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Effects of Fe substitution by Nb on physical properties of BaFeO

3

: A DFT + U study

Imène Cherair

a

, Nadia Iles

b,

, Lyacine Rabahi

c,d

, Abdelhafid Kellou

a

aTheoretical Physics Laboratory, Faculty of Physics, USTHB, BP 32 El Alia, Bab Ezzouar, Algiers, Algeria

bLaboratory of Thin Films Physics and Materials for Electronics, Oran 1 University, Oran, Algeria

cMaterial Physics Laboratory, Faculty of Physics, USTHB, BP 32 El Alia, Bab Ezzouar, Algiers, Algeria

dResearch Center in Industrial Technologies (CRTI), BP 64, Cheraga, Algiers, Algeria

a r t i c l e i n f o

Article history:

Received 11 March 2016

Received in revised form 1 October 2016 Accepted 10 October 2016

Keywords:

BaFe1 xNbxO3perovskites Structural properties Magnetic moments Density Functional Theory GGA + U

Quasi-harmonic Debye model

a b s t r a c t

The structural, electronic, magnetic and thermal properties of BaFe1 xNbxO3perovskites oxides are inves- tigated using the Density Functional Theory (DFT). The Generalized Gradient Approximation (GGA) and on-site Hubbard potential corrections (GGA+U) are considered. According to the formation energies and phonon spectra, the stoichiometric BaFeO3and BaNbO3oxides have a stable cubic phase. TheGGA +Ucalculations show a half metallic behavior of BaFeO3with a large exchange splitting, in agreement with previous experimental and theoretical works. The Fe substitution by Nb forx= 0.5 leads to a surpris- ing insulating ground state. The values of the band gap is 0.40 eV and 1.84 eV usingGGAandGGA+U, respectively. Forx= 0.875 andx= 1, the corresponding alloys are metallic and non-magnetic, while for x= 0.5 andx= 0.625 the antiferromagnetic ground state is found usingGGA+U. For the remaining Nb compositions a half metallic character is noticed with a ferromagnetic state. The quasi-harmonic Debye model is successfully applied to study the temperature evolution of lattice parameters and bulk moduli for different Nb compositions.

Ó2016 Elsevier B.V. All rights reserved.

1. Introduction

The ABO3perovskites have gained a growing interest in recent years thanks to their promising physical properties such as ferro- electricity[1]and ferromagnetism[2]. These oxides have attractive applications in many technological fields such as data storage, energy and sensing devices[3]. New functionalities with peculiar physical properties appear when the B element is substituted by another element B0 leading to complex perovskite oxides (ABxB01 xO3). For example, Bormanis et al. [4] have evidenced capacitors with tunable permittivity in PbMg1/3Nb2/3O3 and PbZn1/3Nb2/3O3solid solutions. Setter et al.[5]have reported that the substitution of Ti by Zr in PbTiO3(PZT) gives rise to piezoelec- tricity. This property is exploited in transducers and actuators devices. Moreover, the substitution of a magnetic element in ABO3perovskites affects considerably their magnetic and transport properties [6]. In this context, BaFeO3 is one of the few oxides which contain Fe as a ferromagnetic element in a high valence state (Fe4+). A stoichiometric BaFeO3 with a cubic structure (Pm3m) has been obtained by Hayashi et al.[7]. This cubic symme-

try is preserved to at least 8 K. BaFeO3 has a A-type spiral spin order below 111 K and changes to a ferromagnetic order under a small magnetic field with a magnetic moment of 3.5

l

B/Fe. These features were investigated theoretically by Li et al.[8]. They have found that the A-and G-type helical orders in BaFeO3are almost degenerate with small energy difference as compared with the fer- romagnetic spin state. A transition from helical order to ferromag- netic order is found when the lattice constant is reduced[9]. Very recently, Rahman et al.[10]have shown that the ground state of cubic BaFeO3is ferromagnetic. The transition from a ferromagnetic to an antiferromagnetic state is yielded only if a displacement of Fe and O ions is considered. However, an experimental work on a thin film BaFeO3deposited by pulse laser technique highlighted a ferro- magnetic insulating behavior of this oxide with an optical gap of 1.8 eV[11].

It was also shown that the cubic structure of BaFeO3facilitates the oxygen vacancies formation making BaFeO3 d(BF) an interest- ing material for innovative electrodes with high activity for oxygen reduction reaction (ORR)[12–14]. This feature is improved when the B-site is substituted by another appropriate element. Among the wide range of B-site dopant that stabilizes the oxygen defi- ciency in BaFeO3 d, Nb5+is a stable cation. Accordingly, BaFe1 x- NbxO3 d is recently exploited as a cathode material for

http://dx.doi.org/10.1016/j.commatsci.2016.10.018 0927-0256/Ó2016 Elsevier B.V. All rights reserved.

Corresponding author.

E-mail address:n_ilesdz@yahoo.fr(N. Iles).

Computational Materials Science 126 (2017) 491–502

Contents lists available atScienceDirect

Computational Materials Science

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