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

Superconductor01:24

Superconductor

A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
Types Of Superconductors01:28

Types Of Superconductors

A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
Network Covalent Solids02:18

Network Covalent Solids

Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

The structure of a crystalline solid, whether a metal or not, is best described by considering its simplest repeating unit, which is referred to as its unit cell. The unit cell consists of lattice points that represent the locations of atoms or ions. The entire structure then consists of this unit cell repeating in three dimensions. The three different types of unit cells present in the cubic lattice are illustrated in Figure 1.
Types of Unit Cells
Imagine taking a large number of identical...
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...
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,...

You might also read

Related Articles

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

Sort by
Same author

Exciton dispersion fine structure and deep ultraviolet optical conductivity of freestanding two-dimensional h-BN.

Nature communications·2026
Same author

Free energy barrier and thermal-quantum behavior of sliding bilayer graphene.

Physical chemistry chemical physics : PCCP·2025
Same author

Infrared markers of topological phase transitions in quantum spin Hall insulators.

npj computational materials·2025
Same author

Excitonic Effects in Phonons: Reshaping the Graphene Kohn Anomalies and Lifetimes.

Physical review letters·2025
Same author

Temperature-invariant crystal-glass heat conduction: From meteorites to refractories.

Proceedings of the National Academy of Sciences of the United States of America·2025
Same author

Interplay of Superconductivity, Ferromagnetism, and Half-Metallicity in Gated Single-Layer g-C<sub>3</sub>N<sub>4</sub>.

The journal of physical chemistry letters·2025

Related Experiment Video

Updated: Jul 2, 2026

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
04:51

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride

Published on: July 8, 2021

High-Tc superconductivity in superhard diamondlike BC5.

Matteo Calandra1, Francesco Mauri

  • 1CNRS and Institut de Minéralogie et de Physique des Milieux condensés, case 115, 4 place Jussieu, 75252, Paris cedex 05, France.

Physical Review Letters
|September 4, 2008
PubMed
Summary

Superhard diamondlike BC5 exhibits superconductivity with a critical temperature comparable to MgB2. This phenomenon is driven by electron-phonon interactions, primarily involving boron and carbon atom vibrations.

More Related Videos

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
05:39

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

Published on: August 2, 2019

Characterization of Ultra-fine Grained and Nanocrystalline Materials Using Transmission Kikuchi Diffraction
09:13

Characterization of Ultra-fine Grained and Nanocrystalline Materials Using Transmission Kikuchi Diffraction

Published on: April 1, 2017

Related Experiment Videos

Last Updated: Jul 2, 2026

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
04:51

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride

Published on: July 8, 2021

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
05:39

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

Published on: August 2, 2019

Characterization of Ultra-fine Grained and Nanocrystalline Materials Using Transmission Kikuchi Diffraction
09:13

Characterization of Ultra-fine Grained and Nanocrystalline Materials Using Transmission Kikuchi Diffraction

Published on: April 1, 2017

Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Solid-State Chemistry

Background:

  • Recent synthesis of superhard diamondlike BC5 presents new avenues for materials research.
  • Understanding the electronic and vibrational properties of novel materials is crucial for discovering new functionalities.

Purpose of the Study:

  • To investigate the superconducting properties of the newly synthesized diamondlike BC5.
  • To determine the key factors contributing to superconductivity in BC5.

Main Methods:

  • Density Functional Theory (DFT) calculations were employed.
  • Analysis of electron-phonon coupling and vibrational properties was performed.

Main Results:

  • BC5 demonstrates superconductivity with a critical temperature similar to that of Magnesium Diboride (MgB2).
  • The calculated average electron-phonon coupling constant (lambda) is 0.89.
  • The phonon-frequency logarithmic average (log) is 67.4 meV, with isotope coefficients alpha(C)=0.3 and alpha(B)=0.2.
  • Superconductivity in BC5 is primarily sustained by the coupled vibrations of boron atoms and their neighboring carbon atoms.

Conclusions:

  • Diamondlike BC5 is a superconductor with properties comparable to established superconducting materials.
  • The electron-phonon interaction, particularly involving B-C vibrations, is the main mechanism behind BC5's superconductivity.