Original scientific paper Informacije ^efMIDEM A Innrnal of Journal of Microelectronics, Electronic Components and Materials Vol. 44, No. 1 (2014), 25 - 31 Compositional and Microstructural Study of Sol-Gel-Derived PbZr^. ^O^/Al^O^/SiO^/Si Thin-Film Structures Evgeniya Khomyakova1,2, Andreja Benčan1, Barbara Malič1 ^Jožef Stefan Institute, Electronic Ceramics Department, Ljubljana, Slovenia 2Jožef Stefan International Postgraduate School, Ljubljana, Slovenia Abstract: In this work we discuss the results of compositional and microstructural analyses of PbZr03Ti07O3/Al2O3/SiO2/Si thin-film structures. The PbZr03Ti07O3 (PZT) and Al2O3 thin films were prepared by the alkoxide-based sol-gel method. A dense, nanocrystalline, 20-nm-thick, Y-alumina layer was formed on the silicon substrate after annealing at 900°C for 1 hour. On top of this alumina layer, a PZT film with a <100> orientation of the tetragonal perovskite phase, about 300-nm-thick, was obtained after annealing at 550°C. The alumina layer did not completely prevent the diffusion of lead oxide from the PZT to the Si substrate. An additional Al-Si-Pb-O amorphous layer with a maximum thickness of 10 nm was observed between the Al2O3 and SiO2 layers. This work is dedicated to the late Professor Marija Kosec Keywords: PZT thin films, interface reactions, SEM, TEM Fazna in mikrostrukturna analiza tankoplastnih struktur PbZr0.^Ti^0. ^O^/Al^O^/ SiO2/Si, pripravljenih s sol-gel sintezo Izvleček: V delu so predstavljeni rezultati fazne in mikrostrukturne analize tankoplastnih struktur PbZr03Ti07O3/Al2O3/SiO2/Si. Z alkoksidno sol-gel sintezo smo pripravili tanke plasti s sestavo PbZr03Ti07O3 (PZT) in Al2O3 na silicijevi podlagi. Po segrevanju na 900°C, 1 uro smo uspeli pripraviti gosto, 20 nm tanko plast Y-aluminijevega oksida na silicijevi podlagi. Na površino omenjenega aluminijevega oksida smo nanesli 300 nm tanko plast PZT, ki ima po segrevanju pri 550°C tetragonalno simetrijo in je orientirana v smeri <100>. Tanek sloj aluminijevega oksida ni popolnoma preprečil difuzije svinčevega oksida iz PZT v silicijevo podlago. Med Al2O3 in SiO2 smo opazili dodatno, 10 nm amorfno plast Al-Si-Pb-O. Ključne besede: Tanke plasti PZT, reakcije med plastmi, SEM, TEM ' Corresponding Author's e-mail: evgeniya.khomyakova@ijs.si 1 Introduction A lead-zirconate-titanate solid solution, with a composition close to the morphotropic phase boundary, is used in many multilayered structures due to its outstanding piezoelectric and ferroelectric properties. However, in order to obtain a stronger piezoelectric response, in-terdigitated electrodes (IDEs) have been introduced to replace the traditional parallel-plate electrode configuration, for example in energy-harvesting applications. [1,2] However, an IDE system requires a direct contact between the active film and the substrate. The direct integration of the piezoelectric Pb(Zr,Ti)O3 layer on the silicon substrate leads to the formation of lead-silicate glass phases, which are not piezoelectric.[3] In order to prevent these undesired reactions, many materials were studied as barrier layers, such as Al2O3[4,5,6], Ba(Mg1/3Ta2/3)O3[7], MgAl2O4[8] and Ir.[9] Alumina is a very good candidate for this barrier layer due to its chemical and thermal stability. Thin alumina layers, as a barrier layer between the Pb(Zr052Ti048)O3 and Si substrate, were prepared by a sol-gel route[4], by chemical vapor deposition (CVD)[5,6] or by a com- bination of the two, i.e., the sol-gel and the CVD methods.[10] Depending on the method used and the heat-treatment conditions, amorphous or crystalline alumina was obtained.[4,5,6] For example, a pure crystalline alumina layer was obtained after annealing at 750°C for 30 min using the sol-gel method[4], and at 1000°C using the CVD method.[5,6] In addition, by using the CVD method, <001> or <111> oriented alumina films can also be grown on the silicon.[5] Later, four layers of PbZr03T07O3 solution were deposited on an Al2O3/SiO2/Si substrate (3000 rpm, 30 sec), with each deposition being followed by 2 min. of drying at 200°C and 2 min. of pyrolysis at 350°C. After the deposition of each second PbZr03T07O3 layer (subsequently denoted as the PZT layer) tli.^ F3ZT/Al2O3/SiO2/ Si structure was exposed to rapid thermal annealing at 550°C for 15 min in air. The heat-treatment conditions were defined according to Malič et al.[12] However, despite the fact that there are a number of articles about the influence of the alumina layer on the functional properties of Pb(Zr,Ti)O3 films, any detailed structural characterization of these multilayered thin-film structures is usually missing. The thermal decomposition of the aluminum precursor solution, dried at 60°C, was followed by thermogravim-etry and differential thermal analysis (TG/DTA, Netzsch STA 409), using a heating rate of 10°C/min. in a Pt crucible and an atmosphere of air. In this work we used the sol-gel route in order to prepare a PbZr0.3Ti0.7O3/Al2O3/SiO2/Si thin-film structure. The aim of the work was, first, to analyze the phase composition and the microstructure of the alumina layer and, second, to evaluate the chemical compatibility between the alumina and the PbZr03Ti07O3 film. The analyses from the micro- to the nano-level were performed by X-ray diffraction and analytical microscopy methods. The phases of the thin-film structures were determine with an X-Ray diffractometer (CuKa radiation, Philips PW 1710) in the range 2e=10°-65° using a step of 0.034° per 100 seconds. Prior to the scanning electron microscope (SEM) and focused ion beam (FIB) microscope analyses the samples were coated with carbon in a sputter coater (SCD 050, BALTEC) to prevent charging and to provide electrical conductivity. 2 Experimental An alumina precursor solution with a concentration of 0.25 M was prepared in a dry atmosphere by dissolving aluminum sec-butoxide, (Al(O-secC4H9)3, Aldrich) in 2-methoxyethanol (CH3-O-CH2-CH2-OH (2-MOE), Alfa Aesar). The solution was then intensively stirred in a dry box for 1 hour. A precursor solution with the composition PbZr03Ti07O3 and 10% excess of PbO was prepared in an atmosphere of dry nitrogen by mixing dehydrated lead acetate (Pb(OAc)2, Alfa Aesar) titanium iso-propoxide (Ti(O-iC3H7)4, Alfa Aesar) and zirconium iso-propoxide (Zr(O-iC3H7)4, Alfa Aesar) in 2-MOE. After the mixing, the solution was refluxed for 2 hours and distilled to reach a concentration of ~0.5 M. After cooling to room temperature, 4 vol.% of formamide (HCONH2, Alfa Aesar) was added to the solution. A detailed description of the Pb(Zr,Ti)O3 solution's preparation can be found in.[11] A thin alumina film was prepared by spin-coating (3000 rpm, 30 sec) the precursor solution on the SiO2/ Si substrate. Four layers of solution were deposited; after which each layer was dried for 5 min. at 200°C and given 5 min. of pyrolysis at 350°C. After the fourth layer, the thin-film Al2O3/SiO2/Si structure was annealed at 900°C for one hour with a heating rate of ~14°C/min. For the transmission electron microscopy (TEM) cross-section observations the thin-film samples were cut into pieces with a wire-saw, after which two pieces were glued together, head-to-head, with highly dispersed epoxy glue, and then glued into a copper ring. After the hardening of the glue, the thickness of the sample was mechanically reduced by grinding from 1 mm to ~100 ^m. The sample was then dimpled from one side to a final thickness of ~20 ^m. Finally, thin disks were exposed to an ion-milling procedure with 3.5-keV argon ions using a precision ion polishing system (PIPS, Gatan, Model 691). The areas adjacent to the specimen hole were used for the TEM observation. The thin-film structures were characterized using a field-emission SEM (FE-SEM, Jeol JSM-7600F), a FIB microscope (FIB, Helios Nanolab 650, FEI) equipped with an INCA X-ray energy dispersive spectrometer (Oxford Instruments), a transmission analytical electron microscope (TEM, Jeol JEM-2100) and a high-resolution TEM (TEM, Jeol JEM-2010F) equipped with an Oxford LINK ISIS 300 energy-dispersive X-ray spectrometer (EDXS). 3 Results and discussion 3.1 Preparation and characterization of the alumina thin film on the SiO^Si substrate In order to define the annealing conditions, a thermal analysis of the dried starting aluminum alkoxide solution was performed. The obtained TG and DTA curves are presented in Figure 1. During heating from room temperature to ~500°C the sample loses 50% of its mass, above 500°C no significant mass loss is observed. The mass loss is accompanied by an endothermic peak at ~140°C, which can be related to the evaporation of water and residual solvent, and the exothermic peak at ~310°C, which can be attributed to the decomposition of organic species.[13] The DTA curve shows two additional exothermic peaks at ~870°C and ~1110°C. Figure 1: TG/DTA curves of aluminum alkoxide solution performed from 20°C to 1400°C. The exothermic peak at 870°C could be related to the crystallization of the cubic Y-alumina from the amorphous gel. According to Bahlawane et al.[14] the Y-alumina crystalizes in the 850-900°C temperature range when using aluminum alkoxide as a precursor. The exothermic peak at 1100°C could be related to the growth of the Y-alumina crystals, which is an exothermic process. However, let us note that at the same temperature, above 1100°C, the alumina also transforms to the rhombohedral a-alumina. Most probably in our case these two effects overlap. Based on the TG/DTA analysis, the dried aluminum precursor was annealed at 900°C for 1 hour, and, in order to characterize the obtained powder, XRD and TEM analyses were performed. An XRD pattern and a TEM bright-field image are shown in Figure 2. Figure 2(a) shows that all the peaks in the XRD pattern can be indexed by y-alumina with a defect cubic spinel structure (PDF#80-1385). The peaks are very broad, indicating that the powder is poorly crystallized. The bright-field TEM image (Figure 2(b)) shows a few-nm-sized Al2O3 powder. According to the SAED analysis (Figure 2(b)) the Al2O3 nano-crystals have a cubic symmetry; this result is in agreement with the XRD data. (a) (b) Figure 2: XRD pattern (a) and TEM image (bright field) (b) of Al2O3, after calcination at 900°C for 1 hour. The diffraction rings (inset of image b) were indexed with the cubic Al2O3 (PDF#80-1385) In accordance with these results, four layers of aluminum alkoxide solution were spin coated on the SiO2/Si substrate and annealed for 1 hour at 900°C. The cross-section SEM micrograph of the prepared Al2O3/ SiO2/Si structure is shown in Figure 3(a). In order to determine the chemical composition a qualitative SEM-EDXS line analysis was performed across all the layers in the Al2O3/SiO2/Si structure. (Figure 3(b)). The surface of the upper layer is dense; the layer consists of a few-nm-sized grains. The SEM-EDXS analysis confirmed the presence of an upper Al2O3 layer on the SiO2/Si substrate. However, the concentration profile of the Si shows that a small amount of Si was also detect- ed within the A\2O3 layer, which can be related to the small spatial resolution of the EDXS analysis. Namely, when using a lower energy (below 10 keV) the information is coming from a depth of approximately 100-200 nm[15], i.e., greater than the thickness of the alumina layer, which is a few tens of nm. Therefore, besides the Al, a Si signal can also be detected. We should note that according to the SiO2-Al2O3 diagram, different alumo-silicates can be formed;[16] however, in the case of a thin, crystalline, alumina film on the silicon substrate, no silicon diffusion was reported in the literature. [4,5,6,10] try. The results are in accordance with the XRD analysis performed on sol-gel-derived Al2O3 powder (Figure 2). (a) (b) Figure 3: Cross-section SEM micrograph of the Al2O3/ SiO2/Si structure, after annealing at 900°C for 1 hour (a). The EDS line analysis across the Al2O3, SiO2 and Si for Si, O and Al, performed at 5 keV (b). The cross-section and imaging were performed with the FIB microscope. In order to analyze the Al2O3 film on the nanometer scale, the Al2O3/SiO2/Si structure was investigated by TEM. In Figure 4, a cross-section TEM micrograph of a ~20-nm-thick Al2O3 film on a SiO2/Si substrate is presented. The film consists of a few-nm-sized Al2O3 grains, as already observed by SEM analysis. According to the SAED analysis, the alumina grains have a cubic symme- Figure 4: Cross-section TEM micrograph (bright field) of a polycrystalline Al2O3 thin film on a SiO2/Si substrate, after firing at 900°C for 1 hour with the corresponding SAED patterns. The diffraction rings were indexed with the cubic Al2O3 (PDF#80-1385) According to the SEM and TEM results, we can conclude that a continuous, dense, crystalline ~20-nm-thick layer of aluminum oxide on the silicon substrate was formed after annealing at 900°C. 3.2 Characterization of the PbZr^. JTi^.^O^/Al^O^/ SiO2/Si structure In the next step, the PbZr03Ti07O3 solution was spin coated on the Al2O3/SiO2/Si substrate and the film was annealed two times, i.e., after the second and the fourth depositions of the solution, at 550°C for 15 min. A cross-section SEM micrograph of the PbZr03Ti07O3/ Al2O3/SiO2/Si structure is shown in Figure 5(a); the surface of the upper PZT layer is shown in Figure 5(b). The PZT film on the Al2O3/SiO2/Si substrate is ~300-nm-thick and the thickness is uniform within the investigated range. It consists of a few-hundred-nm-sized, irregularly shaped grains. In the surface microstructure, the boundaries between the grains are clearly visible. Besides larger PZT grains, some small, white, round inclusions of a lead-rich secondary phase are also seen at the PZT grain boundaries. A similar microstructure for a PZT thin film on a platinized silicon substrate was observed by Kosec et al.[17] The authors explained that up to 4-^m-sized grains of PZT are formed due to the small number of nucleation sites.[17] The PbO secondary phase at the PZT surface was also observed by Bur-sill et al.[18] In Figure 6, the X-ray powder-diffraction pattern of the PbZr03Ti07O3/Al2O3/SiO2/Si structure is shown. High-in- (a) Figure 5: SEM-BE micrographs of the PbZr03Ti07O3/ Al2O3/SiO2/Si structure (a), the surface of the PZZiT liay^r on the Al2O3/SiO2/Si substrate (b), after annealing at 550°C. tensity peaks marked with hkl indices can be ascribed to the randomly oriented perovskite PZT phase with the tetragonal symmetry; however, no {00l} reflections were detected. Evidently, the PZT film is a-axis oriented, which in other words means that the c-axis of the PZT unit cell is parallel with the Al2O3/SiO2/Si substrate. Such an orientation of the Pb(Zr,Ti)O3 film on the silicon substrate is a consequence of the tensile stresses within the multilayered structure that develop during cool-ing.[19,20] A low-intensity reflection at 20=29°, which could be ascribed to PbO, was also observed. The XRD results are in accordance with the SEM analysis, where besides the larger perovskite PZT grains, smaller round inclusions of lead oxide at the grain boundaries between the PZT grains were observed (see Figure 5). 2-theta ( Figure 6: XRD pattern of the PbZr0.3Ti0.aO3/Al2O3/SiO2/Si structure after annealing at 550°C. Peaks belonging to the tetragonal PbZr03Ti0aO3 perovskite phase (ICSD 90473) are marked with hkl, the peak belonging to the silicon substrate (PDF 01-072-1088) is marked with Si, the peak marked with P could be indexed with the or-thorhombic PbO (PDF 01-072-0094). thick PZT layer is observed on the top of the thin poly-crystalline alumina layer with a uniform thickness. The PZT layer consists of ~300-nm-sized grains. Small pores are visible within the PZT layer. The SAED pattern of the PZT grain, shown in Figure 7(b), was indexed with the tetragonal PbZr03Ti07O3 unit cell (a, b=3.978 Ä and c=4.148 Ä, SG: P4mnn, ICSD #90473). According to the diffraction pattern the PZT grain is oriented in the <001> zone axis. The c-axis of the perovskite grain is perpendicular to the observed plane, i.e., it is parallel to the Al2O3/SiO2/Si substrate. The result is in accordance with the XRD data, where an a-axis-oriented PZT film was observed (Figure 6). However, a closer look at the structure (Figure 7(c)) shows that an intermediate layer of amorphous secondary phase is formed between the alumina and the SiO2. A maximum thickness of the secondary phase is around 10 nm. In order to determine the chemical composition of the secondary phase, a TEM-EDXS analysis was performed through all the layers, as shown in Figure 8. According to the EDXS analysis, the intermediate layer below the Al2O3 contains Al, Si, O and Pb, indicating that PbO diffused through the alumina layer towards the substrate. In the PZT and alumina concentration profiles, silicon is also present, most probably due to the sputtering of silicon during the preparation of the TEM sample. In order to analyze the PbZr03Ti0 7O3/Al2O3/SiO2/Si structure at the nano level the TEM analysis was performed (Figure 7(a)). An enlarged view of the PZT layer is shown in Figure 7(b) and the boundaries between the PZT-Al2O3-SiO2 layers in Figure 7(c). A dense, ~300-nm- To conclude, although the nanosized Al-Si-Pb-O-con-taining amorphous phase was formed below the alumina layer, no lead-deficient pyrochlore phase was observed in the PZT film. Presumably, the small amount of diffusion of PbO from the PZT to the Si was compen- (a) (c) Figure 7: Cross-section TEM micrographs (bright-field) of PbZr03Ti07O3/Al2O3/SiO2/Si structure (a), enlarged view of the PZT layer with SAED of the tetragonal perovskite PZT grain in the <100> zone axis (b) and the boundaries between the SiO2, Al2O3, and PZT layers (c). Figure 8: TEM - EDXS patterns obtained from the PbZr03Ti07O3/Al2O3/SiO2/Si structure. Inset: On the HR-TEM image the regions where the analyses were performed are marked. 4 Conclusions A dense, nanocrystalline layer of Y-alumina oxide was successfully synthesized on a silicon substrate using the sol-gel method. After the deposition and annealing at 900°C for 1 hour an ~20-nm-thick alumina layer was obtained, and investigated as a buffer layer between the PbZr0.3Ti0.7O3 (PZT) layer and the silicon substrate. An a-axis-oriented tetragonal PZT film was obtained on the Al2O3/SiO2/Si substrate after annealing at 550°C. The PZT layyer is ~300-nm-thick and consists of ~300-nm-sized grains. According to the TEM-EDXS analysis, an additional, up to 10 nm, Al-Si-Pb-O phase was observed below the alumina layer, indicating that a minor diffusion of lead oxide through the alumina layer into the silicon took place during the annealing at 550°C. 5 Acknowledgment This work was supported by the Slovenian Research Agency PR-05024. The authors would like to thank Jena Cilenšek, Silvo Drnovšek, Brigita Kmet and Goran Dra-zic for support in the experimental work. Authors also acknowledge the Center of Excellence Nanoscience and Nanotechnology for access to the FIB. sated with an excess of PbO used in the starting precursors. It seems that the alumina layer is not thick enough (~20 nm) to prevent lead oxide diffusion from the PZT towards the Si substrate completely, and thus, a thicker alumina layer would be needed. 6 References 1. N. Chidambaram, A. Mazzalai, P. Muralt. Measurement of effective piezoelectric coefficients of PZT thin films for energy harvesting application with interdigitated electrodes. IEEE Transactions on Ul- trasonics, Ferroelectrics, and Frequency Control. 59 (2012) 1624-1631; 2. Y.B. Jeon, R. Sood, J. Jeong, S.G. Kim. MEMS power generator with transverse mode thin film PZT. Sens. Actuators A. 122 (2005) 16-22; 3. Y. Shichi, S. Tanimoto. T. Goto, K. Kuroiwa, Y. Tarui. Interaction of PbTiO3 films with Si substrate. Jpn. J. Appl. Phys. 33 (19943) 5172-5177; 4. S.-H. Kim, C.-E. Kim, Y.-J. Oh. Influence ofAlJO^ diffusion barrier and PbTiO3 seed layer on microstructur-al and ferroelectric characteristics of PZT thin films by sol-gel spin coating method. Thin Solid Films. 305 (1997) 321-326; 5. D. Akai, M. Yokawa, K. Hirabayashi, K. Matsushita, K. Sawada, M. Ishida. Ferroelectric properties of solgel delivered epitaxial PbZ^T^.O^ thin films on Si using epitaxial g-Al2O3 layers. Appl. Phys. Lett. 86 (2005) 202906; 6. D. Akai, K. Sawada, M. Ishida. Fabrication of Pb(Zr,Ti)O3 films on epitaxial gamma-Al2O3(001)/ SifCCl) substrates. Journal of Crystal Growth. 259 (2003) 90-94; 7. Y.-H. Chu, Ch.-W. Liang, S.-J. Lin, K.-Sh. Liu, I-N. Lin. Low-temperature deposition of Pb(Zr,Ti)O3 thin films on Si substrates using Ba(Mg13Ta2^3)O3 as buffer layer. Jpn. J. Appl. Phys. 43 (200-4) 5-409-5413; 8. Sh. Matsubara, S. Miura, Y. Miyasaka, N. Shohata. Preparation of epitaxial ABO3 perovskite-type oxide thin films on a (100) MgAlJO/Si substrate. J. Appl. Phys. 66 (1989) 5826-583^; 9. L. Trupina, C. Miclea, C. Tanasoiu, L. Amarande, C. T. Miclea, M. Cioangher. Iridium layer as oxygen barrier and growth substrate for oriented PZT thin films. J. Optoelec. Advan. Mat. 9 (2007) 1508-1510; 10. A. Chin, M.Y. Yang, C.L. Sun, S.Y. Chen. Stack gate PZT/Al2O3 one transistor ferroelectric memory. IEEE Elect. DD ev. Lett. 22 (2001) 336-338; 11. M. Kosec, B. Malic, J. Holc, M. Hrovat, M. Mandeljc, A. Bencan, Z. Samardzija, G. Drazic. Interface reactions among electrodes, substrates and Pb(Zr,Ti)O3-based films. Acta Chim. Slov. 48 (2001) 51-62; 12. B. Malič, J. Cilenšek, M. Mandeljc, M. Kosec. Crystallization study of the alkoxide-based Pb(Zrg3Tig7) O3 thin-film precursor. Acta Chim. Slov. 52 (2005) 2539-263; 13. M.M. Amini, S.J.S. Sabounchei, F. Mirnajafi, M. Mir-zaee, M. Sharbatdaran. Preparation of y-alumina from aluminum aminoalkoxides. Ceramics - Silika-ty, 49 (2005) 138-141; 14. N. Bahlawane, T. Watanabe. New sol-gel route for the preparation of pure a-alumina at 950°C. J. Am. Ceram. Soc. 83 (2000) 2324-26; 15. J. Goldstein, D. Newbury, D. Joy, C. Lyman, P. Ech-lin, E. Lifshin, L. Sawyer, J. Michael. Scanning electron microscopy and X-ray microanalysis. 3rd ed. New York, New York Kluwer academic/Plenum (2003); 16. C.G. Bergeron, S.H. Risbud, Introduction to Phase Equilibria in Ceramics. The American Ceramic Society, Westerville (1984); 17. M. Kosec, U. Delalut, B. Malic, V. Bobnar, G. Drazic. Influence of different lead precursors on the micro-structure and properties of sol-gel PZT thin films. ISAF'96: Proc. of the Tenth IEEE International Symposium on Application of Ferroelectrics, B.M. Kul-wicki, A. Amin, A. Safari, IEEE (1996) 443-445; 18. L.A. Bursill, K.G. Brooks. Crystallization of sol-gel derived lead-zirconate-titanate thin films in argon and oxygen atmospheres. J. Appl. Phys. 75 (1994) 4501-4509; 19. R.J. Ong, T.A. Berfield, N.R. Sottos, D.A. Payne. Solgel derived Pb(Zr,Ti)O3 thin films: residual stress and electrical properties. J. of the Europ. Ceram. Soc. 25 (2005) 2247-2251; 20. G.L. Brennecka, W. Huebner. Use of stress to produce highly oriented tetragonal lead zirconate ti-tanate (PZT40/60) thin films and resulting electrical properties. J. Am. Ceram. Soc. 87 (2004) 14591465. Arrived: 09. 10. 2013 Accepted: 11. 01. 2014