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...
IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration01:16

IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration

A covalently bonded heteronuclear diatomic molecule can be modeled as two vibrating masses connected by a spring. The vibrational frequency of the bond can be expressed using an equation derived from Hooke's law, which describes how the force applied to stretch or compress a spring is proportional to the displacement of the spring. In this case, the atoms behave like masses, and the bond acts like a spring.
According to Hooke's law, the vibrational frequency is directly proportional to the...
Atomic Force Microscopy01:08

Atomic Force Microscopy

Atomic force microscopy (AFM) is a type of scanning probe microscopy that can analyze topographic details of various specimens like ceramics, glass, polymers, and biological samples. AFM offers over 1000 times more resolution than the optical imaging system. Images generated from AFM are three-dimensional surface profiles, offering an advantage over the flat, two-dimensional images from other imaging techniques.
The AFM Probe
The probe is regarded as the heart of any AFM setup and comprises the...
Interaction of EM Radiation with Matter: Spectroscopy01:12

Interaction of EM Radiation with Matter: Spectroscopy

Electromagnetic (EM) radiation can be considered an oscillating electric and magnetic field propagating through a medium that can interact with matter in its path. The electric field in the radiation can interact with electrical charges in the atoms or molecules in the matter. On the other hand, the magnetic field can interact with the magnetic field in the atomic nucleus. The study of the interaction between electromagnetic radiation and matter is termed spectroscopy. Spectroscopy is the study...
The Bohr Model02:18

The Bohr Model

Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as the nucleus...
X-ray Crystallography02:18

X-ray Crystallography

The size of the unit cell and the arrangement of atoms in a crystal may be determined from measurements of the diffraction of X-rays by the crystal, termed X-ray crystallography.
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...

You might also read

Related Articles

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

Sort by
Same author

Spectral Function of the Chiral One-Dimensional Fermi Liquid in the Regime of Strong Interactions.

Physical review letters·2022
Same author

Quasiparticle Energy Relaxation in a Gas of One-Dimensional Fermions with Coulomb Interaction.

Physical review letters·2021
Same author

Viscous Properties of a Degenerate One-Dimensional Fermi Gas.

Physical review letters·2020
Same author

Structure and antibacterial properties of Ag-doped micropattern surfaces produced by photolithography method.

Colloids and surfaces. B, Biointerfaces·2018
Same author

Hybrid Sound Modes in One-Dimensional Quantum Liquids.

Physical review letters·2018
Same author

Second Sound in Systems of One-Dimensional Fermions.

Physical review letters·2018

Related Experiment Video

Updated: May 16, 2026

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

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

Imaging the electron-phonon interaction at the atomic scale.

Igor Altfeder1, K A Matveev, A A Voevodin

  • 1Nanoelectronic Materials Branch, Air Force Research Laboratory, Wright Patterson AFB, Ohio 45433, USA. Igor.Altfeder.Ctr@wpafb.af.mil

Physical Review Letters
|December 11, 2012
PubMed
Summary
This summary is machine-generated.

Researchers studied electron-phonon coupling in lead (Pb) films on silicon (Si). They found that the coupling strength (λ) depends on how electrons scatter at the interface, revealing insights into metal-insulator interactions.

More Related Videos

Picometer-Precision Atomic Position Tracking through Electron Microscopy
15:04

Picometer-Precision Atomic Position Tracking through Electron Microscopy

Published on: July 3, 2021

Novel Techniques for Observing Structural Dynamics of Photoresponsive Liquid Crystals
10:35

Novel Techniques for Observing Structural Dynamics of Photoresponsive Liquid Crystals

Published on: May 29, 2018

Related Experiment Videos

Last Updated: May 16, 2026

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

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

Picometer-Precision Atomic Position Tracking through Electron Microscopy
15:04

Picometer-Precision Atomic Position Tracking through Electron Microscopy

Published on: July 3, 2021

Novel Techniques for Observing Structural Dynamics of Photoresponsive Liquid Crystals
10:35

Novel Techniques for Observing Structural Dynamics of Photoresponsive Liquid Crystals

Published on: May 29, 2018

Area of Science:

  • Surface science
  • Condensed matter physics
  • Materials science

Background:

  • Investigating electron-phonon interaction is crucial for understanding interfacial phenomena in thin films.
  • Lead (Pb) films on silicon (Si) offer a model system for metal-insulator interface studies.

Purpose of the Study:

  • To directly image and quantify the electron-phonon coupling parameter (λ) at the Pb/Si(111) interface.
  • To elucidate the relationship between interfacial electron scattering and electron-phonon coupling.

Main Methods:

  • Epitaxial growth of thin Pb films on a 7×7 reconstructed Si(111) surface.
  • Utilizing scanning tunneling microscopy (STM) for real-space imaging.
  • Employing inelastic electron tunneling spectroscopy (IETS) to probe electron-phonon coupling.

Main Results:

  • Direct real-space visualization of the electron-phonon coupling parameter (λ).
  • Observed that λ increases with diffuse electron scattering and decreases with specular electron scattering at the Pb/Si(111) interface.
  • Demonstrated that transverse redistribution of electron density within a quantum well drives this effect.

Conclusions:

  • The nature of electron scattering at the metal-insulator interface significantly influences electron-phonon coupling.
  • Understanding interfacial scattering mechanisms is key to controlling electronic properties in thin film systems.
  • This study provides a direct method for characterizing electron-phonon coupling in model systems.