effect

flux quantization

The confinement of magnetic flux in quantized units within superconducting structures.
63 related articles · 6 formulas

Description

Flux quantization is a fundamental property of superconductors: the magnetic flux threading a superconducting loop or a vortex can only take discrete values, multiples of the flux quantum Φ₀ = h/2e ≈ 2.07×10⁻¹⁵ webers. This arises because the superconducting state is described by a macroscopic quantum wavefunction, and its phase must be single-valued around any closed path. Flux quantization is the basis for superconducting quantum interference devices (SQUIDs), which are the most sensitive magnetometers known, and it also governs the behavior of magnetic vortices in type-II superconductors.

History

Flux quantization was predicted by Fritz London in 1948 and experimentally confirmed in 1961 by Deaver and Fairbank, and independently by Doll and Näbauer, using thin superconducting cylinders.

How it works

In a superconductor, electrons form Cooper pairs that condense into a single quantum state. The current density is proportional to the gradient of the phase of this wavefunction. Around a loop, the phase change must be a multiple of 2π, which forces the enclosed magnetic flux to be an integer multiple of Φ₀. In type-II superconductors, magnetic field penetrates in the form of vortices, each carrying exactly one flux quantum, surrounded by circulating supercurrents that screen the field elsewhere.

In practice

SQUIDs exploit flux quantization to measure tiny magnetic fields, with applications in medical magnetoencephalography, non-destructive testing, and geophysical surveys.

Fun fact

The flux quantum is exactly h/2e, where the factor 2 reflects the fact that the charge carriers in superconductors are Cooper pairs, not single electrons.

Concept graph →

Formulas

$$\Delta Q = \nu \frac{e \Delta \Phi}{\Phi_0}$$
Charge quantization in superconductors relates flux change to accumulated charge.
What is in the formula
\Delta QvariableAccumulated charge change in the superconductor — electric charge coulomb
\Delta \PhivariableChange in magnetic flux through the superconducting loop — magnetic flux weber
\nuvariableFilling factor (integer or fractional) of the quantum Hall state — dimensionless
econstantMagnitude of the electric charge of a single electron or proton — elementary charge = 1.602176634e-19 coulomb
\Phi_0constantSuperconducting flux quantum, h/(2e), the fundamental unit of magnetic flux in a superconductor — magnetic flux quantum = 2.067833848e-15 weber
δq_{\rma}/e=ν(δ\phi/\phi_0) · 2603.05341
$$\Phi_0 = \frac{h}{2e}$$
The magnetic flux quantum is the fundamental unit of magnetic flux in superconductors.
What is in the formula
Φ_0variableMagnetic flux quantum — magnetic flux weber
hconstantPlanck constant, the fundamental quantum of action — planck constant = 6.62607015e-34 joule second
econstantElementary charge, the magnitude of charge of a single electron — elementary charge = 1.602176634e-19 coulomb
\phi_0=\frac{h}{2e} · 2607.14697
$$ds_E^2 = d\tau^2 + a^2(\tau) d\Omega_3^2$$
Euclidean metric for closed universe with scale factor a(τ).
What is in the formula
ds_EvariableEuclidean line element — line element metre
τvariableEuclidean time coordinate — time second
avariableScale factor of the universe — scale factor
dΩ_3variableLine element on a unit 3-sphere — solid angle element
ds_e^2=dτ^2+a^2(τ)dω_3^2 · 2605.13777v2
$$\sigma_H = \frac{\nu e^2}{h}$$
Hall conductivity quantized in units of e²/h.
What is in the formula
σ_HvariableHall conductivity — electrical conductivity siemens
νvariableFilling factor (integer or fractional) — filling factor
evariableElementary charge — electric charge coulomb
hvariablePlanck constant — planck constant joule second
σ_h=\frac{qq}{2πn} · 2607.10561
$$F_{\text{total}} = \sigma T^4$$
Total flux equals Stefan-Boltzmann radiation.
What is in the formula
F_{\text{total}}variabletotal radiative flux emitted per unit area — radiative flux watt per square metre
Tvariableabsolute temperature of the radiating body — temperature kelvin
\sigmaconstantStefan-Boltzmann constant relating temperature to radiated power — stefan boltzmann constant = 5.670374419e-8 watt per square metre per kelvin to the fourth
f_{\rmrad}+f_{\rmconv}=σ_{\rmsb}t_{\rmeff}^4 · 2607.24141v1
$$\mathbf{F} = -\frac{c}{\kappa \rho} \nabla e_{\text{rad}}$$
Radiation flux in diffusion approximation.
What is in the formula
\mathbf{F}variableRadiation flux vector — radiation flux watt per square metre
\kappavariableOpacity (mass absorption coefficient) — opacity square metre per kilogram
\rhovariableMass density — mass density kilogram per cubic metre
e_{\text{rad}}variableRadiation energy density — energy density joule per cubic metre
cconstantSpeed of light in vacuum — speed of light = 299792458 metre per second
\nablaoperatorSpatial gradient — nabla operator
{f}_{{diff}}=-λ\frac{c}{\kappa_s}\frac{\nablae_{{rad}}}{ρ} · 2607.05508v1

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