instrument

superconducting loop

A loop of superconducting material that reacts to electric fields, used to detect tiny asymmetries in nuclei.
25 related articles

Description

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.

History

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.

How it works

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.

In practice

Superconducting loops are used in SQUID magnetometers for medical imaging (magnetoencephalography), in quantum computing as qubits, and in precision measurements of nuclear properties.

Fun fact

A superconducting loop can maintain a persistent current for years without any power source, as long as it stays below its critical temperature.

Concept graph →

Related articles · 25

Superconductivity2026-08-211 minarXiv:2608.21273express
An Alloy That Won't Give In to Magnetism
A metal made of five different atoms is like a soup with bits of carrot, peas, potato, onion, and meat floating in it. Each bit is its own element: chromium, vanadium, titanium, niobium, and tantalum. Such an alloy is called high-entropy: there is no single order, and the atoms are mixed almost randomly.
Mesoscale2026-08-181 minarXiv:2608.17789express
A Quantum Ladder Made of Germanium
Imagine a ladder whose rungs are tiny magnets. If neighboring magnets point in opposite directions, the ladder is "calm." But if you make them all point the same way, the whole structure becomes magnetized and "stubborn." Scientists built such a ladder from germanium atoms — a semiconductor used to make transistors.
Strongly Correlated2026-08-042 minarXiv:2608.03024express
Superconductivity in a Quantum Spin Liquid
A quantum spin liquid is a state of matter in which the magnetic moments of atoms behave like a fluid: they constantly fluctuate and never settle into a rigid order, even at extremely low temperatures. One of the most famous theoretical models of such a liquid was proposed by Alexei Kitaev.
Superconductivity2026-08-022 minarXiv:2608.01209express
Superconducting diode from a layered crystal
Hidden within thin layers of tantalum selenide (TaSe₂) is a property that defies conventional physics. When guest atoms were added between the layers of this material, the structure lost its center of symmetry, and inside, superconductivity with armor emerged.
Superconductivity2026-08-012 minarXiv:2608.00512express
Magnetic Jitters Give Rise to Superconductivity in Nickelates
Lossless current is the dream of energy technology. Some materials become superconductors, but usually only at extreme cold. Recently, in the family of nickelates, compounds based on nickel, candidates were found that work at higher temperatures.
Superconductivity2026-07-182 minarXiv:2607.16684express
Superconductivity in Nickelates Without Doping
A piece of metal is cooled to minus two hundred degrees, and electric current begins to flow through it without the slightest friction, like water in a pipe flowing without touching the walls. This behavior is called superconductivity.
When Repulsion Gives Birth to Pairs: A New Perspective on the Riddle of Superconductivity
For nearly forty years, high-temperature superconductivity in cuprates has remained one of the deepest riddles of condensed matter physics.
Mesoscale2026-06-273 minarXiv:2606.28877
Superconductivity2026-05-281 minarXiv:2605.29352express
Superconductivity in the simplest cuprate finally works
Imagine a sandwich where the bread is made of copper oxide layers and the filling is a thin layer of strontium ions. That's the infinite-layer cuprate, the simplest version of superconducting ceramics, conceived nearly 40 years ago.
Superconductivity2026-05-241 minarXiv:2605.25197express
Light Turns an Ordinary Conductor into a One-Way Street
An ordinary diode in electronics works like a one-way street: current flows in only one direction. In superconductors, where electricity flows without resistance, such behavior has long been elusive — current is usually symmetric. The authors of the new work found a way to create a perfect superconducting diode using light.
Quantum Physics2026-05-181 minarXiv:2605.19125express
A Tiny Magnet Sneaks Through an Invisible Wall
A tiny magnet levitates in a magnetic trap, like a weightless needle. Its magnetized axis is like a stubborn compass needle that is prevented from turning. An invisible wall rises before it. But in the quantum world, particles can seep through barriers — this trick is called tunneling.
Quantum Physics2026-05-101 minarXiv:2605.09632express
Pendulum Swinging Nonstop for Five Days
A tiny ball weighing a fraction of a milligram, suspended in a magnetic field and cooled to near absolute zero, oscillates for 110 hours without stopping: this is record isolation. The energy loss is so small that the system's entropy barely increases, making any external influence noticeable.
Superconductivity2026-04-141 minarXiv:2604.12742express
Domain Wall Steers the Current
Two superconducting banks are connected by a bridge of magnetic material. Inside the bridge lies a domain wall: a narrow boundary where the magnetization rotates, like a column of soldiers changing their marching direction.
Superconductivity2026-04-111 minarXiv:2604.10133express
The Hidden Metal Inside Superconductors
Inside copper-based superconductors, materials that carry current without loss at unexpectedly high temperatures, there is a hidden phase. It behaves like an ordinary metal, but it's invisible in standard measurements.
Superconductivity2026-04-071 minarXiv:2604.05997express
How a Superconductor Is Born from a Flat Band
Superconductivity is when electric current flows without losses, like water through a perfectly smooth pipe. It usually occurs at very low temperatures, but there are materials where it appears at higher ones.
Superconductivity2026-03-251 minarXiv:2603.24711express
Current That Outruns the Vortices
Electric current in a superconductor is like a crowd running down a frictionless corridor. But in type-II superconductors there are obstacles, tiny vortices of magnetic field, that the current shoves out of place. Once a vortex moves, resistance appears and the current drops.
HEP Phenomenology2026-03-231 minarXiv:2603.22647express
Levitating Magnet Catches Dark Matter
A tiny superconductor, levitating above a magnet, is like a cork on the surface of an invisible ocean. The slightest breath of dark matter makes it shudder. Scientists examined two kinds of such 'wind'. The first – gravitational waves, which stretch and squeeze space itself, like ripples on the fabric of the cosmos.
Superconductivity2026-03-111 minarXiv:2603.11278express
Heat Unlocks the Secret of a Superconductor
A uranium crystal the size of a grain of rice was cooled to one-fiftieth of a degree above absolute zero. At such temperatures, heat is not transported chaotically but strictly according to the rules of the quantum world.
Superconductivity2026-03-092 minarXiv:2603.08891express
A Superconducting Ring That Becomes a Magnet
An ordinary superconductor expels magnetic fields, but this ring does the opposite: it creates a magnetic field inside itself. The ring is made of Fe(Te,Se) — a compound of iron, tellurium, and selenium that loses its electrical resistance at very low temperatures.
Superconductivity2026-02-261 minarXiv:2602.22788express
Oscillations in a Wireless Superconductor
An ordinary superconductor loses resistance when cooled, and current flows through it without loss. But in ultrathin films, things are different: the material fluctuates between normal and superconducting states, and in this transition zone, strange resistance waves emerge. Resistance rises and falls as if someone were turning a volume knob.
Strongly Correlated2026-02-112 minarXiv:2602.11011express
A Quantum Crossroads Inside a Superconductor
Inside some materials, electric current flows with zero resistance. These are superconductors, and they only work when it's very cold. Copper oxides are special: they stay superconducting at somewhat higher temperatures, but why has been a puzzle for forty years.
Superconductivity2026-02-091 minarXiv:2602.08358express
The Spin That Won't Give In to Magnetic Fields
An ordinary superconductor is like a squad of soldiers marching in pairs: electrons pair up, and their spins (internal 'tops') point in opposite directions. A magnetic field easily flips such pairs, destroying superconductivity. In UTe₂, things are different.
Superconductivity2026-01-191 minarXiv:2601.12676express
Micrometers Decide the Fate of Superconductivity
A superconductor is like a city where electrons stop jostling and start moving in pairs, like people strolling arm in arm. In neodymium-strontium nickelate (Nd₀.₈Sr₀.₂NiO₂), this 'parade' kicks in at around 10 kelvin (minus 263 degrees Celsius), but not uniformly.
Superconductivity2026-01-161 minarXiv:2601.10939express
Electron Ripples in a Superconductor
In NaAlSi, as it cools, electrons form fleeting ripples — stripes that appear and vanish, like patterns on water stirred by wind. These stripes intertwine with superconductivity, a state where current flows without resistance. Typically, for this, electrons pair up with uniform binding energy.
Noise as an X-ray: How Hidden Triplet Superconductivity Emerged at a Superconductor-Iron Interface
Run a current through a contact between a superconductor and a ferromagnet, and you will hear the whisper of the quantum world. In the lab at 0.3 K, that whisper turned into a roar: the shot noise—electrical noise due to the discreteness of charge—was a hundred times louder than theory allows for ordinary contacts.