Related Experiment Video
Updated: Jul 11, 2026

11:24
Optimized Fabrication Procedure for High-Quality Graphene-based Moiré Superlattice Devices
Published on: July 11, 2025
Dynamical layer decoupling in a stripe-ordered high-T(c) superconductor.
1Department of Physics, Stanford University, Stanford, California 94305-4060, USA.
Physical Review Letters
|October 13, 2007
Summary
In stripe-ordered electronic systems, superconductivity can arise with a unique wave vector. This leads to vanishing Josephson coupling in specific crystals like La(2-x)Ba(x)CuO(4), explaining observed layer decoupling.
Area of Science:
- Condensed matter physics
- Materials science
- Superconductivity
Background:
- Strongly correlated two-dimensional electronic systems exhibit complex ordered states.
- Stripe order and superconductivity are emergent phenomena in these systems.
- Layered cuprate materials like La(2-x)Ba(x)CuO(4) display intricate electronic behaviors.
Purpose of the Study:
- To investigate the relationship between stripe order and superconductivity in two-dimensional electronic systems.
- To explain the vanishing Josephson coupling in specific layered structures.
- To elucidate the cause of dynamical decoupling observed in transport measurements.
Main Methods:
- Theoretical analysis of superconducting condensate wave vectors.
- Investigation of Josephson coupling in layered materials with specific crystal structures.
- Correlation of theoretical predictions with experimental transport measurements.
Main Results:
- Superconducting condensate can form at a nonzero wave vector, doubling the charge order period.
- Josephson coupling between adjacent planes vanishes identically in systems with specific structures (e.g., La(2-x)Ba(x)CuO(4)).
- This vanishing coupling is proposed as the cause for dynamical decoupling at x = 1/8.
Conclusions:
- The spatial modulation of the superconducting condensate is intrinsically linked to the stripe order.
- Vanishing Josephson coupling provides a mechanism for the observed layer decoupling in certain cuprates.
- This finding offers a new perspective on the interplay between different electronic orders in layered materials.
More Related Videos
Related Concept Videos
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...
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...
Electrostatic Boundary Conditions in Dielectrics
When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's permittivity.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's permittivity.
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...
Dielectric Polarization in a Capacitor
The presence of a dielectric medium in a capacitor not only changes the voltage and capacitance but also affects the electric field. In general, dielectrics can be of two types: polar and nonpolar. In a polar dielectric, the positive and negative charges in the molecules are separated by a distance and hence have a permanent dipole moment. In contrast, no such charge separation exists in a nonpolar dielectric, however the nonpolar molecules get polarized in the presence of an external electric...
Magnetic Field due to Moving Charges
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...

