Elsevier

Journal of Alloys and Compounds

Volume 623, 25 February 2015, Pages 192-196
Journal of Alloys and Compounds

Ferromagnetic behaviour of bismuth germanate oxides glass–ceramic materials

https://doi.org/10.1016/j.jallcom.2014.10.104Get rights and content

Highlights

  • Diluted ferromagnetism was evidenced in Bi based glass ceramics (BGO).

  • It is related mainly to oxygen defects in the atypical amorphous phase.

  • The coercivity depends on the density of such defects.

  • The magnetization depends on the overall number of O defects in GeO4 tetrahedra.

Abstract

The content of defects in Bi4Ge3O12 (BGO) glass–ceramic materials together with their ordering during crystallization induces ferromagnetic behaviours in these materials. The observed ferromagnetism has to be associated strictly with the GeO4 related defects in the atypical amorphous phase. The photoluminescence of BGO glass–ceramic materials can give useful information about the nature of defects, especially the oxygen vacancies from the GeO4 tetrahedra and Bi4Ge3O12 cubic structures. The concentration of these defects depends on annealing between 600 °C and 700 °C where orthorhombic and cubic phases coexist. The magnetization at saturation is higher in the samples dominated by the amorphous phase and the strength of the exchange interaction is higher in the samples dominated by the cubic phase, obtained over 700 °C, when the GeO4 tetrahedra are rearranged during crystallization together with their oxygen vacancies.

Introduction

Amorphous materials become an important player nowadays in the fabrication of very resistant devices, being more efficient than the crystalline structures [1]. However, heterogeneous nucleation of these amorphous materials drastically changes the physical properties of the obtained glass–ceramic materials.

Bismuth germanate oxides are known as scintillator materials based on the Bi3+ emission [2], [3], [4]. These oxides have eulityne-type cubic structure and crystallize in the space group I-43d. The Bi4Ge3O12 cubic structure consists of a regular arrangement of GeO4 tetrahedra and distorted BiO6 octahedrons [5], [6]. The heterogeneous crystallization of these oxides is obtained by controlled nucleation in which the glass precursor is thermally transformed, firstly in nano-crystalline dispersed particles in the whole glass [7]. At high temperatures, bismuth germanate oxides crystallize in a cubic structure as a dominant phase, but at lower temperatures some other crystalline phases are involved in the crystallization processes. For example, there is the intermediate phase of orthorhombic structure, Bi2GeO5, which is important due to its ferroelectric behaviour [8].

In the recent years, a series of oxides have been studied for their ferromagnetic behaviour at room temperature, e.g. MgO [9], Al2O3 [10], ZnO [10] and GaN [11]. The controversy regarding the ferromagnetic properties of transition metal (TM) doped oxides (diluted magnetism due to indirect interactions between TM ions versus magnetism due to TM based magnetic precipitates) is in case of these compounds based on just diamagnetic TM ions (as for example Bi3+) even more pronounced. Their magnetic behaviour is generally associated with inherent defects induced in a nanoparticule-like morphology, giving rise to local magnetic moments. Such defects might be also related to oxygen vacancies, which might have a direct influence on the photoluminescence properties of the oxides. The gradually annealing of the amorphous glasses of bismuth germanate oxides involves a critical temperature range in which the high and low temperature phases can co-exist and transform one to another. Expectedly, such a gradually transformation might tune the density of the oxygen vacancies together with the photoluminescence and ferromagnetic properties of the glass–ceramic materials, which can be finally used as case study of such inter-relations. For example, the photoluminescence of bismuth germanate oxides is based on three different aspects related to this material: GeO4 luminescence, Bi3+ optical transitions and the oxygen vacancies produced during sample preparation. It is clearly that in the bismuth germanate oxides perfect crystals, the number of oxygen vacancies are expected to be as low as possible, whereas formation of nanocrystalline phases allows to tune in a controlled manner the density of both the oxygen vacancies and expected magnetic defects.

The aim of this paper is focused on the study of the ferromagnetic behaviour of the bismuth germanate oxides glass–ceramic materials (previously annealed between 600 °C and 700 °C, where nanocrystalline Bi2GeO5 is dominant) in connection with their photoluminescence and XRD analysis, providing information about different defects in materials.

Section snippets

Materials and methods

Bi2O3 (99.999%) and GeO2 (99.999%) raw materials, purchased from Sigma-Aldrich and Alfa Aesar respectively, were used without further purifications. The drying and heating were made in Nabertherm P320 furnace with 400°C/h heating ramp.

Molar percents of Bi2O3 and GeO2 (40% and 60%, respectively) were wet-mixed in acetone. After drying at 100°C for 24 h, the mixtures were transferred to Al2O3 crucibles and then covered with an alumina lid. The mixtures have been rapidly melted at 1050 °C for 5 ÷ 10 

Results

The first crystallization peak at 571°C in DTA measurements (Fig. 1) was explained based on the Flynn–Wall–Ozawa method applied to Bi4Ge3O12 and by using a non-isothermal procedure. It was related to nanocrystallites of Bi4Ge3O12 with a disk-shape type [14]. However the presence of the second crystallization peak at 652 °C concludes on the existence of at least one additional crystalline phase, which is specifically stable in this range of temperatures.

The XRD results (Fig. 2) obtained on the

Discussions

Differential Thermal Analysis has shown two distinguished crystallization exothermic peaks between 550 °C and 700 °C going from a cubic to an orthorhombic structure. This fact involves a rearranging process of the GeO4 tetrahedra around Bi3+ ions which leads to a variation of the oxygen defects in the matrix. All of these processes influence the magnetic behaviour of the sample.

According to the mentioned XRD data, the sample annealed at 645 °C (close to the temperature of 652 °C of the second peak

Conclusions

Photoluminescence of BGO glass ceramic materials are closely connected to the oxygen vacancies, mainly in the GeO4 tetrahedra, during crystallization process. These oxygen vacancies can be correlated with BGO ferromagnetic properties inducing magnetization and exchange interactions. On the other hand, this crystallization process is connected to a critical temperature range in which two crystallographic structures coexists, resulting in different defect densities. In this temperature domain,

Acknowledgement

The authors acknowledge the financial contribution of UEFISCDI, Contract 45 N, Project PN09-450102 and of Project PN-II-PCE 75/2011.

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