cm8b04447_si_001.pdf (875.87 kB)
Stoichiometric Control over Ferroic Behavior in Ba(Ti1–xFex)O3 Nanocrystals
journal contribution
posted on 2019-01-14, 00:00 authored by Julien Lombardi, Long Yang, Frederick A. Pearsall, Nasim Farahmand, Zheng Gai, Simon J. L. Billinge, Stephen O’BrienBa(Ti,Fe)O3 is a useful system for the exploration of
multiferroic properties as a function of composition and variation
in structure, based upon a model of intersubstitution of the B site
cation. Nanocrystals of Ba(Ti,Fe)O3 could be used as building
blocks for composite multiferroic materials, provided ferroic properties
are recognizable at this length scale and Ti and Fe serve as ideal
models for the case of d0 versus dn in a ferroic perovskite.
A series of iron-substituted barium titanate nanocrystals (BaTi1–xFexO3) were synthesized at 60 °C using a hybrid sol–gel
chemical solution processing method. No further crystallization/calcination
steps were required. The as-prepared nanocrystals are fully crystalline,
uniform in size (∼8 nm by TEM), and dispersible in polar organic
solvents, yielding nanocrystal/alcohol formulations. Complete consumption
of the reactant precursors ensures adequate control over stoichiometry
of the final product, over a full range of x (0,
0.1 to 0.75, 1.0). Pair distribution function (PDF) analysis enabled
in-depth structural characterization (phase, space group, unit cell
parameters, etc.) and shows that, in the case of x = 0, 0.1, 0.2, 0.3, BaTiO3, and BaTi1–xFexO3 nanocrystals,
it is concluded that they are tetragonal noncentrosymmetric P4mm with lattice parameters increasing
from, e.g., c = 4.04 to 4.08 Å. XPS analysis
confirms the presence of both Fe3+(d5) and Fe4+(d4), both
candidates for multiferroicity in this system, given certain spin
configurations in octahedral field splitting. The PDF cacluated lattice
expansion is attributed to Fe3+(d5, HS) incorporation. The evidence of noncentrosymmetry, lattice
expansion, and XPS conformation of Fe3+ provides support
for the existence of multiferroicity in these sub-10 nm uniform dispersed
nanocrystals. For x > 0.5, Fe impacts the structure
but still produces dispersible, relatively monodisperse nanocrystals.
XPS also shows an increasing amount of Fe4+ with increasing
Fe, suggesting that Fe(IV) is evolving as charge compensation with
decreasing Ti4+, while attempting to preserve the perovskite
structure. A mixture of Fe3+/Fe4+ is thought
to reside at the B site: Fe4+ helps stabilize the structure
through charge balancing, while Fe3+ may be complimented
with oxygen vacancies to some extent, especially at the surface. The
structure may therefore be of the form BaTi1–xFexO3‑δ for increasing x. At higher concentrations (Fe
> 0.5) the emergence of BaFeO3 and/or BaFe2O4 is offered as an explanation for competing phases,
with BaFeO3 as the likeliest competing phase for x =
1.0. Because of the good dispersibility of the nanocrystals in solvents,
spin coating of uniform 0–3 nanocomposite BaTi1–xFexO3/polyvinylpyrrolidone
thin film capacitors (<0.5 μm) was possible. Frequency dependent
dielectric measurements showed stable dielectric constants at 1 MHz
of 27.0 to 22.2 for BaTi1–xFexO3 samples for x = 0–0.75, respectively. Loss tangent values at 1 MHz were
∼0.04, demonstrating the ability to prepare capacitors of magnetic
Ba(Ti1–xFex)O3 with relatively high permittivity. Magnetic
characterization by MPMS (both magnetic hysteresis loops and zero
field and field cooling measurements) showed increased magnetization
with increasing Fe ion concentration. Weak magnetic coercivity and
a small remanence magnetization is observed (<5 K), implying a
weak ferromagnetic state at low temperatures (<5 K).