Novel Ag/Si composite particles through galvanic displacement and its conductive application
© The Author(s) 2016
Received: 12 July 2016
Accepted: 5 September 2016
Published: 13 September 2016
Here we synthesized a novel Ag/Si composite sub-micro particle using galvanic displacement by capitalizing on the active chemical surface of Si particles sludge from wafer-slicing process. Si works as chemical reactant, as well as reaction site to form composite particles. Sequent structural characterizations and analysis which include X-ray diffraction, transmission electron microscopy, scanning electron microscope, energy dispersive X-ray and electrical properties of this composite particle were done. A well-proved hetero-epitaxial growth mechanism could explain Ag nano-island/layer with a satisfactory bond property deposited on the Si surface. Since these Si are mechanically cleaved from crystal, formed conductive Ag/Si composites retain the flake shape from Si sludge particles, and narrow size distribution. They are preferred as conductive fillers, an Ag/Si composite-based conductive ink was prepared, its conductance was tested through screen printing, film thickness and resistivity were measured. The resistivity reached the µΩ cm level, even without optimizing the ink formulation. Our methods not only convert this Si sludge into highly conductive composite particles as filler for applications, but also considerably reduce the consumption of precious metal.
The synthesis, characterization of precious metal particles have been extensively studied and used in various applications. For example, Au wires are used for Integrated Circuit, light-emitting diode (LED) chip packaging and various bio-applications (Schröter et al. 2011; Chen and Goodman 2004), Ag paste is used in solar cell metallization and for electrical connection in many types modern devices (Mette et al. 2007; Roberson et al. 2015), and Pt is used as a fuel cell electrode catalyst (Stamenkovic et al. 2007). These metals have excellent conductivity, stable chemical properties, but their reserves on Earth are limited, thus are expensive. For decades, researchers have been efficiently using precious metals (Chancerel et al. 2009) or attempting to discover inexpensive replacements for these precious metals for use in existing applications (Felix et al. 2008). In the applications of catalysts for fuel cells, researchers have studied the synthesis, and electrochemical performance of hybrid Pt/Pd nanoparticles and demonstrated that these nanoparticles have superior catalytic activity and high stability (Peng et al. 2009). Ag electrodes are replaced with Cu or Ni plating on the solar cell surface (Lennon et al. 2013). For most common conductive applications in electronic devices, Ag/Cu shell/core hybrid particle-based conductive paste is used to reduce costs (Choi and Lee 2015).
Precious metal particles are normally synthesized by colloid chemical reduction method (Sau and Rogach 2010). Subsequent downstream products, such as Ag conductive paste, can be made using fine Ag particles. However, during the syntheses of precious metal-based nanoparticles, the atoms reduced from a precursor spontaneously form nuclei with different shapes and sizes, finally form particles. If no dispersant or seed is used in the nanoparticle synthesis, the shape and size of metal nanoparticles are difficult to control. Several research results demonstrated the shape-controlled synthesis of precious metal nanocrystals under thermodynamically and kinetically controlled conditions (Xia et al. 2015; Vigderman et al. 2012).
Doped Si wafers are widely used in Ultra Large Scale Integration (ULSI) and photovoltaic industries. To produce wafers, Si ingots are mechanically sliced, and polished. In the mechanical slicing process, some Si parts are crushed into particles by grits and carried away by aqueous slurry and eventually forming Si sludge. This is defined as Si kerf-loss (Moeller 2006). Compared with other Si byproducts, Si sludge not only retains the properties of the Si ingot matrix, such as satisfactory purity and resistivity, but also has several features for making novel material. Si sludge particles already have sub-micrometer dimensions, with D50 of approximately 1–2 µm (Drouiche et al. 2014). During the sawing process, Si cleavages actually occur on crystal structures and mostly become the flake shape. Most importantly, the particles retain the electrochemical properties of Si, but have a more active surface area than a bulk substrate does. Mass production of photovoltaic wafers causes considerable solid pollution because of Si sludge, however, suitable applications for this waste material are under development.
Galvanic displacement has been widely extended to the fabrication of various Si nanostructures (Peng et al. 2006; Nakamura et al. 2010; Nakamura et al. 2011), such as highly oriented Si nanowires by metal-assisted chemical etching (Huang et al. 2011). Oskam reviewed the electrochemical deposition of metals on Si substrates and demonstrated that the thermodynamics and kinetics of metal deposition on Si surfaces are dependent on several complex factors, such as the doping type of Si, concentration of HF solution, and dropping rate (Oskam et al. 1927). So far, the main research on metal–Si contacts focus on metals as contamination at the Si substrate surface during the ULSI process (Gorostiza et al. 1997). Reports on the electrochemical deposition of metals on semiconductor powder, particularly ultrafine Si powder, are scant. One promising application of Si powder in lithium ion batteries has stimulated research on the low-cost and large-scale fabrication of Si porous structures (Ge et al. 2014). In this application, the etching mechanisms are the same as etching bulk Si, but with different compositions of etchants. The deposition of precious metals with a high metal–Si ratio on Si powder has not been experimentally reported yet.
Ag/Si composite particle formation and characterizations
The galvanic reaction of Ag–Si on the surface of Si is as follows:
Conductive ink composition based on our particle
Hybrid solid Ag/Si particle
Results and discussions
Among various reducing agents for forming Ag particles, actually relying on the redox ability of them, several parameters, such as the concentration of reducing agent, temperature, and pH value as well as the dropwise sequence of solution could influence the morphological structure of the final Ag particles. Different dispersants were selected to prevent the accumulating of Ag nuclei, otherwise, Ag nuclei accumulate rapidly to form Ag particles of >10 µm and widely distribute, which is detrimental for downstream applications.
The galvanic redox process described here is straightforward and can generate Ag–Si composite particles in an easy and controllable manner. During this process, Si particles act as mild reducing agents as well as the reaction site, which the Si particle–aqueous solutions interface. Thus we could control the Ag nuclei formation on the site and prevent random nucleus formation, which occurs during the traditional redox system of producing Ag particles. The formed bundle of Ag nuclei mainly affixes to the surface of Si particles; therefore, an additional dispersant to restrict the Ag nuclei gathering process is not required.
Quasi-spherical metal nanoparticles are formed in most synthesis processes, because it is the most thermodynamically and kinetically favorable shape. To create low contact resistance among individual metal particles, we prefer synthesizing flake or wire-shaped particles, having a relatively large contact area with anisotropic growth. Here, we grew an Ag top layer on the Si core through galvanic displacement, and the flake shape of the Ag–Si composite was realized naturally and easily, almost no spherical-shaped composites were found, as displayed in Fig. 2a. This is because crystalline Si wafering process is a mechanical cleavage process occurring along the tetrahedral Si, the Si sludge forms the preferred flake shape of the final Ag–Si composite.
Figure 2b displays the approximate percentage of major elements, particularly Ag and Si in the composed particles. In conductive fillers, if approximately 15–20 % of the weight of Si can be replaced by that of Ag, as displayed in the EDX, the cost of precious metal conductive fillers can be reduced considerably. In addition to particle composition, we could confirm the particle size through PSD measurement, as demonstrated in Fig. 2c. It displays that Ag–Si composite particles have a narrow distribution, an average size D50 of approximately 800–900 nm and are completely dependent on Si matrix particles. This narrow distribution of conductive filler can prevent nozzle jam when a Ag–Si composite particle-based conductive ink is used for highly precise printed electronic devices (Mao et al. 2014).
From the XRD pattern of Fig. 3, we find this Si sludge has poly-crystalline phase, which is because of the mechanical slicing, a tough process broken Si original crystalline structure. For Ag–Si composite, the four solid peaks indicate crystalline phase of Ag, and the weak (111) peak of Si at 28.5° indicates crystallites with a deviating orientation have formed from Si core. This could prove the co-exist of crystalline Si and Ag of these samples. Figure 4a is a bright field (BF) TEM image of the composite. It shows that some dark particles with various sizes disperse on the flakes, the selected area electron diffraction (SAED) patterns in Fig. 4b were taken from a thick flake particle. According to the index results, the crystal orientation relationship between Si and Ag is determined as Si//[−113]Ag and (31-1)Si//(220)Ag. The lattice distortions are −6.13 % for Si and 6.25 % for Ag. Combing the results of TEM experiments and the XRD, which illustrates only pure Ag and Si phase exist, it could be supposed that a island or a layer/flake structure composed by Ag/Si might form additionally. Based on all the information and analysis, we can believe that crystalline Ag structures are formed on the Si matrix, and these Ag layer and/or islands structure will contribute for the conductive application.
The growth mechanism of metallic nanoparticles on semiconductor Si through galvanic displacement has a suggested mode (Sayed et al. 2009): Stranski–Krastanov mode, also called epitaxial growth mode, which is very common for lattice-mismatched hetero-epitaxial growth systems, such as Si nanowires growth using Au as a catalyst (Shimizu et al. 2007), Ag–Si interface also is investigated previously (Starr et al. 2001). In this study, we believe that hetero-epitaxial growth possibly occurred on the certain Si–Ag interface. Because of it, we assert that the Ag layer strongly bond to the Si particle matrix, and the resultant Ag–Si composite particles have excellent scratch-resistant property for applications, compared with other Ag-based shell/core particles, typically Ag/SiO2.
For conductive applications, the measured resistivity still is higher than the ordinary resistivity of an Ag conductive ink. The difference could be attributed to low solid content or low baking temperature. This would not affect the applications if we could optimize further.
For the Ag-based conductive ink, the dispersion ability of conductive filler is a critical property because the heavy Ag particles easily sink in the conductive ink. A specific amount of light Si-composed Ag–Si composite particles reduce the actual particle density, thus the particles do not easily sink in the ink during the fabrication of electrical devices. This is another advantage for the conductive ink applications.
Two conductive theories describe the conduction mechanism of conductive filler ink applications (Vigolo et al. 2005). The contact resistance of individual particles and intrinsic resistance of a single particle have major roles in the conduction mechanism. Although the Si sludge inherits the resistivity from the mother ingots, its conductance is still much less than that of Ag; therefore, an additional thermal doping diffusion, could be performed if further improvement of the conductance of Ag–Si composite particles is needed.
Except traditional methods, we also could tune the weight ratio of the reactants Ag over Si, and the resultant Ag–Si composite particles could have an extremely broad conductance range for various applications. Finally, the Ag thin island/layer can affix well with Si flake core as Ag–Si composite particles because of a chemical reaction and more less reduce the use of noble metals for conductive applications (Hilali et al. 2006; Toriyama and Ishiwatari 2008).
According to galvanic displacement, a set of other precious metals can form the shell or islands structure on the Si sludge particle cores, indicating that a set of precious metal–Si composite materials can be produced. These materials could, in part, replace traditional precious metals in various applications. All such composite particles are worthy of investigation in other new applications, such as in surface-enhanced Raman scatterings (Cao et al. 2002) and hydrogen generation catalysts (Mckone et al. 2011).
We exploited the features of ultrafine Si sludge powder as a reducing agent and a reaction site in galvanic reaction with noble metal and fabricated Ag–Si composite sub-micron structures. The structural analysis and characterizations of the fabricated particles proved that metal islands or layer could grow on the Si particle matrix. Ag–Si composites also retained the flake shape, similar to that of original Si particle matrix. A test for conductivity and measured resistivity of the composite particle-based ink revealed a satisfactory conductive property by using the Ag–Si composites as conductive fillers. Overall, the present study provides an easy, controlled process to synthesize similar metal/semiconductor composite particles that has various applications, not only for conductive ink.
Si wafer processing offers a large amount of Si sludge. Our method uses this pollutant as starting material and form valuable noble metals composite for their applications. Most importantly, these composites could substantially reduce the total use of expensive precious metals.
CY, XL, TL from Hunan university did composite particle synthesis and conductive ink preparation, LZ, CC, YW, LC from Harbin Institute of Technology did TEM and XRD characterization, Dr. LC helped to analyze the TEM and diffraction pattern evaluation. On the manuscript, the main part of the work was completed by CY. XL is responsible for checking references and Dr. TL is responsible for the grammar and details revision. All authors read and approved the final manuscript.
The authors gratefully acknowledge the center of analysis measurement of Harbin Institute of Technology (HIT) for TEM work and the Suzhou Institute of Nano-Tech and Nano-Bionics, CAS for the screen printing test. This study was financially supported in 2013 by “the Fundamental Research Funds for Central Universities” Program at Hunan University and in 2012 by the “100 Talents Plan” Program at HIT.
Authors declare that there is no financial interesting on it and no competing interests to include personal and professional conflicts.
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- Cao WC, Jin RC, Mirkin CA (2002) Nanoparticles with Raman spectroscopic fingerprints for DNA and RNA detection. Science 297:1536ADSView ArticlePubMedGoogle Scholar
- Chancerel P, Meskers C, Hageluken C (2009) Assessment of precious metal flows during preprocessing of waste electrical and electronic equipment. J Ind Ecol 13:791View ArticleGoogle Scholar
- Chen MS, Goodman DW (2004) The structure of catalytically active gold on titania. Science 306:252ADSView ArticlePubMedGoogle Scholar
- Choi EB, Lee JH (2015) Ethylene glycol-based Ag plating for the wet chemical fabrication of one micrometer Cu/Ag core/shell particles. J Alloy Compd 643:S231View ArticleGoogle Scholar
- Drouiche N, Cuellar Guardado PR, Fouad K, Medjahed S, Boutouchent-Guefti N, Ouldhamou M (2014) Recovery of solar grade silicon from kerf loss slurry waste. Renew Sustain Energy Rev 32:936View ArticleGoogle Scholar
- Felix S, Abild-Pedersen F, Thomas B (2008) Identification of non-precious metal alloy catalysts for selective hydrogenation of acetylene. Science 320:1320ADSView ArticleGoogle Scholar
- Ge MY, Lu YH, Ercius P, Rong JP, Fang X, Mecklenburg M, Zhou CW (2014) Large-scale fabrication, 3D tomography, and lithium-ion battery application of porous silicon. Nano Lett 14:261View ArticlePubMedGoogle Scholar
- Gorostiza P, Diaz R, Servat J, Sanz F, Morante JR (1997) Atomic force microscopy study of the silicon doping influence on the first stages of platinum electroless deposition. J Electrochem Soc 144:909View ArticleGoogle Scholar
- Hilali M, Nakayashiki K, Khadilkar C, Reedy RC, Rohatgi A, Shaikh A, Kim S, Sridharan S (2006) Effect of Ag particle size in thick-film Ag paste on the electrical and physical properties of screen printed contacts and silicon solar cells. J Electrochem Soc 153:A5View ArticleGoogle Scholar
- Huang Z, Geyer N, Werner P, de Boor J, Goesele U (2011) Metal-assisted chemical etching of silicon. Adv Mater 23:285View ArticlePubMedGoogle Scholar
- Lennon A, Yao Y, Wenham S (2013) Evolution of metal plating for silicon solar cell metallization. Prog Photovolt Res Appl 21:1454View ArticleGoogle Scholar
- Mao L, Chen Q, Li YW, Li Y, Cai JH, Su WM, Bai S, Jin YZ, Ma CQ, Cui Z, Chen LW (2014) Flexible silver grid/PEDOT:PSS hybrid electrodes for large area inverted polymer solar cells. Nano Energy 10:259View ArticleGoogle Scholar
- Mckone JR, Warren EL, Bierman MJ et al (2011) Evaluation of Pt, Ni, and Ni–Mo electrocatalysts for hydrogen evolution on crystalline Si electrodes. Energy Environ Sci 4(9):3573–3583View ArticleGoogle Scholar
- Mette A, Richter PL, Hoerteis M, Glunz SW (2007) Precise parameterization of the recombination velocity at passivated phosphorus doped surfaces. Prog Photovolt Res Appl 15:621View ArticleGoogle Scholar
- Moeller HJ (2006) Wafering of silicon crystals. Phys Status Solidi A 203:659ADSView ArticleGoogle Scholar
- Nakamura T, Hosoya N, Tiwari BP, Adachi S (2010) Properties of silver/porous-silicon nanocomposite powders prepared by metal assisted electroless chemical etching. J Appl Phys 108:104315ADSView ArticleGoogle Scholar
- Nakamura T, Tiwari BP, Adachi S (2011) Properties of silver/porous-silicon nanocomposite powders prepared by metal assisted electroless chemical etching. Jpn J Appl Phys 50:081301ADSView ArticleGoogle Scholar
- Oskam G, Long JG, Natarajan A, Searson PC (1927) Electrochemical deposition of metals onto silicon. J Phys D Appl Phys 1998:31Google Scholar
- Peng KQ, Hu JJ, Yan YJ, Wu Y, Fang H, Xu Y, Lee ST, Zhu J (2006) Platinum nanoparticle decorated silicon nanowires for efficient solar energy conversion. Adv Funct Mater 16:387View ArticleGoogle Scholar
- Peng Z, Wu J, Yang H (2009) Synthesis and oxygen reduction electrocatalytic property of Pt-on-Pd bimetallic heteronanostructures. Am Chem Soc 131:7542View ArticleGoogle Scholar
- Roberson DA, Wicker RB, MacDonald E (2015) Ohmic curing of printed silver conductive traces. J Electron Packag 137:031004View ArticleGoogle Scholar
- Sau TK, Rogach AL (2010) Nonspherical noble metal nanoparticles: colloid-chemical synthesis and morphology control. Adv Mater 22:1781View ArticlePubMedGoogle Scholar
- Sayed SY, Wang F, Malac M, Meldrum A, Egerton RF, Buriak JM (2009) Heteroepitaxial growth of gold nanostructures on silicon by galvanic displacement. ACS Nano 3:2809View ArticlePubMedGoogle Scholar
- Schröter W, Seibt M, Gilles D (2011) High-temperature properties of transition elements in silicon. In: Handbook of semiconductor technology set, pp 671–679Google Scholar
- Shimizu T, Xie T, Nishikawa J, Shingubara S, Senz S, Goesele U (2007) Synthesis of vertical high-density epitaxial Si(100) nanowire arrays on a Si(100) substrate using an anodic aluminum oxide template. Adv Mater 19:917View ArticleGoogle Scholar
- Stamenkovic VR, Fowler B, Mun BS, Wang GF, Ross PN, Lucas CA, Markovic NM (2007) Improved oxygen reduction activity on Pt3Ni(111) via increased surface site availability. Science 315:493ADSView ArticlePubMedGoogle Scholar
- Starr DE, Ranney JT, Larsen JH, Musgrove JE, Campbell CT (2001) Measurement of the energetics of metal film growth on a semiconductor substrate: Ag/Si(100)-2 × 1. Phys Rev Lett 87:106102ADSView ArticlePubMedGoogle Scholar
- Toriyama T, Ishiwatari T (2008) Preparation of glue joints and bridges between Ag nanowires and their metallization. A possible method for nano-soldering. J Mater Chem 18:5537View ArticleGoogle Scholar
- Vigderman L, Khanal BP, Zubarev ER (2012) High-yield synthesis of gold nanorods with longitudinal SPR. Adv Mater 24:4811View ArticlePubMedGoogle Scholar
- Vigolo B, Coulon C, Maugrey M, Zakri C, Poulin P (2005) An experimental approach to the percolation of sticky nanotubes. Science 309:920ADSView ArticlePubMedGoogle Scholar
- Xia YN, Xia XH, Peng H-C (2015) Shape-controlled synthesis of colloidal metal nanocrystals: thermodynamic versus kinetic products. J Am Chem Soc 137:7947View ArticlePubMedGoogle Scholar