A loop of superconducting material that reacts to electric fields, used to detect tiny asymmetries in nuclei.A superconducting loop is a closed circuit made of a superconducting material — a substance that conducts electricity with zero resistance below a critical temperature. These loops are extraordinarily sensitive to magnetic fields and electric fields, making them ideal for detecting tiny asymmetries in atomic nuclei. The loop's behavior is governed by quantum mechanics on a macroscopic scale, where the superconducting current is a coherent quantum state that can interfere with itself, much like light in an interferometer.
The concept of superconducting loops with Josephson junctions was developed in the 1960s, following Brian Josephson's prediction of tunneling in superconductors in 1962. The first SQUID was built by Robert Jaklevic and colleagues in 1964.
When a superconducting loop is exposed to a magnetic field, it generates a persistent current that exactly cancels the field inside the superconductor (the Meissner effect). However, if the loop contains a small 'weak link' — a Josephson junction — the current can tunnel through it, and the loop becomes sensitive to the magnetic flux threading it. This forms the basis of a SQUID (Superconducting Quantum Interference Device), which can measure magnetic fields with exquisite precision. The loop's quantum state is also sensitive to electric fields, which can shift the energy levels of the system, allowing detection of tiny asymmetries in the charge distribution of nuclei.
Superconducting loops are used in SQUID magnetometers for medical imaging (magnetoencephalography), in quantum computing as qubits, and in precision measurements of nuclear properties.
A superconducting loop can maintain a persistent current for years without any power source, as long as it stays below its critical temperature.










