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

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...
Propagation of Waves01:07

Propagation of Waves

When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
Propagation Speed of Electromagnetic Waves01:30

Propagation Speed of Electromagnetic Waves

Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
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:
Types of Responses of Series RLC Circuits01:11

Types of Responses of Series RLC Circuits

A second-order differential equation characterizes a source-free series RLC circuit, marking its distinct mathematical representation. The complete solution of this equation is a blend of two unique solutions, each linked to the circuit's roots expressed in terms of the damping factor and resonant frequency.
Types of Damping01:20

Types of Damping

If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...

You might also read

Related Articles

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

Sort by
Same author

Thermodynamic constraints and pseudotransition behavior in a one-dimensional waterlike system.

Physical review. E·2025
Same author

Thermodynamics and inhomogeneous hole distribution in an exactly solvable model of a randomly decorated CuO spin ladder.

Physical review. E·2025
Same author

Unusual low-temperature behavior in the half-filled band of the one-dimensional extended Hubbard model in atomic limit.

Physical review. E·2024
Same author

Crossing the Rift valley: using complete mitogenomes to infer the diversification and biogeographic history of ethiopian highlands <i>Ptychadena</i> (anura: Ptychadenidae).

Frontiers in genetics·2023
Same author

Formation of topological defects in nematic shells with a dumbbell-like shape.

Soft matter·2022
Same author

Universal dynamical scaling laws in three-state quantum walks.

Physical review. E·2021

Related Experiment Video

Updated: Jun 19, 2026

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
07:42

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

Published on: December 15, 2021

Wave-packet dynamics in chains with delayed electronic nonlinear response.

F A B F de Moura1, Iram Gléria, I F dos Santos

  • 1Instituto de Física, Universidade Federal de Alagoas, Maceió AL 57072-970, Brazil.

Physical Review Letters
|October 2, 2009
PubMed
Summary
This summary is machine-generated.

We investigated electron wave packet dynamics with nonadiabatic electron-phonon interactions. We found that self-trapping requires weaker nonlinearity for short delays but stronger nonlinearities in slowly responding media.

More Related Videos

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

Related Experiment Videos

Last Updated: Jun 19, 2026

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
07:42

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

Published on: December 15, 2021

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

Area of Science:

  • Condensed Matter Physics
  • Quantum Mechanics
  • Nonlinear Dynamics

Background:

  • Electron-phonon interactions are crucial in determining material properties.
  • Nonadiabatic effects can significantly alter electron dynamics.
  • Self-trapping is a key phenomenon in nonlinear systems.

Purpose of the Study:

  • To investigate the dynamics of a single electron wave packet in a chain with nonadiabatic electron-phonon coupling.
  • To analyze the influence of delayed nonlinear responses on self-trapping.
  • To explore the conditions leading to self-trapping under varying nonlinearity and delay times.

Main Methods:

  • Solving the time-dependent Schrödinger equation.
  • Modeling electron-phonon coupling via delayed cubic nonlinearity.
  • Analyzing the phase diagram of self-trapping.

Main Results:

  • Self-trapping occurs when nonlinearity exceeds a critical value in the adiabatic limit.
  • Shorter delay times reduce the nonlinearity threshold for self-trapping.
  • Slow nonlinear responses lead to a reentrant phase diagram, requiring stronger nonlinearities for self-trapping.

Conclusions:

  • The interplay between nonlinearity, delay time, and response speed dictates self-trapping behavior.
  • Nonadiabatic electron-phonon interactions introduce complex dynamics not present in adiabatic models.
  • Understanding these dynamics is essential for designing materials with specific electronic properties.