Disrupting crystalline order to restore superfluidity

October 15, 2018, University of Hamburg
Credit: CC0 Public Domain

What if you could disrupt the crystalline order of quantum matter so that a superfluid could flow freely even at temperatures and pressures where it usually does not? This idea has been demonstrated by a team of scientists led by Ludwig Mathey and Andreas Hemmerich from the University of Hamburg.

Freezing water entails a change from one phase of matter to another, called a phase transition. While this transition, like countless others that occur in nature, typically takes place at the same fixed conditions—in this case, the freezing point—it might be influenced in a controlled way. The freezing transition can be controlled to produce a sorbet or a slushy. To make a cold and refreshing slushy with the perfect consistency, a slush machine with constantly rotating blades prevents from crystalizing and turning the slushy into a solid block of ice.

Imagine controlling quantum matter in this same way. Rather than forming a normal liquid, like a melted slushy under the sun, quantum matter can form a superfluid. This counterintuitive form of matter was first observed in liquid helium at very , less than two Kelvin above absolute zero. The helium atoms have a strong tendency to form a crystal, like the water molecules in a slushy, and this restricts the of helium to very low temperatures and low pressures.

But what if you could turn on the blades in your slush machine for ? What if you could disrupt the crystalline order so that the superfluid could flow freely, even at temperatures and pressures where it usually does not? This was the idea now demonstrated by a team of scientists led by Ludwig Mathey and Andreas Hemmerich from the University of Hamburg. They have disrupted crystalline order in a quantum system in a controlled manner by shining light on it that oscillates in time at a specific frequency. Physicists use the term "driving" to describe this kind of periodic change applied to the system—an action performed by the churning blades in a slushy machine. Their work, published in Physical Review Letters, identified a fundamental mechanism for how a typical system with competing phases responds to an external periodic driving.

The researchers studied a gas of cold atoms placed between two highly reflecting mirrors. The mirrors form a cavity that serves as a resonator for photons as the atoms scatter them multiple times before being detected in experiments. To provide a source of photons, an external pump laser beam is directed at the cloud of atoms.

Similar to water changing its phase from liquid to ice, this light-matter system exhibits a . Atoms from an initially homogeneous gas spontaneously organize themselves in a checkerboard pattern when the intensity of the pump beam gets sufficiently strong. The self-organization comes at the expense of the superfluid, which is suppressed by the crystalline order. This is one of the many examples in nature of competition in which one phase wins over the other. The researchers show that with a little bit of "drive," you can tip the balance in favor of the underdog—in this example, the superfluid phase. "We observe from our computer simulations that a periodic modulation of the pump intensity can destabilize the dominant self-organized phase," explains lead author Jayson Cosme. "This allows the previously unstable homogeneous phase to reemerge and this restores the superfluid. It's light induced superfluidity."

The scientists then observed their prediction in an experiment conducted in the group of Andreas Hemmerich. "Intuitively, one might expect that if we shake the system, all it does is heat up. It was intriguing to see a clear signature of the quantum fluid reemerging," explains Andreas Hemmerich.

The enhancement or suppression of a due to an external driving force has also been suggested in other physical systems. For instance, in high-temperature superconductors, laser pulses can melt the equilibrium dominant striped order, paving the way for superconductivity to emerge—a phenomenon called light-induced superconductivity. The fundamental mechanism that can help explain this process is still a subject of debate. "We proposed this type of light control of superfluidity to demonstrate the principle that has been hypothesized for light induced superconductivity," explains Ludwig Mathey. With this finding, cold atom physics demonstrates a general, counterintuitive mechanism of controlling in many-body systems. It opens a new chapter of solid state physics in which scientists not only measure equilibrium properties of matter, but rather design a non-equilibrium state with desired properties via light control.

Explore further: Superradiant matter: A new paradigm to explore dynamic phase transitions

More information: Dynamical Control of Order in a Cavity-BEC System, J. G. Cosme, C. Georges, A. Hemmerich, and L. Mathey, Phys. Rev. Lett. 121, 153001 (2018). DOI: 10.1103/PhysRevLett.121.153001

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not rated yet Oct 15, 2018
See "Light touch transforms material into a superconductor," Physorg article dated January 14, 2011. My four comments to that article explain that result, and that same 2011 explanation applies equally well, seven years later, to the above result.
not rated yet Oct 15, 2018
In 1665, Christiann Huygens noted an "odd sympathy" between the periodic oscillations of the pendulums of two of his clocks. Their periodic oscillations synced (in a perfectly anti-phase manner). More recently, about 300 years later, Art Winfree explored systems of synchronized oscillators. Phases of matter are systems of coupled periodic oscillators.
not rated yet Oct 15, 2018
See also "Scientists discover new magnetic phase in iron-based superconductors," Physorg dated May 23, 2014, where I also made four comments under my Macksb pen name.

The key magnetic phase in the 2014 article is anti-phase spin. (Just like the odd sympathy that Huygens discovered.) The precise 4 way pairing is anti-phase across 2 diagonal pairs.

Cooper pairs follow the same principle. Anti-phase fermions form a boson.

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