Citation: Himcinschi, C.; Drechsler,
F.; Walch, D.S.; Bhatnagar, A.; Belik,
A.A.; Kortus, J. Unexpected Phonon
Behaviour in BiFe
x
Cr
1−x
O
3
,a
Material System Different from Its
BiFeO
3
and BiCrO
3
Parents.
Nanomaterials 2022, 12, 1607. https://
doi.org/10.3390/nano12091607
Academic Editor: Sam Lofland
Received: 31 March 2022
Accepted: 5 May 2022
Published: 9 May 2022
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nanomaterials
Article
Unexpected Phonon Behaviour in BiFe
x
Cr
1-x
O
3
, a Material
System Different from Its BiFeO
3
and BiCrO
3
Parents
Cameliu Himcinschi
1,
* , Felix Drechsler
1
, David Sebastian Walch
2,3
, Akash Bhatnagar
2,3
, Alexei A. Belik
4
and Jens Kortus
1
1
Institute of Theoretical Physics, TU Bergakademie Freiberg, D-09596 Freiberg, Germany;
felix.drechsler@student.tu-freiberg.de (F.D.); jens.kortus@physik.tu-freiberg.de (J.K.)
2
Zentrum für Innovationskompetenz SiLi-nano, Martin-Luther-Universität Halle-Wittenberg,
D-06120 Halle (Saale), Germany; david.knoche@physik.uni-halle.de (D.S.W.);
akash.bhatnagar@physik.uni-halle.de (A.B.)
3
Institut für Physik, Martin-Luther-Universität Halle-Wittenberg, D-06120 Halle (Saale), Germany
4
International Center for Materials Nanoarchitectonics (WPI-MANA), National Institute for Materials
Science (NIMS), Namiki 1-1, Ibaraki, Tsukuba 305-0044, Japan; alexei.belik@nims.go.jp
* Correspondence: himcinsc@physik.tu-freiberg.de
Abstract: The dielectric function and the bandgap of BiFe
0.5
Cr
0.5
O
3
thin films were determined from
spectroscopic ellipsometry and compared with that of the parent compounds BiFeO
3
and BiCrO
3
.
The bandgap value of BiFe
0.5
Cr
0.5
O
3
is lower than that of BiFeO
3
and BiCrO
3
, due to an optical
transition at ~2.27 eV attributed to a charge transfer excitation between the Cr and Fe ions. This optical
transition enables new phonon modes which have been investigated using Raman spectroscopy by
employing multi-wavelengths excitation. The appearance of a new Raman mode at ~670 cm
−1
with a
strong intensity dependence on the excitation line and its higher order scattering activation was found
for both BiFe
0.5
Cr
0.5
O
3
thin films and BiFe
x
Cr
1−x
O
3
polycrystalline bulk samples. Furthermore,
Raman spectroscopy was also used to investigate temperature induced structural phase transitions in
BiFe
0.3
Cr
0.7
O
3
.
Keywords: Raman spectroscopy; thin films; spectroscopic ellipsometry; charge transfer; phase
transition; multiferroics; BiFe
x
Cr
1−x
O
3
1. Introduction
Bi
2
FeCrO
6
was first theoretically proposed as a bismuth-based multiferroic material
having large spontaneous magnetisation and polarisation by means of first principle studies
by Baettig et al. [1,2]. Following this theoretical prediction, Bi
2
FeCrO
6
epitaxial films have
also been synthesised and its multiferroic character demonstrated [3,4]. Consequently,
a lot of attention was dedicated to the characterisation of structural, ferroelectric and
multiferroic properties of the material, and to the optimisation of the growth parameters for
thin films [5–8]. Promising photovoltaic properties, the low bandgap and the possibility to
tune it by the growth conditions, cationic ordering, and the domain size have attracted a lot
of attention in recent years [9–13]. Various heterostructures or BiCrO
3
/BiFeO
3
superlattices
with different thicknesses and repetitions have been proposed for designing efficient
ferroelectric photovoltaic devices [14–16].
Raman spectroscopy is an established method to detect subtle structural changes
induced by strain or temperature and it has been already very successfully applied to the
study of the lattice dynamics in the class of oxides with perovskite structures. However,
in the case of Bi
2
FeCrO
6
there are very few Raman or infrared spectroscopic studies
reported [17–19].
In the present paper Raman spectroscopy was used in combination with spectro-
scopic ellipsometry for the characterisation of BiFe
0.5
Cr
0.5
O
3
thin films and polycrystalline
Nanomaterials 2022, 12, 1607. https://doi.org/10.3390/nano12091607 https://www.mdpi.com/journal/nanomaterials