phenomenon

strain induced superconductivity

Superconductivity achieved by applying mechanical strain to materials like graphene or alloys.
46 related articles · 1 formulas

Description

Strain-induced superconductivity is the phenomenon where applying mechanical deformation—stretching, compressing, or twisting—to a material causes it to become superconducting, or enhances its superconducting transition temperature. This is particularly striking in materials that are not superconducting under normal conditions, such as certain forms of graphene or thin films of gold. The strain alters the lattice structure, which in turn modifies the electronic band structure and the strength of electron-phonon coupling, potentially enabling Cooper pair formation.

History

The idea that strain can influence superconductivity dates back to the 1960s, but the modern wave of interest began in the 2010s with theoretical predictions and experimental observations of strain-induced superconductivity in graphene and other two-dimensional materials.

How it works

Mechanical strain changes the distances between atoms and the symmetry of the crystal lattice. This directly affects the electronic bands near the Fermi level: it can increase the density of states at the Fermi energy, enhance the electron-phonon coupling constant, or suppress competing instabilities like charge density waves. In graphene, for example, uniaxial strain can open a band gap or shift the Dirac points, and in specific configurations, it can lead to a superconducting phase. The effect is often highly anisotropic—stretching along one direction may induce superconductivity while compressing along another does not.

In practice

Strain engineering is used to tune the properties of superconducting devices, such as improving the critical current in thin films or creating superconducting regions in otherwise non-superconducting materials for quantum circuits.

Fun fact

In 2023, researchers demonstrated that a single layer of gold, just one atom thick, becomes superconducting when stretched by only a few percent—a property not seen in bulk gold.

Concept graph →

Formulas

$$\dot{E} \propto \rho v^3 R^2$$
Power from ram pressure scales with density and velocity cubed.
What is in the formula
ρvariablemass density of the medium — mass density kilogram per cubic metre
vvariablevelocity of the object relative to the medium — velocity metre per second
Rvariablecharacteristic radius of the object — radius metre
E_dotvariablepower (energy per unit time) from ram pressure — power watt
\dot{e}_{{in}}=πr_{\star}^2ρv_{\star}δu\approx5.6*10^{42}{эрг/с}(\frac{v_{\star}}{0.1c})^3(\frac{ρ}{3.6*10^{-8}{г/см}^3})(\frac{r_{\star}}{r_{\odot}})^2 · 2607.05508v1

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