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

Van der Waals Interactions01:24

Van der Waals Interactions

Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.Polar molecules have a partial positive charge on one end and a partial negative charge on the other end of the molecule,...
Bonding in Metals02:32

Bonding in Metals

Metallic bonds are formed between two metal atoms. A simplified model to describe metallic bonding has been developed by Paul Drüde called the “Electron Sea Model”.
Magnetic Field Due To A Thin Straight Wire01:27

Magnetic Field Due To A Thin Straight Wire

Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
The Electrical Double Layer01:30

The Electrical Double Layer

In the region where two bulk phases meet, an intricate electric charge distribution arises due to charge transfer, ion adsorption, molecular orientation, and charge distortion. This complex distribution is commonly referred to as the electrical double layer.When a solid electrode interfaces with ions in an electrolyte solution, the speed of electron transfer dictates the rates of oxidation and reduction. The electrode acquires a charge through the escape of atoms into the solution as cations or...
Metallic Solids02:37

Metallic Solids

Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability. Many...

You might also read

Related Articles

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

Sort by
Same author

Discovering Quantum Phase Transitions with Fermionic Neural Networks.

Physical review letters·2023
Same author

Quantum Monte Carlo Study of Positron Lifetimes in Solids.

Physical review letters·2022
Same author

Quasiparticle Effective Mass of the Three-Dimensional Fermi Liquid by Quantum Monte Carlo.

Physical review letters·2021
Same author

Variational and diffusion quantum Monte Carlo calculations with the CASINO code.

The Journal of chemical physics·2020
Same author

Shape and energy consistent pseudopotentials for correlated electron systems.

The Journal of chemical physics·2017
Same author

Quasiparticle and excitonic gaps of one-dimensional carbon chains.

Physical chemistry chemical physics : PCCP·2016

Related Experiment Video

Updated: Jul 10, 2026

Fabricating van der Waals Heterostructures with Precise Rotational Alignment
09:25

Fabricating van der Waals Heterostructures with Precise Rotational Alignment

Published on: July 5, 2019

van der Waals interactions between thin metallic wires and layers.

N D Drummond1, R J Needs

  • 1TCM Group, Cavendish Laboratory, University of Cambridge, Cambridge CB3 0HE, United Kingdom.

Physical Review Letters
|November 13, 2007
PubMed
Summary

Quantum Monte Carlo methods provide accurate binding energies for metallic wires and layers. These results differ significantly from random phase approximation, especially at low densities.

More Related Videos

Residue-Free Fabrication of van der Waals Heterostructures of Two-Dimensional Materials
04:57

Residue-Free Fabrication of van der Waals Heterostructures of Two-Dimensional Materials

Published on: July 18, 2025

Evaluating Plasmonic Transport in Current-carrying Silver Nanowires
09:00

Evaluating Plasmonic Transport in Current-carrying Silver Nanowires

Published on: December 11, 2013

Related Experiment Videos

Last Updated: Jul 10, 2026

Fabricating van der Waals Heterostructures with Precise Rotational Alignment
09:25

Fabricating van der Waals Heterostructures with Precise Rotational Alignment

Published on: July 5, 2019

Residue-Free Fabrication of van der Waals Heterostructures of Two-Dimensional Materials
04:57

Residue-Free Fabrication of van der Waals Heterostructures of Two-Dimensional Materials

Published on: July 18, 2025

Evaluating Plasmonic Transport in Current-carrying Silver Nanowires
09:00

Evaluating Plasmonic Transport in Current-carrying Silver Nanowires

Published on: December 11, 2013

Area of Science:

  • Condensed matter physics
  • Quantum chemistry
  • Computational physics

Background:

  • Accurate calculation of binding energies is crucial for understanding material properties.
  • Homogeneous electron gas models (1D and 2D) are used to simulate metallic systems.
  • Previous studies often rely on approximations like the random phase approximation.

Purpose of the Study:

  • To obtain accurate binding-energy data for parallel metallic wires and layers using Quantum Monte Carlo (QMC) methods.
  • To compare QMC results with those from the random phase approximation (RPA).
  • To investigate the pair-correlation functions in these metallic systems.

Main Methods:

  • Utilizing Quantum Monte Carlo (QMC) methods for high-accuracy energy calculations.
  • Modeling systems as one-dimensional (1D) and two-dimensional (2D) homogeneous electron gases.
  • Calculating pair-correlation functions for biwire and bilayer configurations.

Main Results:

  • QMC methods yielded accurate binding energies for metallic biwires and bilayers.
  • Significant quantitative differences were observed between QMC and RPA binding energies.
  • Disagreement in asymptotic behavior at low densities was found between QMC and RPA for bilayers.
  • Pair-correlation functions were calculated for the first time for these systems.

Conclusions:

  • QMC provides a more accurate description of binding energies compared to RPA for these systems.
  • The findings highlight limitations of RPA, particularly at low electron densities.
  • The calculated QMC data can serve as a benchmark for developing and testing van der Waals energy functionals.