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...
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...
Equipotential Surfaces and Conductors01:16

Equipotential Surfaces and Conductors

For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic situation, if a...
Ferromagnetism01:31

Ferromagnetism

Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...

You might also read

Related Articles

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

Sort by
Same author

Planar thermal Hall effect from phonons in a Kitaev candidate material.

Nature communications·2024
Same author

Reconciling scaling of the optical conductivity of cuprate superconductors with Planckian resistivity and specific heat.

Nature communications·2023
Same author

Large phonon thermal Hall conductivity in the antiferromagnetic insulator Cu<sub>3</sub>TeO<sub>6</sub>.

Proceedings of the National Academy of Sciences of the United States of America·2022
Same author

Linear-in temperature resistivity from an isotropic Planckian scattering rate.

Nature·2021
Same author

Thermal Hall conductivity in the cuprate Mott insulators Nd<sub>2</sub>CuO<sub>4</sub> and Sr<sub>2</sub>CuO<sub>2</sub>Cl<sub>2</sub>.

Nature communications·2020
Same author

Pseudogap phase of cuprate superconductors confined by Fermi surface topology.

Nature communications·2017

Related Experiment Video

Updated: May 30, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

Fermi surface reconstruction in high-T(c) superconductors.

Louis Taillefer1

  • 1Canadian Institute for Advanced Research, Regroupement Québécois sur les Matériaux de Pointe, Département de Physique, Université de Sherbrooke, Sherbrooke, Canada.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|August 10, 2011
PubMed
Summary

Stripe order in cuprates reconstructs the Fermi surface, creating electron pockets. This quantum critical behavior explains transport anomalies and pseudogap phenomena in high-temperature superconductors.

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

Optimized Fabrication Procedure for High-Quality Graphene-based Moir&#233; Superlattice Devices
11:24

Optimized Fabrication Procedure for High-Quality Graphene-based Moiré Superlattice Devices

Published on: July 11, 2025

Related Experiment Videos

Last Updated: May 30, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

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

Optimized Fabrication Procedure for High-Quality Graphene-based Moir&#233; Superlattice Devices
11:24

Optimized Fabrication Procedure for High-Quality Graphene-based Moiré Superlattice Devices

Published on: July 11, 2025

Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Quantum Materials

Background:

  • High-temperature superconductors (cuprates) exhibit complex electronic behavior.
  • Underdoped cuprates show quantum oscillations and negative Hall coefficients, indicating an electron pocket in their Fermi surface.
  • This suggests a Fermi surface reconstruction from the overdoped regime.

Purpose of the Study:

  • To investigate the role of stripe order in Fermi surface reconstruction in hole-doped cuprates.
  • To identify the critical doping concentration for this reconstruction.
  • To analyze the transport properties at this critical doping.

Main Methods:

  • Analysis of quantum oscillation data.
  • Examination of Hall coefficient measurements.
  • Theoretical consideration of stripe order (charge/spin modulation).
  • Identification of critical doping levels.
  • Analysis of temperature dependence of transport coefficients.

Main Results:

  • Quantum oscillations and negative Hall coefficient reveal an electron pocket in underdoped cuprates.
  • Stripe order is identified as the cause of Fermi surface reconstruction.
  • The critical doping for reconstruction is identified.
  • Transport coefficients at critical doping resemble those of metals at a quantum critical point.
  • The pseudogap phase may be a precursor to stripe order.

Conclusions:

  • Stripe order drives Fermi surface reconstruction in hole-doped cuprates.
  • This reconstruction is linked to quantum critical behavior.
  • The pseudogap phase is potentially related to fluctuating stripe order.