J. Phys. Chem. C 2008, 112, 13901–13904

13901

Synthesis of Vertically Aligned Pd2Si Nanowires in Microwave Plasma Enhanced Chemical Vapor Deposition System Rakesh K. Joshi,†,| Masamishi Yoshimura,† Kei Tanaka,† Kazuyuki Ueda,† Ashok Kumar,‡ and Niranjan Ramgir§ Nano High Tech Research Centre, Toyota Technological Institute Hisakata 2-Chome, Tempaku-Ku, Nagoya 4688511, Japan, Department of Mechanical Engineering, 4202 East Fowler AVenue, ENB 252, UniVersity of South Florida, Tampa, Florida 33620, and College of Engineering, 4202 East Fowler AVenue, ENB 118, UniVersity of South Florida, Tampa, Florida 33620 ReceiVed: March 28, 2008; ReVised Manuscript ReceiVed: July 15, 2008

Vertically aligned Pd2Si nanowires with Pd on tip have been grown using microwave plasma enhanced chemical vapor deposition system in hydrogen atmosphere with high degree of reproducibility. High resolution scanning electron microscopy and transmission electron microscopy show the growth of nanowire structures via root growth in vapor-liquid-solid (VLS) mechanism where hydrogen acts as catalyst for silicide formation with Pd-hydride being the dominant moving species in the microwave environment. 1. Introduction Palladium silicide (Pd2Si), the equilibrium reaction product between Pd and Si, is used to make low resistance reproducible ohmic contacts to Si. Palladium silicide has advantage over other metal silicides that it has lower silicidation temperature which makes it more flexible for device fabrication process.1,2 For the Pd-Si system, it is known that, after a relatively low temperature annealing (200-300 °C) the Pd2Si phase is formed.3-6 However, the PdSi is formed at temperatures higher than 700 °C. The formation of epitaxial or polycrystalline Pd2Si is known to be affected by the precursor material’s purity, growth rate and the environmental conditions during growth.7-9 The growth and structure of Pd2Si have been studied extensively in the past, but the reports dealing with the formation of Pd2Si in nanodimensions, especially the nanowires, have been rare to mention. Nanowires of such alloys are expected to be extremely useful as interconnectors for nanoelectronic applications. Nanowires of various materials have been grown and studied extensively in past based on different growth mechanisms. Using the well-known vapor-liquid-solid (VLS) mechanism,10 several researchers exploited different techniques to create the necessary nanometer-scale metastable droplets of transitionmetal catalysts in order to synthesize nanowires.11,12 However, the required synthesis temperatures when using these metals range from 500 to 1000 °C for various transition metals. Other variations of VLS techniques such as solution-liquid-solid13 and vapor-solid-solid14 methods have also been reported. Equipped by the well know affinity of Pd toward hydrogen,15 coupled with the knowledge of the fact that the Pd-H system is unstable at higher temperature,15 along with the indication of possible modifications in the nucleation and growth of Pd2Si by varying the growth conditions we made attempts to grow the Pd2Si nanostructures for the first time by using H2 environ* To whom correspondence should be addressed. E-mail: rjoshi77@ yahoo.com. † Toyota Technological Institute Hisakata 2-Chome. ‡ Department of Mechanical Engineering, University of South Florida. § College of Engineering, University of South Florida. | Present address: Department of Mechanical Engineering, 4202 E. Fowler Ave, ENB 252, University of South Florida, Tampa, FL 33620.

ment in microwave plasma enhanced chemical vapor deposition (MPECVD) system. Formation of palladium silicide at low temperatures such as 350-500 °C via diffusion limited growth has been reported in past.4,6 Here, we report a metal induced VLS technique in a chemical vapor deposition method that does not require very high temperatures for the growth of selfassembled Pd2Si nanowires on Si wafer. The growth of nanowire is induced by a layer of electrochemically grown palladium particles on silicon substrate. 2. Experimental Section The Pd nanoparticles were grown on Si substrates through potentiostatic electrodeposition using 0.04 mol/L PdSO4 (50 mL) mixed with sulfuric acid (10 mL) electrolyte solution. Some measured quantity (20 mL) of this electrolyte was taken into an electrochemical cell for the growth of Pd nanoparticles on Si substrates. Chemically cleaned Si substrates were dipped in the electrolyte solution and voltage of -0.1 V was applied to the substrate. After the chosen deposition time the substrates were taken out of the solution and dried. Detailed growth procedure and mechanism have been reported elsewhere.16,17 Once dried, they are introduced into the MPECVD chamber for the Pd2Si nanowire growth. Ultra pure hydrogen (H2) was introduced with a flow rate of 80 standard cubic centimeters (sccm), into the growth chamber, and the pressure was kept at 1.7 Torr by adjusting the vacuum valve connecting between a rotary pump and the growth chamber, for the growth time of 5 min at a temperature of ∼550 °C of the sample holder. Substrate (Si) is a kind of thermal-insulator; therefore, the real temperature at the particles could be higher than the measured. We used a microwave of 2.45 GHz and 500 W. During growth, -200 V was applied to the bottom electrode on which the substrate was mounted. The as-grown Pd2Si nanostructure samples were characterized by high resolution scanning electron microscope (HRSEM), high resolution transmission electron microscope (HRTEM) and glancing angle X-ray diffraction (GAXRD) to study their surface and structural morphology. Palladium nanoparticles with spherical shape and nearly monodisperse quality16 were used to grow the Pd2Si nanowires.

10.1021/jp8050752 CCC: $40.75  2008 American Chemical Society Published on Web 08/13/2008

13902 J. Phys. Chem. C, Vol. 112, No. 36, 2008

Joshi et al.

Figure 1. SEM pictures for the MPECVD grown vertically aligned Pd2Si nanowires grown using Pd nanoparticle of 50 (right) and 75 nm (left).

Figure 2. (a) TEM micrograph for the single Pd2Si nanowire, with SAED patterns for different regions, as indicated, to show the crystallinity of the nanowires (b) TEM pictures for single Pd2Si nanowire grown on Pd nanoparticle of 40 nm and (c) lattice imaging for Pd2Si nanowire, showing the d spacing.

3. Results and Discussion Pd2Si nanostructures were grown on Si substrates, and characterized as grown by using SEM and TEM. Figure 1 shows the SEM pictures for the MPECVD grown vertically aligned Pd2Si nanowires. Pd2Si nanostructures grown under such conditions were visualized by extensive SEM study (Supporting Information (SI)-1). Different shapes of Pd nanoparticles,16,17 such as spheres, traingles, cubes and stars were used for Pd2Si growth separately in order to test the reproducibility. Architecture of Pd2Si was noticed to be independent of initial Pd shape and size under the experimental limits. The nanowires are randomly grown on the substrate coated by Pd particles. In addition, during the growth at temperature ∼550 °C the shape of the Pd particles can be changed and the nearby small particles may combine to form bigger particles. As noticed from the SEM study that the final density of Pd2Si nanowires is much less than the initial density of Pd particles on silicon substrate. It is

highly probable that many Pd particles are contributing for the growth of one nanowire of Pd2Si. Vertically aligned nanowires were successfully grown, with extremely high degree (∼100%) of reproducibility. In order to understand the crystallography of these nanostructures, HRTEM measurements were performed. The constant electrical bias of -200 V applied to the substrate helps to get vertically aligned nanostructures via VLS growth with hydrogen as catalyst. The TEM micrographs for the nanowires grown on 50 (a), and 40nm (b) Pd nanoparticles are shown in Figure 2 and as well as in SI-2. Analysis of the TEM measurements shows the crystallinity of the nanowires, where the body of the nanowires is observed to be polycrystalline hexagonal-Pd2Si shown by the ring type selected area electron diffraction (SAED) pattern (Figure 2 insettop right, and SI-2 inset) and neck of the nanowires is fully crystalline ‘epitaxial’ Pd2Si with hexagonal structure (Figure 2 inset- bottom left) with its (nanowire’s) tip occupied by Pd with

Synthesis of Vertically Aligned Pd2Si Nanowires

J. Phys. Chem. C, Vol. 112, No. 36, 2008 13903

Figure 3. Schematic representation of different stages of the Pd2Si nanowire growth via VLS mechanism using MPECVD growth.

fcc structure. Presence of Pd on the tip of the nanowires is clearly shown as color contrast with respect to body Pd2Si in the SEM micrographs (SI-1) and also in the TEM micrographs. Signatures of the presence of fcc palladium in the nanowires have been observed by the XRD (SI-3) and TEM. The detailed TEM analysis has been performed to estimate the inter planer distance‘d’ by using the HRTEM imaging. The‘d’ value was found to be equal to ∼0.569 nm as shown in Figure 2 c. This calculated value was compared with the theoretically available‘d’ values for Pd2Si (d(100) ) 0.563 nm, hexagonal, space group P62m).18 The structural results, obtained by TEM are supported by the XRD. Growth of the nanowires is explained in the following section. VLS,10,19 the well-known growth mechanism for free-standing semiconductor nanowires, has been found to be responsible for the growth of vertically aligned Pd2Si nanowires. Palladium has dual role of acting partially as catalyst as well as of taking part in maintaining the stoichiometry of Pd2Si. This was made possible by the presence of H2 during growth in the diffusion limited growth resulting into the formation of Pd2Si. The conditions of the substrate such as its orientation and nature of the catalyst can modify the growth conditions. Moreover, the gaseous environment at the vicinity of targeted substrate contributing predominantly toward the formation of Pd and Sihydrides as well as taking part in mass transport through the silicide formation. Si species from the substrate and from the dissociation product of SiH4 diffuse into the Pd particles and get consumed for the nanowire formation taking place as per the root growth mechanism. Schematic illustration in Figure 3 clearly indicates the different steps involved in the root growth as per VLS mechanism. Presence of hydrogen increases the rate of palladium silicide formation by altering the diffusion barrier at the Pd/Si interface. Hydrogen diffusion is known to occur for distances over several microns in the Si substrate at low reaction temperature; however, it is hindered in the silicide layer. Initially at low reaction temperature, formation of palladium hydride (Pd-H) takes place due to the strong affinity of Pd toward hydrogen. 15 However, the Pd-H system is unstable at higher temperatures (above ∼300 °C) maintained during the growth process. Figure 3 shows the formation of palladium hydride and silicon hydride at lower temperatures. The increase in reaction temperature results in the loss of hydrogen at the Pd2Si/Si interface. Interestingly, small amount of palladium mass

transport do occur and the corresponding traces can be clearly seen in the TEM image (Figure 2). The triangular Pd marks observed within the nanowires (Figure 2, and SI-2) are the signatures of the occurrence of slow Pd mass transport. During the synthesis, part of Pd particles split off from the root particles due to capillary suction, as a result of the fuse state of the particles and surface instabilities. Selected area electron diffraction for the nanowire surfaces, interface of Pd tip and body further confirms the silicide formation. The palladium richness in the nanowires can also be attributed to the higher initial Pd thickness on the substrate (1 µm). This is to mention, that no nanowire formation was observed on replacing hydrogen by argon and nitrogen gas, however, the formation of Pd2Si islands on the silicon substrate was noticed in the inert atmosphere at temperatures ∼500 °C. Therefore, hydrogen has been determined as a necessary catalytic gaseous environment for the growth of Pd2Si nanowires with repeatable morphology. All the factors, such as, the nanoparticle nature of Pd, presence of catalytic hydrogen environment, formations of intermediates Pd-H and Si-H4, possibly combining together for the Pd2Si nanowire growth. Conclusions Pd2Si nanowires have been grown via root growth in VLS mechanism wherein hydrogen initiates and sustains the silicide formation. Hydrogen acts as catalyst, and observed to be necessary for the growth of Pd2Si nanowires. Hydrogen reacts, with Pd to form Pd-H, and with Si to form Si-H4 as intermediate states, and making them available for the Pd2Si formation as the temperature progress duing the growth. Acknowledgment. This work was supported by “project for private universities: matching fund subsidy” from MEXT (2006-2008), Japan. Supporting Information Available: Figures SI-1-SI-3 as described in the text. This material is available free of charge via the Internet at http://pubs.acs.org. References and Notes (1) Sano, K.; Hino, M.; Ooishi, N.; Shibahara, K. Jpn. J. App. Phys. 2005, 44, 3774. (2) Yang, C.-S.; Lue, J.-T. Phy Stat. Sol. A 2005, 101, 151.

13904 J. Phys. Chem. C, Vol. 112, No. 36, 2008 (3) Chikyow, T.; Ohdomari, I; Suzuko, S. Phys. ReV. B 1986, 34, 4807. (4) Tsaur, B. Y.; Nicolet, M.-A. Appl. Phys. Lett. 1980, 37, 708. (5) Abhaya, S.; Amarendra, G.; Gopalan, P.; Reddy, G. L. N.; Saroja, S. J. Phys. D: Appl. Phys. 2004, 37, 3140. (6) Beshkov, G.; Dimitov, D. B.; Koprinarova, J.; Gesheva, K. Vacuum 1998, 51, 177. (7) Muraka, S. P. Silicide for VLSI application; Academic Press: New York, 1983. (8) Bower, R. W.; Sigurd, D.; Scott, R. E. Solid Sate Electron. 1973, 16, 1461. (9) Paccagnella, A.; Majni, G.; Ottaviani, G.; Mea, G.-D Appl. Phys. Lett. 1985, 47, 806. (10) Wagner, R. S.; Ellis, W. C. Appl. Phys. Lett. 1964, 4, 89. (11) Morales, A. M.; Lieber, C. M. Science 1998, 279, 208. (12) Duan, X.; Lieber, C. M. AdV. Mater. 2000, 12, 298.

Joshi et al. (13) Holmes, J. D.; Johnston, K. P.; Doty, R. C.; Korgel, B. A. Science 2000, 287, 1471. (14) Gole, J. L.; Stout, J. D.; Rauch, W. L.; Wang, Z. L. Appl. Phys. Lett. 2000, 76, 2346. (15) Lewis, F. A. Platinum Met. ReV. 1982, 26, 20. (16) Joshi, R. K.; Yoshimura, M.; Chiu, C.-C.; Tung, F.-K.; Ueda, K; Tanaka, K. J. Phys. Chem. C 2008, 112, 1857. (17) Joshi, R. K.; Yoshimura, M.; Matsuura, Y.; Ueda, K; Tanaka, K. J. Nanosci. Nanotechnol. 2007, 7, 2078. (18) Kennedy, S. J.; Wu, E.; Kisi, E. H.; Gray, E. M.; Kennedy, B. J. J. Phys.: Condens. Matter 1995, 7, L 33. (19) Sood, D. K.; Sekhar, P. K.; Bhansali, S. Appl. Phys. Lett. 2006, 88, 143110.

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