NON-CARBON PREPARATION OF SILICON BY MECHANICALLY ACTIVATED THERMAL SYNTHESIS T.F. Grigorieva1, T.L. Talako2, A.I. Letsko2, V. Šepelák3, V.G. Scholz4, M.R. Sharafutdinov1, I.A. Vorsina1, A.P. Barinova1, P.A. Vitiaz2, N.Z. Lyakhov1 1 Institute of Solid State Chemistry and Mechanochemistry, Kutateladze str., 18, Novosibirsk, 630128, Russia. grig@solid.nsc.ru 2 Powder Metallurgy Institute, Platonov str., 41, Minsk 220005, Belarus 3 Inst. of Nanotechnology, KIT, Eggenstein-Leopoldshafen, 76344, Germany; 4 Inst. of Chemistry, Humboldt Univ. Berlin, 12489, Germany Introduction In industrial processes, the production of Si is based on the reduction of silicon dioxide by carbon at a temperature of about 1800 C. [1]. However, the coke applied to the reduction can be hardly refined from the most dangerous for silicon impurities like boron, phosphorus, arsenic and antimony. That is why development of non-carbon routes for silicon production is a topical problem of a silicon industry. Reduction of oxides with magnesium and aluminum by the method of selfpropagating high-temperature synthesis (SHS) has been used in industry for a long time [2]. As such reactions are highly exothermal, they can be also organized with the use of mechanochemistry, for instance, reduction of the copper oxide by aluminum. Mechanochemical reduction of iron oxide by aluminum, aimed at obtaining precursors with different compositions for intermetallide/oxide SHS composites, has been also considered [3–6]. SiO2 + Al reaction is not high exothermic enough to organize the SHS without preliminary heating [7]. Mansurov et al. [8] reported creation of ceramic composites in several stages: first, the silicon oxide was mechanochemically treated in an organic compound environment, then the resultant material was annealed (carbonized) at ~ 850 C, and finally the mixture of the carbonized silicon oxide with aluminum was subjected to SHS. However, as-formed product included silicon carbide. The objective of activities described in this paper is to study the possibility of using mechanochemical treatment for obtaining silicon/aluminum oxide composites by the SHS and thermal synthesis at considerably lower temperatures with the following removal of alumina. 53 Sample preparation and examination procedures The PA-4 aluminum powder and the silicon oxide with a particle size of ~ 3 nm were used in our experiments. A stoichiometric mixture of the silicon oxide with aluminum was processed in a high energy planetary ball mill (drum volume 250 cm3, ball diameter 5 mm, mass of the balls 200 g, mass of the sample 10 g, and velocity of rotation of the drums around a common axis ~1000 rpm). The IR spectra were recorded by a Specord IR 75 spectrometer; the samples for this study were pressed with annealed potassium bromide. The 27Al (I = 5/2) NMR spectra were recorded on a Bruker Advance 400 spectrometer corresponding to a 27Al resonance frequency of 78.2 MHz. MAS experiments were realized with a high speed probe using 2.5 mm zirconia rotor. The spinning speed was 20 KHz. The magnetic field strength (in frequency unit) was set to 104.262 MHz. The excitation pulse duration was chosen equal to 1 s. The recycling delay between each acquisition was fixed to 1 s. To see weak signals in the AlO region in mechanically activated samples, we applied accumulations numbers up to 56000 (i.e. measurement time of 15 hours). The dynamics of the SHS process was studied with the use of diffraction of synchrotron radiation and an OD-3 single-coordinate detector. The samples for SHS were prepared in the form of pellets 20 mm in diameter and 1–2 mm thick by pressing at a pressure of 200 atm. The resultant samples were placed onto a ceramic plate so that they were in the center of the goniometer. The process was initiated by a nichrome spiral. The OD-3 detector was triggered to operate in the “fast filming” mode simultaneously with the beginning of pellet burning. The time of one “frame” was 0.5 sec, and the number of “frames” was 128. The radiation wavelength was 1.527 Å. For investigation of mechanically activated thermal synthesis the samples were heated up to 650 C in the reaction chamber XRK 900 in air with a heating rate 10 /min. The OD-3 detector was also used for studying the process dynamics, though time of one “frame” was 1 min. 54 Results and discussion First, we made an attempt of direct mechanochemical reduction of the silicon oxide by aluminum. The study of this process showed that the chemical reaction of SiO2 reduction does not occur within 6 min of mechanical activation. The IR spectrum of the initial mixture contains clear absorption bands with the maximums at 1005 and 480 cm−1 (valence and deformation oscillations of the Si–O bond of the SiO4 tetrahedra of the silicon–oxygen skeleton) and two maximums in the range of 900–670 cm−1 due to oscillations of the Si–O–Si bridges. The phenomena observed in the course of mechanical activation were a gradual decrease in intensity and broadening of the characteristic bands of the Si–O bond (Fig. 1). Fig. 1. IR spectra of the SiO2 + Al mixture before mechanical activation (1) and after mechanical activation during 0.5 (2), 1 (3) and 6 (4) min Fig. 2. Microphotograph of the mechanocomposite after 1 min activation in Si characteristic radiation An electron-microscopy study of the SiO2/Al composite obtained after 1 min of mechanical activation in characteristic radiation revealed a 55 very small grain size and a very uniform distribution of the components in the mechanocomposite (Fig. 2). Based on the data of the differential thermal analysis (DTA), even short-time activation of this mixture appreciably affects its thermal characteristics. For the initial mixture, the real chemical interaction occurs at a temperature T > 1000 C (Tmax = 1083.6 C) (Fig. 3 a), i.e., substantially higher than the melting point of aluminum, whereas the situation is different for the mixture subjected to mechanical activation during 20 sec. Two clearly expressed exothermal peaks appear: the first peak at 621.7–648.6 C (Tmax = 632.7 C) and the second peak at 992.1– 1075.9 C (Tmax = 1029.2 C) (Fig. 3 b). For the mixture activated for 40 sec, the first peak is at 604.5–636.6 C (Tmax = 612 C), and the second peak is extremely broad and smeared in the range of 816.1–1111.7 C (Tmax = 1038.1 C). These observations can be explained by the fact that a tight contact is created between some part of the ultrafine non-plastic silicon oxide and plastic aluminum already within 20 sec of mechanical activation; the silicon oxide is “wetted” by aluminum; as a result, some part of the silicon oxide starts to interact with aluminum at a temperature T = 621.7C, which is lower than the melting point of the latter. As mechanical activation is continued, aluminum becomes also dispersed to nanoparticles, greater amounts of the components of the mixture are involved into the contact, and the temperature of the interaction beginning decreases: after 1 minute of activation, the interaction begins at T = 539.9 C and ends at T = 630.3 C (Fig. 3 c). The curve for this sample obtained by the method of differential scanning calorimetry (DSC) has only one exothermal peak, i.e., the entire process proceeds at a temperature lower than the melting point of aluminum. Longer activation further decreases the temperature of reaction beginning (Table 1), but there are no any further significant changes in the system parameters determined by DSC. The duration of mechanochemical treatment was limited to 6 min for the following reasons: - the IR spectra are so smeared already after 4 min that do not provide any new information (see Fig. 1); - the DTA study does not reveal any significant changes in the thermal characteristics after 1 min of mechanical activation (see Table 1); 56 - mechanochemical actions should be always minimized to ensure the minimum possible contamination of the products by milling. Fig. 3. Results of differential scanning calorimetry (DSC) and thermogravimetry (TG) studies of the SiO2 + Al mixture before (a) and after mechanical activation during 20 (b) and 60 sec (c). 57 Table 1. Parameters of Exothermal Peaks on DTA Curves of SiO2 + Al Samples after Mechanical Activation Temperature, C Duration of activation 1 min beginning of the reaction 593.0 2 min 587.1 624.3 4 min 586.7 629.1 6 min 587.0 625.8 27 end of the reaction 630.3 Al MAS NMR spectra of the nanostructured SiO2/Al mechanocomposites are dominated by a broad resonance associated with the presence of nanostructured Al matrix (Fig. 4). The interesting observation is that additional resonance lines appear in the spectra of mechanoactivated samples corresponding to AlO4, AlO5 and AlO6 polyhedra. Their content is slightly increasing with increasing milling time, however, the relative intensity of AlOx polyhedra compared with the Al matrix spectral intensity is even after the longest milling period very low. It can be assumed that these nonequilibrium local coordinations of aluminium atoms are located on the SiO2-Al interfaces [9]. The intensity of the resonance lines belonging to various polyhedra relative to the total spectral intensity allows us to calculate the volume fraction of interface regions in the nanocomposites. Furthermore, assuming a spherical shape of SiO2 nanoparticles, the thicknees of the interface regions was calculated their known volume fraction. Thus, the study of mechanically activated SiO2+Al mixtures shows that silicon reduction does not occur during mechanical activation step except formation of some AlOx species at the interfaces, but an exothermal reaction in activated mixtures can proceed at substantially lower temperatures. In the subsequent step, the nanostructured SiO2/Al mechanocomposites were used as precursors for the preparation of Si/Al2O3 composites via self-propagating high-temperature synthesis. Our experience shows that combustion initiation requires sample 58 preheating approximately to 200 C (as compared with 650-860 С reported in [7]). Fig. 4. 27 Al MAS NMR spectra of non-activated sample (a), the sample mechanoactivated for 1 (b) and 6 (c) minutes. 59 The overall pattern of phase transformations is illustrated in Fig. 5 a. To analyze them, however, it is more convenient to use the projection onto the diffraction angle (β)–time plane (Fig. 5 b). As the silicon oxide used in these experiments is amorphous to x-ray radiation, only aluminum peaks are observed. Fig. 5. Dynamics of phase transformations in the Al + SiO2 mechanocomposite 60 image; (b) projection onto the in the SHS mode: (a) three-dimensional diffraction angle–time plane. It is clearly seen that aluminum becomes heated as the combustion wave approaches: the peaks are shifted toward smaller angles, i.e., greater distances between the planes. After that, the intensity of these peaks drastically decreases, which is apparently due to melting. No crystalline phases are observed in the two frames (~ 1 sec). In our opinion, corundum (Al2O3) peaks appear slightly earlier than silicon Fig. 6. Microphotograph of the SHS product in Si characteristic radiation. peaks. A possible reason is the lower melting point of silicon (1410 C), as compared with corundum (2050 C). An electronmicroscopic study of the SHS product of the SiO2 + Al system subjected to mechanical activation during 1 min in characteristic radiation (Fig. 6) shows a fairly uniform distribution and small size of all elements in the system, including silicon being formed. Previously, it was shown that chemical interaction between SiO2 and Al in the mechanocomposites formed during the mechanical activation starts at essentially (~ 500 C) lower temperatures as compared with the non-activated mixtures. In the final step, we used as-formed mechanocomposites as precursors for the preparation of Si/Al2O3 composites via thermal synthesis. The samples after mechanical activation for 6 min were placed into cuvette and gently prepressed to get the plane surface. Then the cuvette with the sample was sited in the furnace. The thermocouple was directly close to the registration area. Recording of diffractograms was started at temperature 230 С. Dynamics of phase transformation in Al / SiO2 composites during heating from 590 up to 660 C is presented in Fig.7. 61 Fig. 7. Dynamics of phase transformation in Al / SiO2 composites during heating from 590 up to 660 C. Fig. 8 XRD-pattern of the thermal synthesis product from the mechanocomposites activated for 6 min and heated up to 660 C. As can be seen from the Fig. 7, the reaction products (silicon and alumina) start to form at about 590 С. It is interesting, that corundum is formed during the SHS and thermal synthesis after low activation time, 62 while -Al2O3 is identified in the product of thermal synthesis after longer MA durations (Fig. 8). Conclusions Thus, though the silicon oxide is not reduced by aluminum directly by mechanical activation, the use of the mechanocomposite as a precursor for both SHS and thermal synthesis allows a fine-grain silicon/aluminum oxide composite to be obtained. In both cases chemical interaction starts at essentially lower temperatures as compared with the non-activated mixtures. Acknowledgements This work was supported by the joint project No. 5 “Non-carbon preparation of Si by mechanically activated thermal synthesis” of NASB and SB RAS. References 1. Denisov V.M, Istomin S.A., Podkopaev O.I, Serebrjakova L.I., Pastuchov E.A., Beletsky V.V. Silicon and its alloys. Ekaterinburg: Publishing house of Ural Branch of the Russian Academy of Sciences, 2005. 467 p (in Russian). 2. A.G. Merzhanov, Forty Years of SHS: Happy Life of a Scientific Discovery (in Russian), Chernogolovka (2007). 3. T.F. Grigoryeva, S.A. Petrova, I.A. Vorsina, et al., “Mechanochemical reduction of a copper oxide,” in: The Optimization of the Composition, Structure and Properties of Metals, Oxides, Composites, Nano and Amorphous Materials, Proc. 6th Israeli–Russian Bi-National Workshop, Jerusalem (2007), pp. 197–204. 4. T.F. Grigoryeva, T.L. Talako, A.A. Novakova, et al., “MA and MA SHS production of nanocomposites metal/oxides and intermetallics/oxides,” ibid., pp. 139–148. 5. N.Z. Lyakhov, P.A. Vityaz, T.F. Grigorieva, et al., “Mechanochemically synthesized SHS precursors for obtaining intermetallide/oxide nanocomposites,” Dokl. Akad. Nauk, 406, No. 6, 776–778 (2005). 63 6. 5. T. Talaka, T. Grigorieva, P. Vitiaz, et al., “Structure peculiarities of nanocomposite powder Fe40Al/Al2O3 produced by MA SHS,” Mater. Sci. Forum, 534–536, 1421–1424 (2007). 7. Maltsev V.M.; Gafiyatulina G.P.; Tavrov A.V. Spreading of the combustion wave in SiO2-Al systems // Proc. SPIE Vol. 3172 (11/1997), p. 724-727. 8. Z.A. Mansurov, R.G. Abdulkarimova, N.N. Mofa, et al., “SHS of composite ceramics from mechanochemically treated and thermally carbonized SiO2 powders,” Int. J. SHS, 16, No. 4, 213–217 (2007). 9. V. Sreeja, T.S. Smitha, Deepak N., Ajithkumar T.G. and P.A. Joy. Size dependent coordination behavior and cation distribution in MgAl2O4 nanoparticles from 27 Al solid state NMR studies. J. Phys. Chem., C 112, 14737-14744 (2008) 64