(Left panel) In nickel molybdate crystals made of two parts nickel, three parts molybdenum and eight parts oxygen, nickel ions are subject to both tetrahedral and octahedral crystalline environments, and the ions are locked in triangular lattices in each environment. (Right panel) Crystal electric field spin excitons from tetrahedral sites in nickel molybdate crystals form a dispersive, diffusive pattern around the Brillouin zone boundary, likely due to spin entanglement and geometric frustrations. The left and right halves of the panel show different model calculations of these patterns. Image: Bin Gao/Rice University.
(Left panel) In nickel molybdate crystals made of two parts nickel, three parts molybdenum and eight parts oxygen, nickel ions are subject to both tetrahedral and octahedral crystalline environments, and the ions are locked in triangular lattices in each environment. (Right panel) Crystal electric field spin excitons from tetrahedral sites in nickel molybdate crystals form a dispersive, diffusive pattern around the Brillouin zone boundary, likely due to spin entanglement and geometric frustrations. The left and right halves of the panel show different model calculations of these patterns. Image: Bin Gao/Rice University.

Perturbing electron spins in a magnet usually results in excitations called ‘spin waves’, which ripple through the magnet like waves on a pond that’s been struck by a pebble. In a new study, physicists at Rice University, together with collaborators, have discovered dramatically different excitations called ‘spin excitons’ that can also ‘ripple’ through a nickel-based magnet as a coherent wave.

In a paper in Nature Communications, the researchers report finding unusual properties in nickel molybdate, a layered magnetic crystal. Typically, electrons, which can resemble miniscule magnets, orient themselves like compass needles in relation to magnetic fields. But in experiments where neutrons were scattered from magnetic nickel ions inside the crystals, the researchers found that the two outermost electrons in each nickel ion behaved differently. Rather than aligning their spins like compass needles, the two canceled one another in a phenomenon physicists call a spin singlet.

“Such a substance should not be a magnet at all,” said Rice’s Pengcheng Dai, corresponding author of the paper. “And if a neutron scatters off a given nickel ion, the excitations should remain local and not propagate through the sample.”

Dai and his collaborators were therefore surprised when instruments in the neutron-scattering experiments detected not one but two families of propagating waves, each at dramatically different energies.

To understand the waves’ origins, it was necessary to delve into the atomic details of the magnetic crystals. For instance, electromagnetic forces from atoms in crystals can compete with the magnetic field and affect electrons inside neighboring atoms. This is called the crystal field effect, and it can force electron spins to orient themselves along directions distinct from the orientation of the magnetic field. Probing crystal field effects in the nickel molybdate crystals required additional experiments and theoretical interpretation of the data from these experiments.

“The collaboration between experimental groups and theory is paramount to painting a full picture and understanding the unusual spin excitations observed in this compound,” said Rice co-author Emilia Morosan.

Morosan’s group probed the response of the crystals to changes in temperature using specific heat measurements. From those experiments, the researchers concluded that two kinds of crystal field environments occurred in the layered nickel molybdate, and that the two affected nickel ions very differently.

“In one, the field effect is rather weak and corresponds to a thermal energy of about 10 Kelvin,” said co-author Andriy Nevidomskyy, a theoretical physicist at Rice who helped interpret the experimental data. “It is perhaps not surprising to see, at few-Kelvin temperatures, that neutrons can excite magnetic spin waves from nickel atoms that are subject to this first type of crystal field effect. But it is most puzzling to see them coming from nickel atoms that are subject to the second type. Those atoms have a tetrahedral arrangement of oxygens around them, and the electric field effect is nearly 20-fold stronger, meaning the excitations are that much harder to create.”

According to Nevidomskyy, this can be understood as if the spins on the corresponding nickel ions had different ‘mass’. “The analogy is that of heavy basketballs that are intermixed with tennis balls,” he said. “To excite the spins of the second type, the heavier basketballs, one must administer a stronger ‘kick’ by shining more energetic neutrons at the material.”

The resulting effect on the nickel spin is called a spin exciton, and one would normally expect the effect of the exciton-producing ‘kick’ to be confined to a single atom. But measurements from the experiments indicated that ‘basketballs’ were moving in unison, creating an unexpected sort of wave. Even more surprising, the waves appeared to persist at relatively high temperatures where the crystals no longer behaved as magnets.

Together with theorist co-author Leon Balents from the University of California, Santa Barbara, Nevidomskyy was able to come up with an explanation for this effect. Heavier spin excitons – basketballs in the analogy — bob in response to the fluctuations of the surrounding, lighter magnetic excitons – the tennis balls. If the interactions between the two types of balls are sufficiently strong, the heavier spin excitons participate in a coherent motion akin to a wave.

“What is particularly interesting,” Dai said, “is that the two kinds of nickel atoms each form a triangular lattice, and the magnetic interactions within this lattice are therefore frustrated.”

In magnetism on triangular lattices, frustration refers to the difficulty in aligning all the magnetic moments anti-parallel (up-down) with respect to their three immediate, nearest neighbors. Understanding the role of magnetic frustrations in triangular lattices is one of the long-standing challenges that Dai and Nevidomskyy have both been working to address for a number of years.

“It is very exciting to find a puzzle, against one’s expectations, and then feel a sense of satisfaction of having understood its origin,” said Nevidomskyy.

This story is adapted from material from Rice University, with editorial changes made by Materials Today. The views expressed in this article do not necessarily represent those of Elsevier. Link to original source.