STUDIA UNIVERSITATIS BABES-BOLYAI, PHYSICA, SPECIAL ISSUE, 2003 SILICA-LIME-PHOSPHATE VITROCERAMICS WITH IRON D. Eniu1 and S. Simon2 1 University of Medicine and Pharmacy, Faculty of Pharmacy, 3400 Cluj- Napoca, Romania 2 Babes-Bolyai University, Faculty of Physics, 3400 ClujNapoca, Romania Abstract Glass transition and crystallisation temperatures determined from thermal analyses indicate the structural evolution of samples in function of composition. The glass stability is enhanced by Fe2O3 addition to silicalime-phosphate host glass up to 20 mol %. Electron paramagnetic resonance and magnetic susceptibility results inform on the surrounding and magnetic interactions between iron ions. The Fe3+-EPR data indicate that the size of ferromagnetic particles increases after heat treatment and their surroundings become more ordonated due to the partial crystallisation of samples. The magnetic susceptibility increases by heat treatment and depends on the treatment temperature. 1. Introduction The use of calcium phosphate glasses and glass ceramics as bone substitutes has become common in orthopedic surgery [1]. Ferromagnetic calcium phosphate glass ceramics are successfully applied to reinforce the bone and to decrease the recurrence of tumors by hyperthermic treatment [2]. In this samples is essential the development of ferromagnetic crystallites in iron reach phases. The aim of this paper is to evidence the structural effects caused by iron addition to calcium-silica-phosphate glasses, the vicinity and magnetic interactions of iron ions of CaO-P2O5-SiO2-Fe2O3 glass and glass ceramic samples. 2. Experimental The starting materials used to obtain 45(3.34 CaOP2O5)(55-x)SiO2xFe2O3 glasses were CaCO3, CaHPO42H2O, SiO2 and Fe2O3 of reagent grade purity. The oxide mixtures corresponding to the desired compositions (0 x 30 mol %) were melted in corundum crucibles at 1550oC for 10 minutes in an electric furnace Carbolite type RHF 1600, in air, under normal conditions. The melts were quickly undercooled by pouring onto stainless steel plates at room temperature. Specimens of the glass samples were heat treated with a rate of 4 oC/min from the room temperature to 1000, 1100 and 1200oC in air. They were maintained at the treatment temperature for 30 minutes and then were slowly cooled in the furnace down to the room temperature. D. ENIU AND S. SIMON The electron paramagnetic resonance (EPR) spectra were recorded on a 300 ESP Bruker spectrometer, in X band, at room temperature on powder samples. The magnetic susceptibility was measured between 80K and 300K with a 10 -8 emu/g sensitivity Faraday-type magnetic balance. Thermal analysis measurements were carried out using a MOM derivatograph with a rate of 10oC/min. 3. Results and discussion The structural evolution of samples in function of composition was first checked by determining the glass transition and crystallisation temperatures from differential thermal analyses. The data obtained show that the glass transition temperature, T g, increases by addition of iron to the calcium-silica-phosphate matrix up to 20 mol % (Fig. 1). One observes that glass transition temperatures are very close for the sample without iron and that with lowest iron content, while Tg has the same value for the samples with 20 and 30 mol % Fe2O3 contents. o Tg ( C) With respect to glass stability, expressed by the difference between the crystallization temperature and glass transition temperature, it was found an increase up to x = 20 Fe2O3 mol %. The local atomic order and the valence state of iron in oxide glass matrices play a major role in determining 400 the physical properties of glasses, inclusively their 390 capability to aggregate in clusters [3]. For glass 380 compounds used as precursor materials of 370 ferromagnetic biomaterials with applications in 360 hyperthermic treatments the iron atoms segregation 350 in clusters is very 0 5 10 15 20 25 30 important. Both cluster x (mol %) size and sample magnetic Fig. 1 The composition dependence of glass susceptibility are to be transition temperature. enlarged in view of this therapy. The EPR spectra of the investigated samples consist in a large, relatively symmetric line. This feature is specific to disordered oxide systems with high Fe2O3 content wherein spherical ferromagnetic monodomain particles are formed [4], most probably magnetite particles. The resonance line at g ≈ 2.0 is shifted to 2 SILICA-LIME-PHOSPHATE VITROCERAMICS WITH IRON lower values of the magnetic field when the iron oxide content increases. This result could be assigned to the occurrence of ferromagnetic multidomain particles in the samples with higher Fe2O3 content. The width of g ≈ 2.0 line increases with Fe2O3 content from 830 Gs, for x =10, to 2780 Gs, for x = 30, and suggests that the Intensity (a.u.) (a) Fig. 2 EPR spectra of (a) glass ceramic and (b) glass samples. (b) 0 1000 2000 3000 4000 5000 6000 7000 B (G) size of ferromagnetic particles are distributed on a relative large values range, but on the other hand they are small enough to be not detected by X-ray diffraction analyse. The size of these particles and the local order are increased by the crystallisation heat treatment. This is also reflected by EPR spectra evolution as can be seen from Figure 2. The spectrum of the heat treated sample contains beside the line typical of untreated glass sample an additional narrow line (B = 195 G) arising from Fe3+ ions disposed in the crystalline phase well developed during the applied heat treatment. The highest local concentration for iron inside the samples was obtained from ESCA measurements [5] for the glass ceramic resulting by the treatment applied at 1000oC. The magnetic susceptibility, , increases by heat treatment, e.g. for the sample with x = 10 mol %, at room temperature, increases from 35 to 150 (10-3 emu/mol). The temperature dependence of the reciprocal magnetic susceptibility for this composition is illustrated in Figure 3. The magnetic susceptibility reaches the largest value after the heat treatment applied at 11000C. Both SiO2 and P2O5 are glass formers. Pure vitreous SiO2 and P2O5 consist in a continuos random network of quasi-tetrahedral SiO4 and PO4 units wherein silicon, 3 D. ENIU AND S. SIMON respectively phosphorous is four coordinated. In these glasses CaO and Fe 2O3 act as glass network modifiers. Fig. 2 Temperature dependence of reciprocal susceptibility for 45(3.34 45(3.34 CaOP2O5)45SiO210Fe2O3 samples heat treated at different temperatures: untreated (■), 10000C (●),11000C (▲,▽),12000C (▼). The thermal diffusivity of these samples has a good stability in the temperature range including the interval of interest for therapy by hyperthermia [6]. 4. Conclusion The glass stability is enhanced by Fe2O3 addition to silica-lime-phosphate host glass up to 20 mol %. With increasing Fe2O3 content the samples contain beside monodomain also multidomain ferromagnetic particles. The size of these particles increases and their local structure becomes more ordonated in vitroceramic samples obtained by heat treatment. The magnetic susceptibility rises up to five times in the partially cristallised samples. References 1. A.D up r az, T .P .N g u ye n, M. Ric h ard , G.D ac ul s i, N.P a ss u ti , Biomaterials, 20, 663 (1999) 2. M.B ab i n ko v a, D. Le sz cz yn s k a, P . So ur i vo n g, P . C ic ma n ec, P .B ab i ne c , J. Magn. Magn. Mater, 225, 109 (2001) 3. F.D ’ Ac ap i to , S.Mo b il i o , J .R. R e g nard , E. Ca ttar u zza , F .Go ne ll a, P .Mazzo ld i , J. NonCryst. Solids, 232-234, 364 (1998) 4. D. L. Gr i sco m, J. Non-Cryst. Solids, 67, 81 (1984) 5. V.S i mo n, S. G. C hi zb ai a n , M.N e u ma n n, D. E ni u, E .Ind r ea, A.T o ro k Ki s s, S.S i mo n, Mod. Phys. Lett. B., 14, 21, p.767 (2000) 6. S. Si mo n, D .E ni u, A. P asca , D.D ad arl at, V .S i mo n, Mod.Phys.Lett.B, 15, 21, 921 (2001). 4