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

Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
Sound Waves: Resonance01:14

Sound Waves: Resonance

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...
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:
Damped Oscillations01:07

Damped Oscillations

In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Electric Field at the Surface of a Conductor01:26

Electric Field at the Surface of a Conductor

Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...

You might also read

Related Articles

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

Sort by
Same author

Physical model of neutron scattering by clathrate hydrate and C60hosting paramagnetic oxygen molecules.

Journal of physics. Condensed matter : an Institute of Physics journal·2024
Same author

Insight into the electronic structure of the centrosymmetric skyrmion magnet GdRu<sub>2</sub>Si<sub>2</sub>.

Nanoscale advances·2023
Same author

Long-lived spin waves in a metallic antiferromagnet.

Nature communications·2023
Same author

Dramatic Plasmon Response to the Charge-Density-Wave Gap Development in 1T-TiSe_{2}.

Physical review letters·2022
Same author

SERS of cylindrospermopsin cyanotoxin: Prospects for quantitative analysis in solution and in fish tissue.

Spectrochimica acta. Part A, Molecular and biomolecular spectroscopy·2022
Same author

The role of high-energy phonons in electron-phonon interaction at conducting surfaces with helium-atom scattering.

Physical chemistry chemical physics : PCCP·2022

Related Experiment Video

Updated: Jun 26, 2026

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System
08:19

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System

Published on: May 9, 2021

Large surface charge density oscillations induced by subsurface phonon resonances.

V Chis1, B Hellsing, G Benedek

  • 1Department of Physics, University of Gothenburg, Fysikgården 6B, S-412 96 Göteborg, Sweden.

Physical Review Letters
|December 31, 2008
PubMed
Summary

Subsurface phonon resonances in copper surfaces trigger significant charge density oscillations. This finding explains anomalous helium atom scattering and has implications for electron-phonon interactions at metal surfaces.

More Related Videos

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
10:40

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps
11:45

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps

Published on: August 17, 2017

Related Experiment Videos

Last Updated: Jun 26, 2026

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System
08:19

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System

Published on: May 9, 2021

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
10:40

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps
11:45

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps

Published on: August 17, 2017

Area of Science:

  • Surface Science
  • Condensed Matter Physics
  • Computational Materials Science

Background:

  • Metal surfaces exhibit complex dynamics influenced by atomic vibrations (phonons).
  • Surface charge density (SCD) oscillations are crucial for understanding surface phenomena.
  • Helium atom scattering is a sensitive probe of surface properties.

Purpose of the Study:

  • Investigate the relationship between subsurface phonon resonances and SCD oscillations on the Cu(111) surface.
  • Explain the origin of large helium atom scattering intensities observed at metal surfaces.
  • Explore the implications of phonon-SCD coupling in surface spectroscopy.

Main Methods:

  • Density Functional Perturbation Theory (DFPT) was employed to study surface dynamics.
  • Embedded-atom methods were used for initial prediction of phonon resonances.
  • Theoretical analysis of electron-phonon interactions at the metal surface.

Main Results:

  • Subsurface phonon resonances, specifically the S3 mode, were identified as triggers for large SCD oscillations.
  • The study explains the anomalous longitudinal resonance observed in helium atom scattering intensity.
  • A strong coupling between specific phonons and SCD oscillations was demonstrated.

Conclusions:

  • Subsurface phonon resonances play a critical role in driving SCD oscillations on metal surfaces.
  • The findings provide a theoretical basis for interpreting helium scattering experiments.
  • The demonstrated electron-phonon coupling has significant implications for inelastic electron tunneling spectroscopy and other surface phenomena.