DCSQUIDs

A dcSQUID, or direct current superconducting quantum interference device, is a highly sensitive magnetic flux sensor based on a superconducting loop interrupted by two Josephson junctions. The device operates at cryogenic temperatures and is typically biased with a current, producing a voltage that depends on the magnetic flux threading the loop. The combination of superconductivity, quantum interference, and flux quantization makes the dcSQUID capable of detecting extremely small magnetic fields.

The operating principle relies on the Josephson effect and flux quantization in the superconducting loop. The two junctions form a interferometer, so the maximum supercurrent (critical current) of the loop varies periodically with the applied magnetic flux, I_c(Φ) ≈ I0 cos(πΦ/Φ0) for symmetric junctions, where Φ0 = h/2e is the magnetic flux quantum. As the device is biased into the resistive state, the voltage across the loop becomes a periodic function of Φ. With a feedback or flux-locked loop (FLL), the dcSQUID provides a linear, broad-band flux-to-voltage transfer function and excellent sensitivity.

Fabrication typically uses niobium-based superconductors with aluminum-oxide tunnel junctions or other junction technologies; devices are operated in cryostats at a few kelvin or lower. Applications include ultra-sensitive magnetometry for biomagnetism (e.g., magnetoencephalography), geophysical surveys, nondestructive testing, and scanning SQUID microscopy, where a miniature dcSQUID is scanned close to a sample surface to map magnetic fields.

Performance is limited by intrinsic noise, environmental magnetic interference, and amplifier noise. Modern dcSQUIDs achieve very low flux noise and high sensitivity, making them a standard tool in low-temperature physics and applied magnetometry.