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Department News
How small is too small to be useful?
Physics Department researchers have done nanoscale analysis on ferroelectric thin films - materials that are used in electronic
devices from computer memories to iPhones and polarize when exposed to an electric charge - and found that when it comes to polarization, both size and location
matter.
The finding by Professor Marco Buongiorno-Nardelli and post-doctoral researcher Matías Nuñez suggests that, in creating tiny electrical devices, the
use of extremely small components comes with the possibility of decreased effectiveness. Ferroelectric thin films are like sandwiches - layers of material held
between two metals. When a charge is applied to the material in the sandwich, it polarizes, taking on a uniformly positive or negative charge.
Buongiorno-Nardelli and Nuñez have theorized that when ferroelectric thin films are miniaturized, at a certain size the material loses its ability to
polarize. They found that this is not exactly the case: The atoms in the ferroelectric thin film still polarize, even on the nanoscale, but they don’t do so in a
uniform way, as they do at a larger scale. Instead, the polarization is disorganized with some atoms taking on a positive and others a negative charge, changing
the overall properties of the material and allowing for residual polarization to exist. Their results were published online in the journal Physical Review
Letters.
Buongiorno-Nardelli and Nuñez used computer modeling to examine how individual atoms within the thin film interacted with one another, and focused
specifically on the distribution of the electrons within the atoms, since electron distribution determines whether the ferroelectric will polarize with a positive
or negative charge. They discovered that at a thickness of around 20 to 30 nanometers, disorganization appears in the material.
"When you get to the nanoscale, you have individual atoms interacting with one another instead of groups of atoms," Buongiorno-Nardelli says. "At that point, it is
no longer the property of the material itself - the ferroelectric - that counts, because the property of the interface, where the atoms bond, becomes dominant."
Energy landscape of the ferroelectric film as function of the local polarization and thickness. For thick films,
the spatial distribution of dipoles that minimizes the total energy forms a domain where both polarizations in the BaO and
TiO2 planes have the same sign [A]. As the number of unit cells is lowered, the minimum shifts to lower values
of the BaO layer polarization [B] until at a critical thickness [C] it becomes zero. Further reduction of the number of layers flips only
the dipoles belonging to the BaO planes establishing a ferrielectric dipole pattern [D]
| Geometry of the ferroelectric thin film (cyan and red atoms) sandwiched between metals (gray atoms).
Blue-gray spheres are the metal atoms at the interface between the two materials, where the bonding is
stronger |
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this article was also published on ncsu's home page.
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