRW framework.
    • Obtained a transport exponent of 2/5 for subdiffusion.
    • Provided a probabilistic model for the spreading dynamics.

    Conclusions:

    • Subdiffusion is a key characteristic of wave packet dynamics in disordered NLSE.
    • The CTRW model effectively describes and predicts this subdiffusive behavior.
    • The derived transport exponent offers a quantitative measure of the spreading process.