concept

superfluidity

Superfluidity is a quantum state of matter where a fluid flows without viscosity, as observed in helium and superconductors.
48 related articles · 1 formulas · 6 who worked here

Description

Superfluidity is a macroscopic quantum effect where a fluid moves without dissipation, has zero viscosity, and can flow through capillaries without resistance. It is observed in liquid helium-4 (bosons) at 2.17 K and in helium-3 (fermions) at about 2.6 mK.

History

In 1937, Pyotr Kapitsa in Cambridge discovered almost complete disappearance of viscosity in helium-4 below 2.17 K. Simultaneously, John Allen and Don Misener observed the fountain effect. In 1941, Lev Landau built a theoretical model, introducing the concepts of superfluid and normal components. The idea of connection with Bose-Einstein condensation, predicted by Satyendra Nath Bose and Albert Einstein, was proposed by Fritz London (not in the list). Superfluidity of He-3 was discovered in 1972 by Douglas Osheroff, Robert Richardson, and David Lee, and explained via Cooper pairing with anisotropy.

How it works

Superfluidity of helium-4 is due to the bosonic nature of atoms. At low temperatures, a macroscopic fraction of atoms occupies a single quantum state — a Bose-Einstein condensate forms. Elementary excitations — phonons and rotons — define the spectrum. According to Nöther's theorem, spontaneous breaking of gauge symmetry leads to a gapless mode of oscillations, providing superfluidity. The superfluid component flows without viscosity until the velocity exceeds a critical value determined by Landau's criterion. Superfluidity in helium-3 is more complex: atoms are fermions, they form Cooper pairs, turning into bosons, which then condense. This is analogous to superconductivity but with p-wave pairing, leading to anisotropic properties.

In practice

Superfluidity helps study quantum effects in the macroscopic world and cool superconducting magnets.

Fun fact

Superfluid helium-4 creates a fountain up to 40 cm high at the slightest thermal disturbance — this thermomechanical effect looks like a sudden geyser in a laboratory vessel.

Concept graph →

Formulas

$$J_0 = \frac{\rho_s}{m}$$
Superfluid stiffness relates to density and effective mass.
What is in the formula
J_0variableBare superfluid stiffness (phase stiffness) — superfluid stiffness joule
ρ_svariableSuperfluid mass density — superfluid density kilogram per cubic metre
mvariableEffective mass of the superfluid particles (e.g., helium atom mass) — mass kilogram
j_0(0)=\frac{n}{2m^*} · 2607.08353

Related articles · 118

A needle of water: how 10,000 agents made the Navier–Stokes equations blow up
In 1934 Jean Leray proved that the Navier–Stokes equations always have solutions "in a generalized sense". Whether a solution stays smooth or can break down into a singularity he could not tell, and nobody could for ninety years. In 2000 the Clay Institute made the question one of its seven Millennium Prize problems.
Light Flows Without Friction: Three Ways to Measure the Limit
In a Paris laboratory, light was made to flow around an obstacle the way water flows around a rock in a stream. But this water is special: it feels no friction.
A Semiconductor's Whisper Beneath a Superconductor's Hum
A thin layer of indium arsenide lies hidden under a superconducting film, like a voice beneath the noise of a crowd. In such a hybrid, current takes the path of least resistance and flows almost entirely through the metal, leaving the semiconductor inaudible to standard probes.
A Supercritical Cocktail: How Hydrogen Dissolves in the Depths of Sub-Neptunes
In the depths of sub-Neptunes, the most common type of planet in the Galaxy, though not one you could stand on, silicate magma and hydrogen mix into a single supercritical cocktail. Previously, it was thought that beneath the dense hydrogen atmosphere lay a sharp boundary with molten silicate, like oil on water.
The Magnesium Key to Sub-Neptune Interiors
Deep inside a sub-Neptune, where pressures reach a hundred thousand bars and temperatures hit four thousand degrees, rock behaves like boiling soup. Heavy vapors of silicon and magnesium rise, cool, and fall back as a rain of solid particles.
Superconductivity2026-08-181 minarXiv:2608.17777express
Heat Under Pressure: How to Measure the Invisible
A superconductor is a material in which electricity flows without loss, like water through a perfectly smooth pipe. But if you squeeze it slightly, like a spring, its properties change. Scientists have long wanted to measure how much heat such a compressed material absorbs, but instruments couldn't fit into the cramped setup. Now they've devised a way around this obstacle.
Superconductivity2026-08-162 minarXiv:2608.15745express
Superconductivity at pressures accessible to laboratories
An ordinary wire heats up when current flows through it — some energy is wasted. A superconductor lacks this flaw: electricity flows through it without loss, like water through a perfectly smooth pipe. The trouble is that most superconductors require either very low temperatures or colossal pressures, like those found in the depths of planets.
Superconductivity2026-08-082 minarXiv:2608.08120express
Strange Current in Graphene: When Weaker Means Stronger
A water pipe: the wider it is, the more water flows through. In superconducting contacts — Josephson junctions (bridges through which current flows without resistance)—it's usually the same: the better the material conducts in its normal state, the larger the superconducting current that flows through it.
Superconductivity2026-08-042 minarXiv:2608.03908express
A Nickel-Oxygen Superconducting Puzzle
A tiny sandwich of oxides, grown layer by layer, becomes perfectly conducting at about minus 200 degrees Celsius. This is not a magic trick but a new chapter in the search for high-temperature superconductors.
Strongly Correlated2026-08-032 minarXiv:2608.02753express
Superconductivity on the Edge of Two Worlds
At low temperatures, many materials become superconductors — current flows without resistance. But how exactly does this happen if electrons were initially trapped in an insulator? Half a century ago, Philip Anderson suggested that the answer lies in a special quantum dance of particles.
Superconductivity2026-08-021 minarXiv:2608.00942express
Superconductor Pushed to 190 Kelvin
Many materials behave like finicky ice: at one pressure they melt, at another they turn harder. Superconductors in the cuprate family are no exception. Their ability to carry current without loss depends on how tightly the crystal lattice is squeezed. In a new study, physicists traced this dependence for the compound Bi-2223.
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.
Superconductivity2026-07-122 minarXiv:2607.10668express
Squeezed, pressed, and peeked into the soul of a superconductor
Imagine trying to overhear a whisper between two people in a noisy hall. That's roughly the challenge physicists face when they want to understand how electrons pair up inside a superconductor. And if the "hall" is also squeezed by a giant press to pressures of hundreds of thousands of atmospheres, the task seems impossible. The authors of the new study found an ingenious solution.
Nuclear Theory2026-07-052 minarXiv:2607.04408express
A Superfluid Vortex with a Memory of Rotation
A superfluid flows without friction, like water that never stops. But when you spin it, it doesn't just rotate: each tiny vortex remembers exactly how it was spun. This 'trace' is not a metaphor but a real geometric imprint, which physicists call the Berry phase (the phase acquired by a wave as it travels along a closed path).
Nuclear Theory2026-07-042 minarXiv:2607.03716express
How an Explosion Protects a Vortex
In accelerators like the Large Hadron Collider, heavy nuclei collide at enormous speeds. For an instant, quark-gluon plasma (QGP) is born — a state of matter where quarks and gluons float freely, just like in the first microseconds after the birth of the universe. This plasma is not just hot.
Ice Labyrinth: When Forbidden Rules Birth a Three-Dimensional Quantum Liquid
In the conventional Heisenberg picture, spins at low temperatures are supposed to line up in a strict pattern. But there are crystals — like pyrochlore — where geometry has its own way. Each ion sits at a vertex of a tetrahedron, and the main interaction enforces a rule: two spins point inward, two outward.
Superconducting Web: How Defects in Graphene Weave Quantum Order
Graphene, a two-dimensional carbon crystal, has long tantalized physicists with the hope of high-temperature superconductivity. Its electrons obey the relativistic equation of Paul Dirac, racing at tremendous speed, barely noticing each other.
Mesoscale2026-06-273 minarXiv:2606.28877
Mesoscale2026-06-263 minarXiv:2606.27788
Symphony of the Quantum Drum: Collective Modes of Helium-3 After a Heat Shock
Imagine: superfluid helium-3 in a thin film receives a sudden heat shock. In that instant, a whole orchestra of collective oscillations awakens within it — like striking an invisible drum produces a multi-voiced chord. The Kibble–Zurek mechanism, familiar from the cracking of ice during rapid freezing, here acquires a quantum elegance.
Superconductivity2026-06-192 minarXiv:2606.21507express
Superconductivity2026-06-182 minarXiv:2606.20157express
Current Runs Along Secret Paths
In the crystal CsV3Sb5-xSnx, which becomes a superconductor at low temperatures, current does not flow as a uniform stream but along narrow, winding paths. A scanning microscope with a sensitive magnetic field sensor helped reveal these paths: it picks up the faintest currents, much like a sonar probes the seafloor.
Superconductivity2026-06-171 minarXiv:2606.18931express
Superconductivity Under Voltage: Current and Resistance Together
A superconductor is like an ideal highway with no traffic lights: electrons race along without hindrance. But apply a voltage, and the picture changes. In a new experiment, physicists found that an electric field penetrates the superconductor and creates a mixed regime inside.
Superconductivity2026-06-172 minarXiv:2606.19171express
Terahertz resonator boosts superconductivity
A well-coordinated orchestra of electrons in a superconductor is easily thrown off rhythm. Thermal jolts destroy the fragile order, and resistance returns. For decades, scientists have sought ways to strengthen this ensemble — mostly by changing the material's composition or compressing it to unimaginable pressures.
Superconductivity2026-06-161 minarXiv:2606.18084express
Terahertz resonator strengthens superconductivity
A thin film of yttrium barium copper oxide warms under a stream of infrared light, and suddenly stops dissipating energy. That's superconductivity: electrons pair up and move as a single quantum swarm. But in underdoped samples, the harmony breaks long before the pairs fall apart. The pairs are there, but the collective rhythm isn't.
Statistical Mech2026-06-142 minarXiv:2606.15557express
Liquid Glass and a Narrow Neck
A hot liquid flows easily: molecules dart around, collide, and quickly find new spots. But cool it below its freezing point, and everything changes. Motion nearly freezes, and viscosity skyrockets. The key question isn't that particles are lazy, but where they can even go. The authors combined two established ideas.
Superconductivity2026-06-061 minarXiv:2606.08181express
The Hg1223 Paradox: Repulsion Creating Superconductivity
Superconductors conduct current without loss, but usually require extreme cold. Hg1223 — a mixture of mercury, barium, calcium, copper and oxygen — breaks the rule: it stops resisting current already at –139°C. The secret is that the strong electrical repulsion between electrons forces them to pair up.
Superconductivity2026-05-311 minarXiv:2606.01235express
Quantum Dance Without a Gap
A stone falls into a pond, and ripples spread across the water. Long waves and short ones travel at the same speed: that's how ordinary sound behaves in almost any medium. But in quantum liquids, things can be different. Physicists considered a superfluid where particles move along a "flat" energy band.
Quantum Gases2026-05-302 minarXiv:2606.00854express
Helium Droplets and Hidden Symmetry
Three floats on water bob chaotically. But three helium atoms cooled to near absolute zero behave differently, as if obeying an invisible law of similarity. Their mutual attraction is so weak that the atoms form a loose cloud.
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.
Superconductivity2026-05-232 minarXiv:2605.24439express
Vacuum Turns an Ordinary Superconductor into an Extraordinary One
A superconductor carries current without resistance, like water running through a pipe without friction. The secret lies in electron pairs: two electrons stick together as one, even though they normally repel. In an ordinary superconductor, the spins of the electrons in a pair point in opposite directions: this is the singlet state.
Quantum Physics2026-05-221 minarXiv:2605.23197express
Quantum Mpemba: Strong Entanglement Melts Faster
Ordinary water freezes as expected. But sometimes hot water turns to ice faster than cold — the Mpemba effect. Recently, a similar rule-breaking was found in quantum entanglement — the invisible link between particles discovered by Erwin Schrödinger.
Superconductivity2026-05-172 minarXiv:2605.17227express
Superconducting glue withstands disorder
A crowd of people who can move freely but suddenly start acting as one: that's how a superconductor carries current without resistance.
Quantum Physics2026-05-171 minarXiv:2605.17507express
When Time and Space Swap Roles: The Hidden Symmetry of the Quantum World
A translator gets distracted by every rustle in the hall, and a one-hour meeting stretches into two. That's roughly how ordinary quantum mechanics works: a particle evolves in time, while space serves as the stage. But what if we swapped their roles? Then the particle 'moves' through space, and time becomes a static backdrop.
General Relativity2026-05-151 minarXiv:2605.16621express
Sound Trap in a Superfluid
Sound travels through a medium at a certain speed. If the medium moves faster, the sound gets swept along by the flow — like a wood chip pulled into a whirlpool. In superfluid helium — a frictionless liquid — rapid rotation spawns vortex funnels. Inside them, an acoustic black hole forms: a region from which sound cannot return.
Superconductivity2026-05-152 minarXiv:2605.15703express
Superconductivity without pressure: nickelates caught the gap
A packed stadium: fans mill about chaotically, creating jostling and resistance. That's how electrons behave in an ordinary conductor. In superconductivity, they pair up and move in sync, like spectators holding hands and calmly leaving the stands, without losing energy.