Science, culture, complexity

Tag: ferromagnetism

  • A new beast: antiferromagnetic quasicrystals

    Scientists have made a new material that is both a quasicrystal and antiferromagnetic — a combination never seen before.

    Quasicrystals are a special kind of solid. Unlike normal crystals, whose atoms are arranged in repeating patterns, quasicrystals have patterns that never exactly repeat but which still have an overall order. While regular crystals have left-right symmetries, quasicrystals have unusual rotational ones.

    For decades, scientists wondered if certain kinds of magnetism, but especially antiferromagnetism, could exist in these strange materials. In all materials the electrons have a property called spin. It’s as if a small magnet is embedded inside each electron. The spin denotes the direction of this magnet’s magnetic field. In ferromagnets, the spins are aligned in a common direction, so the materials are attracted to magnets. In antiferromagnetic materials, the electron spins line up in alternating directions, so their effects cancel out.

    While antiferromagnetism is common in regular crystals, it’s thus far never been observed in a true quasicrystal.

    The new study is the first to show clear evidence of antiferromagnetic order in a real, three-dimensional quasicrystal — one made of gold, indium, and europium. The findings were published in Nature Physics on April 14.

    The team confirmed such a material is real by carefully measuring how its atoms and spins are arranged and by observing how it behaves at low temperatures. Their work shows that even in the weird world of quasicrystals, complex magnetic order is possible, opening the door to new discoveries and technologies.

    The scientists created a new alloy with the formula Au56In28.5Eu15.5. This means in 1,000 atoms’ worth of the material, 560 will be gold, 285 will be indium, and 155 will be europium. The composition tells us that the scientists were going for a particularly precise combination of these elements — which they could have known in one of two ways. It might have been trial-and-error*, but that makes research very expensive, or the scientists had reasons to expect antiferromagnetic order would appear in this material.

    They did. Specifically, the team focused on Au56In28.5Eu15.5 because of its (i) unique positive Curie-Weiss temperature and (ii) rare-earth content, and (iii) because its structural features matched the theoretical criteria for stable antiferromagnetic order. Previous studies focused on quasicrystals containing rare-earth elements because they often have strong magnetic interactions. However, these compounds typically displayed a negative Curie-Weiss temperature, indicating dominant antiferromagnetic interactions but resulting only in disordered magnetic states.

    A positive Curie-Weiss temperature indicates dominant ferromagnetic interactions. In this case, however, it also suggested a unique balance of magnetic forces that could potentially stabilise antiferromagnetic order rather than spin-glass behaviour. Studies on approximant crystals — periodic structures closely related to quasicrystals — had also shown that both ferromagnetic and antiferromagnetic orders are stabilised only when the Curie-Weiss temperature is positive. In contrast, a negative temperature led to spin-glass states.

    The scientists of the new study noticed that the Au-In-Eu quasicrystal fit into the positive Curie-Weiss temperature category, making it a promising candidate to have antiferromagnetic order.

    For added measure, by slightly altering the composition, e.g. adding an impurity to increase the electron-per-atom ratio, the scientists could make the antiferromagnetic phase disappear, to be replaced by spin-glass behaviour. This sensitivity to electron concentration further hinted that the composition of the alloy was at a sweet spot for stabilising antiferromagnetism.

    Finally, the team had also recently discovered ferromagnetic order in some similar gold-based quasicrystals with rare-earth elements. The success encouraged them to explore the magnetic properties of new compositions, especially those with unusual Curie-Weiss temperatures.

    The Au-In-Eu quasicrystal is also a Tsai-type icosahedral quasicrystal, meaning it features a highly symmetric atomic arrangement. Theoretical work has suggested that such structures could support antiferromagnetic order in the right conditions, especially if the atoms occupied specific sites in the lattice.

    To make the alloy, the scientists used a technique called arc-melting, where highly pure metals are melted together using an electric arc, then quickly cooled to form the solid quasicrystal. To ensure the mixture was even, the team melted and flipped the sample several times.

    Then they used X-ray and electron diffraction to check the atomic arrangement. These techniques passed X-rays and electrons through the material. A detector on the other side picked up the radiation scattered by the material’s atoms and used it to recreate their arrangement. The patterns showed the material was a primitive icosahedral quasicrystal, a structure with 20-sided symmetry and no repeating units.

    The team also confirmed special arrangement of atoms by the way the diffraction patterns followed mathematical rules that are special to quasicrystals. Team members also used a magnetometer to track how much the material was magnetised when exposed to a magnetic field, from temperatures as low as 0.4 K to up to 300 K. Finally they also measured the material’s specific heat, i.e. the amount of heat energy it took to raise its temperature by 1º C. This reading can show signs of magnetic transitions.

    Left: The arrangement of atoms in the quasicrystal alloy. The atoms are arranged in a combination of two patterns, shown on the right. The colouring denotes their place in either pattern rather than different elements. Credit: Nature Physics volume 21, pages 974–979 (2025)

    To confirm how the spins inside the material were arranged, the team used neutron diffraction. Neutrons are adept at passing through materials and are sensitive to both atoms’ positions and magnetic order. By comparing patterns at temperatures above and below the suspected transition point, they could spot the appearance of new peaks that signal magnetic order.

    This way, the team reported that at 6.5 K, the magnetisation curve showed a sharp change, known as a cusp. This is a classic sign of an antiferromagnetic transition, where the material suddenly changes from being unordered to having a regular up-and-down pattern of spins. The specific heat also showed a sharp peak at this temperature, confirming something dramatic was happening inside the material.

    The scientists also reported that there was no sign of spin-glass behaviour — where the spins are pointing in random directions but unchanging — which is common in other magnetic quasicrystals.

    Below 6.5 K, new peaks appeared in the neutron diffraction data, evidence that the spins inside the material were lining up in the regular but alternating pattern characteristic of antiferromagnetic order. The peaks were also sharp and well-defined, showing the order was long-range, meaning they were there throughout the material and not confined to small patches.

    The team also experimented by adding a small amount of tin to the alloy, which changed the balance of electrons. This little change caused the material to lose its antiferromagnetic order and become a spin glass instead, showing how delicate the balance is between different magnetic states in quasicrystals.

    The findings are important because this is the first time scientists have observed antiferromagnetic order in a real, three-dimensional quasicrystal, settling a long-standing debate. They also open up a new field of study, of quasiperiodic antiferromagnets, and suggest that by carefully tuning the composition, scientists may be able to find yet other types of magnetic order in quasicrystals.

    “The present discovery will stimulate both experimental and theoretical efforts to elucidate not only its unique magnetic structure but also the intrinsic properties of the quasiperiodic order parameter,” the scientists wrote in their paper. “Another exciting aspect of magnetically ordered quasicrystals is their potential for new applications such as functional materials in spintronics” — which use electron spins to store and process information in ultra-fast computers of the future.


    * Which is not the same as serendipity.

    Featured image credit: Nature Physics volume 21, pages 974–979 (2025).

  • The Berry phase of Kancha Gachibowli

    There’s a concept in quantum mechanics, and also in parts of classical mechanics, called the Berry phase. Say you’re walking around a mountain. You start off along a path and follow it all the way until you’re back to the point where you started. You’re at the same point, sure, but you’re probably facing a different direction now. The Berry phase works something like this. Say you’ve got a bunch of electrons that you’re manipulating using a magnetic field. As you vary the field in continuous increments, the electrons will respond continuously in some way. But as you vary the field through a cycle of changes and bring it back to the original setting, the electrons won’t exactly be at their original configuration as well. Or they will be in addition to some change. This ‘additional change’ is called the Berry phase.

    Reading about the Kancha Gachibowli forest brought the Berry phase to mind. Yesterday, India’s new Chief Justice, B.R. Gavai, faced Telangana state with a choice: “between restoring the forest or having the Chief Secretary and [half a dozen] officials in prison,” per The Hindu. The latter people are being held responsible for attempting to divert mostly moderately and densely forested land to a planned campus for information technology companies. The court had no sympathy for Telangana counsel Abhishek Manu Singhvi’s argument that the state’s efforts had been good-intentioned. The principle reason: the state hasn’t been able to explain the fact that it organised a phalanx of bulldozers to bring down 104 acres of old trees during an extended weekend, when the courts were closed, leaving the felling’s opponents without access to legal recourse. A few telling passages from The Hindu:

    The State had previously denied the land was a forest. The claim, it said, that the area was forest land had sprung up only after developmental activities commenced following the allotment of the land to the Telangana Industrial Infrastructure Corporation. Mr. Singhvi submitted that the processes regarding the allotment had been on since March 2024. He said the intention of the State was bona fide.

    Mr. Singhvi maintained that “thousands” of trees were not cut. “We have seen the photographs,” Chief Justice Gavai responded.

    Mr. Singhvi submitted that not a leaf has been moved on the site after the apex court ordered everything to be stopped on April 16. The State was complying with the court’s direction in letter and spirit. A huge afforestation programme was underway in the area.

    Amicus curiae, senior advocate K. Parameshwar, drew the attention of the court to a finding in a Forest Survey of India report, which was forwarded to the Central Empowered Committee, that out of the 104 acres cut in two nights, over 60% had been moderately and heavily dense forest.

    It’s worthwhile these days to treat the concept of afforestation as a yellow flag at best and a despicable idea at worst. In the last decade it has evolved regressively into a sort of olive branch offered up alongside casual excuses to divert forested land for non-forest uses, often in open defiance of India’s existing forest protection laws — which sadly have been increasingly enfeebled by the environment ministry. That the state is now afforesting the area is little consolation because the trees that have already been cut represent a greater ecological loss than that can be recouped by young plants anytime in the near future. We may have come full circle since the state first felled the trees but we bear the burden of an additional change as well.

    In fact, this could be more like magnetic hysteresis than the Berry phase depending on the mode of afforestation. Quantum systems are said to have acquired a Berry phase when they undergo a reversible process in which entropy doesn’t increase*. But entropy, the amount of disorder, has indeed increased. We’ve lost energy. We’ve lost old trees and their ecosystem services. We’ve lost a sustainable carbon store. We’ve learnt that the Telangana government is willing to act in bad faith. We’ve learnt that our forest protection laws continue to not work. Why, we’ve been reminded that the Supreme Court remains the country’s last democratic institution, perhaps short of Parliamentary majority, prepared to measure the loss of green cover by the precepts of sustainable development. Every Supreme Court decision to stall a project that entails deforestation has been met with cheers in the conservation and environmental justice communities but each such verdict also serves a reminder that we remain at the mercy of the last line of defence. If someday the Supreme Court also yields, or is let down by Parliament passing a law that makes a mockery of protecting trees, we are only left with protest — like the brave students of the University of Hyderabad mounted to bring the Kancha Gachibowli issue to the whole country’s attention.

    When you apply a magnetic field over a ferromagnet, like a block of iron, it becomes magnetised. If you remove the magnetic field, the block stays magnetised to some degree. This phenomenon is called remanence. Future attempts to magnetise and demagnetise the block will have to work against the remanence, causing the block to lose energy over time as heat. This macroscopic feature is called magnetic hysteresis**: it’s irreversible, dissipative, disorderly, and vexatious. Much like the state of Telangana, it claims to find value in the context of computers (disk drives in particular), and much like the trees of Kancha Gachibowli, there’s nothing a ferromagnet can do about it.


    * I’ve used entropy here with reference to a quantum adiabatic process. In a thermodynamic adiabatic process, entropy isn’t produced only if the process is also reversible.

    ** The term ‘hysteresis’ comes from the Greek ‘hústeros’, meaning ‘later’. This is a reference to the shape of the curve on a graph with the strength of the magnetic field H on one axis and the magnetisation M on the other. As the H curve rises and falls, the M curve starts to fall behind. The seemingly closely related ‘hysteria’ comes from the Greek ‘hustéra’, for ‘womb’, and is thus unrelated. However, the well-known Cornell University physicist James P. Sethna wrote sometime before 1995:

    There seems to be no etymological link between hysteresis and either hysterical (fr. L hystericus of the womb) or history (fr. Gk, inquiry, history, fr. histor, istor knowing, learned). This is too bad, as there are scientific connections to both words. (There is no link, scientific or etymological, to histolysis, the breakdown of bodily tissues, or to blood.) … Many hysteretic systems make screeching noises as they respond to their external load (hence, the natural connection with hysteria).

    ‘Hysteria’ has of course rightly fallen out of favour both within and without clinical contexts.

  • Unexpected: Magnetic regions in metal blow past speed limit

    You’re familiar with magnetism, but do you know what it looks like at the smallest scale? Take a block of iron, for example. It’s ferromagnetic, which means if you place it near a permanent magnet – like a refrigerator magnet – the block will also become magnetic to a large extent, larger than materials that aren’t ferromagnetic.

    If you zoom in to the iron atoms, you’ll see a difference between areas that are magnetised and areas that aren’t. Every subatomic particle has four quantum numbers, sort of like its Aadhaar or social security ID. No two electrons in the same system can have the same ID, i.e. one, some or all of these numbers differ from one electron to the next. One of these numbers is the spin quantum number, and it can have one of two values, or states, at any given time. Physicists refer to these states as ‘up’ and ‘down’. In the magnetised portions, in the iron block, you’ll see that electrons in the iron atoms will either all be pointing up or all down. This is a defining feature of magnetism.

    Scientists have used it to make hard-disk drives that are used in computers. Each drive stores information by encoding it in electrons’ spins using a magnetic field, where, say, ‘1’ is up and ‘0’ is down, so a series of 1s and 0s become a series of ups and downs.

    In the iron block, the parts that are magnetised are called domains. They demarcate regions of uniform electron spin in three dimensions in the block’s bulk. For a long time, scientists believed that the ‘walls’ of a domain – i.e. the imaginary surface between areas of uniform spin and areas of dis-uniform spin – could move at up to around 0.5 km/s. If they moved faster, they could destabilise and collapse, allowing a kind of magnetic chaos to spread within the material. They arrived at this speed limit from their theoretical calculations.

    The limit matters because it says how fast the iron block’s magnetism can be manipulated, to store or modify data for example, without losing that data. It also matters for any other application that takes advantage of the properties of ferromagnetic materials.

    In 2020, a group of researchers from the Czech Republic, Germany, and Sweden found that if you stacked up a layer of ferromagnets, the domain walls could move much faster – as much as 14 km/s – without collapsing. Things can move fast in the subatomic realm, yet 14 km/s was still astonishing for ferromagnetic materials. So scientists set about testing it.

    A group from Italy, Sweden, and the US reported in a paper published in Physical Review Letters on December 19 (preprint here) that they were able to detect domain walls moving in a composite material at a stunning 66 km/s – greater than the predicted speed. Importantly, however, existing theories that explain a material’s magnetism at the subatomic scale don’t predict such a high speed, so now physicists know their theories are missing something.

    In their study, the group erected a tiny stack of the following elements, in this order: tantalum, copper, a cobalt-iron compound, nickel, the cobalt-iron compound, copper, and tantalum. Advanced microscopy techniques revealed that the ferromagnetic nickel layer (just a nanometre wide) had developed domains of two shapes: some were like stripes and some formed a labyrinth with curved walls.

    The researchers then tested the domain walls using the well-known pump-probe technique: a blast of energy first energises a system, then something probes it to understand how it’s changed. The pump here was an extremely short pulse of infrared radiation and the probe was a similarly short pulse of ultraviolet (UV) radiation.

    The key is the delay between the pump and probe pulses: the smaller the delay, the greater the detail that comes to light. (Three people won the physics Nobel Prize this year for finding ways to make this delay as small as possible.) In the study it was 50 femtoseconds, or 500 trillionths of a second.

    The UV pulse was diffracted by the electrons in nickel. A detector picked up the diffraction patterns and the scientists ‘read’ them together with computer simulations of the domains to understand how they changed.

    How did the domains change? The striped walls were practically unmoved but the curved walls of the labyrinthine pattern did move, by about 17-23 nanometres. The group made multiple measurements. When they finally calculated an average speed (which is equal to distance divided by time), they found it to be 66 km/s, give or take 20 km/s.

    An image depicting domains (black) in the nickel layer. The coloured lines show their final positions. Source: Phys. Rev. Lett. 131, 256702

    The observation of extreme wall speed under far-from-equilibrium conditions is the … most significant result of this study,” they wrote in their paper. This is true: even though the researchers found that the domain-wall speed limit in a multilayer ferromagnetic material is much higher than 0.5 km/s – as the 2020 group predicted – they also found it to be a lot higher than the expected 14 km/s. Of course, it’s also stunning because the curved domain walls moved at more than 10-times the speed of sound in that material – and the more curved a portion was, the faster it seemed to move.

    The researchers concluded that “additional mechanisms are required to fully understand these effects” – as well as that they could be “important” to explain “ultrafast phenomena in other systems such as emerging quantum materials”.

    This is my second recent post about scientists finding something they didn’t expect to, but in settings more innocuous than in the vast universe or at particle smashers. Read the first one, about the way paint dries, here.