Related Experiment Video
Updated: Apr 27, 2026

10:32
Fabrication of Uniform Nanoscale Cavities via Silicon Direct Wafer Bonding
Published on: January 9, 2014
9.2K
Friedel Oscillations in Nanoconfined ^{4}He.
Bernd Rosenow1, Adrian Del Maestro2,3
1Universität Leipzig, Institut für Theoretische Physik, D-04103, Leipzig, Germany.
Physical Review Letters
|April 25, 2026
Summary
We found Friedel oscillations in one-dimensional bosonic quantum liquids, like helium in nanopores. This scattering phenomenon has observable signatures in elastic scattering and mass transport.
Area of Science:
- Condensed matter physics
- Quantum liquids
- Low-dimensional systems
Background:
- One-dimensional bosonic systems, such as helium-4 confined to nanopores, exhibit Luttinger liquid behavior.
- Collective excitations in these systems manifest as density waves.
Purpose of the Study:
- Investigate the impact of a scattering potential on a low-dimensional quantum liquid.
- Analyze the behavior of helium-4 inside a perturbed nanopore with a localized constriction.
Main Methods:
- Utilized a microscopic model of helium-4 within a perturbed nanopore.
- Employed quantum Monte Carlo simulations.
- Analyzed the density of the core within an effective low-energy framework.
Main Results:
- Revealed the emergence of Friedel oscillations in a bosonic quantum liquid, notably in the absence of a Fermi surface.
- Demonstrated the pinning phenomenon caused by the scattering potential.
Conclusions:
- The Luttinger liquid model predicts observable signatures of the scattering phenomenon.
- These signatures can be detected via elastic scattering measurements.
- Temperature and pressure dependence of mass transport through the deformed nanopore offer further experimental evidence.
Related Concept Videos
Molecular Orbital Theory II
21.6K
Molecular Orbital Energy Diagrams
21.6K
The de Broglie Wavelength
25.6K
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...
25.6K
The Bohr Model
67.7K
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...
67.7K
The Pauli Exclusion Principle
51.6K
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
51.6K
Forced Oscillations
6.3K
When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
6.3K
Oscillations about an Equilibrium Position
5.7K
Stability is an important concept in oscillation. If an equilibrium point is stable, a slight disturbance of an object that is initially at the stable equilibrium point will cause the object to oscillate around that point. For an unstable equilibrium point, if the object is disturbed slightly, it will not return to the equilibrium point. There are three conditions for equilibrium points—stable, unstable, and half-stable. A half-stable equilibrium point is also unstable, but is named so...
5.7K

