What Gas Turns Into a Superfluid When Cooled to Absolute Zero?

The universe holds many surprising states of matter, particularly those that occur when substances are pushed to the limits of cold. As the temperature of a gas is drastically lowered, the familiar rules of classical physics begin to break down, giving way to profound quantum phenomena. This transition reveals a new form of existence for matter, characterized by synchronized particle behavior. Under these extreme conditions, matter can enter an exotic state that flows without any internal resistance. Scientists explore this boundary to observe how the collective behavior of atoms transforms a common substance into an entirely different, frictionless medium.

The Specific Gas and the Temperature Extreme

The substance that undergoes this transformation is the noble gas Helium, specifically its most common isotope, Helium-4. Helium is unique because it remains a liquid even at extremely low temperatures, unlike almost every other substance that solidifies under cooling. This normal liquid state, known as Helium I, must be cooled below a specific point to reveal its unusual characteristics. The transition to the frictionless state occurs precisely at the lambda point, which is about 2.17 Kelvin (K) at standard pressure.

This temperature is remarkably close to the theoretical limit known as absolute zero (0 Kelvin), where all thermal motion of particles ceases. While absolute zero is physically unattainable, the transformation in Helium-4 happens just over two degrees above this ultimate cold limit. Below the 2.17 K threshold, the liquid phase separates into two components, and the quantum-mechanically ordered component steadily increases as the temperature drops. By the time the liquid reaches 1 Kelvin, it is almost entirely in the frictionless state.

Helium-4 remains liquid down to the lowest temperatures, rather than freezing, due to its quantum nature. Even at 0 K, atoms possess a small, irreducible amount of energy called zero-point energy, a consequence of quantum mechanics. This zero-point energy is so substantial that it prevents the atoms from settling into a rigid, crystalline solid structure unless high pressure is applied. This allows the liquid to persist and exhibit the quantum effects that lead to its frictionless flow.

Defining the Superfluid State

The state of matter that Helium-4 enters below 2.17 K is termed a superfluid, a phase with properties that contrast sharply with normal liquids. Its defining characteristic is zero viscosity, meaning the liquid flows without any internal friction or resistance. If a superfluid were set into motion inside a closed loop, it would circulate indefinitely, never slowing down due to friction against itself or the container walls. This lack of resistance allows the fluid to pass effortlessly through microscopic channels and pores that would completely block any ordinary liquid.

The superfluid also exhibits extremely high thermal conductivity, which is millions of times greater than that of normal liquid Helium or copper metal. When heat is introduced, it does not bubble or boil like a normal liquid. Instead, the heat is transported almost instantly and efficiently throughout the entire volume by a unique counterflow of the fluid components. This process is so effective that the liquid remains perfectly still and clear, evaporating smoothly from its surface rather than violently boiling.

The most visually striking demonstration of this behavior is the creeping film effect, also known as the Rollin film. The liquid helium forms an extremely thin film, only a few hundred atoms thick, that adheres to and spreads across any solid surface it contacts. This film flows without friction, allowing the liquid to creep up and over the sides of its container, seemingly defying gravity. The superfluid continues to flow over the rim until the liquid level inside the container equalizes with the level of the surrounding bath, meaning an open container will simply empty itself by climbing out.

The Quantum Physics Behind Liquid Helium

The explanation for these behaviors is rooted entirely in quantum mechanics, specifically the classification of the Helium-4 atom as a boson. Particles fall into two categories based on their quantum spin: fermions (half-integer spin) and bosons (whole-integer spin). Because the Helium-4 nucleus contains an even number of protons and neutrons, the entire atom acts as a composite boson.

Bosons are unique because multiple identical particles can occupy the exact same quantum state simultaneously, a critical difference from fermions. When liquid Helium-4 is cooled below the lambda point, a significant fraction of its atoms condense into the lowest possible energy state. This phenomenon, known as Bose-Einstein Condensation (BEC), causes the liquid to behave not as a collection of individual atoms, but as a single, synchronized, macroscopic quantum entity.

The atoms within the condensate move in a coherent, collective manner, governed by a single wave function. This synchronization eliminates the random movement that causes friction in ordinary liquids. The portion of the liquid that has undergone BEC forms the superfluid component, possessing zero viscosity and zero entropy, while the rest remains a normal, viscous liquid. This is formalized in the two-fluid model, which treats the liquid as an inseparable mixture of these two components.

The quantum nature also manifests in the rotation of the superfluid, which cannot simply spin like a normal liquid. When stirred, it forms tiny, quantized vortices—miniature whirlpools that carry all the angular momentum. The circulation around the core of these vortices is restricted to specific, discrete values, demonstrating the quantization of motion on a macroscopic scale.

By contrast, the lighter isotope, Helium-3, is a fermion because its nucleus has an odd number of particles. Fermions cannot undergo simple BEC, so Helium-3 does not become a superfluid in the same way or at the same temperature. Instead, Helium-3 atoms must first form pairs, similar to the electron Cooper pairs in a superconductor, to collectively act as a boson. This complex pairing mechanism requires the liquid to be cooled to an even more extreme temperature, around 2.5 millikelvin, to achieve its own superfluid state.