Yingqiong
Yong
,
Tetsu
Yonezawa
*,
Masaki
Matsubara
and
Hiroki
Tsukamoto
Division of Materials Science and Engineering, Faculty of Engineering, Kita 13 Nishi 8, Kita-ku, Sapporo, Hokkaido 060-8628, Japan. E-mail: tetsu@eng.hokudai.ac.jp; Fax: +81 011 706 7881; Tel: +81 011 706 7112
First published on 9th April 2015
To facilitate sintering of copper particles at low temperatures and achieve excellent electrical conductivity of copper films, reducing particle size is a common method. However, strong reducing agents which are usually used for reducing the size of particles limit their application. Here we report a novel approach to obtain highly conductive copper films. Firstly, copper fine particles were prepared by a one-pot reduction reaction utilizing D-isoascorbic acid as a mild reductant. Secondly, tight connection facilitating the sintering of particles was formed by generating convex surfaces, nanorods or nanoparticles during the oxidation procedure. The mechanism of the oxidative preheating process and its effects on the conductivity were clarified. High conductivity of copper films at low temperatures can be achieved due to the critical role of the oxidative preheating process.
Copper inks, owing to the higher electromigration resistance of metallic copper,9,10 much lower cost and low resistivity, have become a promising candidate for future conductive inks. In order to achieve high conductivity of copper films prepared from the copper inks, a well-known approach is to decrease the size of copper particles, which can facilitate the sintering of copper particles.10–12 Generally speaking, strong reductants can produce nanoparticles because of their high nucleation rate and high density of nuclei.13–15 Thus far, strong reductants such as hydrazine and sodium borohydride have been frequently utilized in the preparation of copper nanoparticles.2,12,15–19 However, hydrazine is extremely dangerous and sodium borohydride can bring in impurities which are difficult to remove by a simple washing procedure using solvent.20
Instead of decreasing the size of nanoparticles to facilitate the sintering of copper particles, a facile thermal oxidation process which can increase the contact between particles might be another solution. Nanorods or nanowire-like coppper oxides prepared via a thermal oxidation process21–24 have been extensively studied because of their wide range of applications in gas sensors,25 heterogeneous catalysts,26etc. To our best knowledge, they have not been used for facilitating the coalescence of copper particles. Some reports have used an oxidative preheating process in air to remove the coated layers on copper nanoparticles27 and demonstrated its crucial role in obtaining conductive films with a low resistivity.28 However, the mechanism of the oxidative preheating process remains unclear. In situ TEM observation of copper fine particles with and without air can reveal the structural changes, but the complete understanding is still difficult.27,29
Herein, we propose a new route towards improving the conductivity using a mild reducing agent. This route can be achieved via a two-step process. Firstly, we synthesized copper fine particles by using D-isoascorbic acid30–32 as the reductant and octylamine33–36 as the capping agent. Then we successfully generated convex surfaces, nanorods or nanoparticles by an oxidative preheating process to facilitate the sintering of particles, resulting in excellent conductivity of copper films after sintering. To our best knowledge, the oxidative preheating process is demonstrated, for the first time, to facilitate the sintering of particles by generating nanorods or nanoparticles. The mechanism of the oxidative preheating process and its effects on the conductivity of copper films were studied. The results show that prepared copper films have high electrical conductivity due to the effects of the oxidative preheating process.
Fig. 1 Schematic illustration of the synthetic procedure of copper fine particles by a one-pot strategy. |
Prepared copper B fine particles were also used for preparing the inks and films using the same method. Then, the prepared films were heated at 250 °C in air at the same flow rate for various oxidative preheating periods (5 min, 30 min, 2 h and 4 h).
For the copper B particles, thermal properties were measured by thermogravimetric analysis (TGA, Shimadzu DTG-60H). The films prepared using copper B particles were also characterized by XRD, SEM and resistivity measurements.
Fig. 3 shows SEM images and XRD of copper A films oxidatively preheated at 200 °C for various heating periods. Before the preheating process, copper A fine particles are separated by the organic layers. The surfaces of copper A fine particles are smooth (Fig. 3a), which indicates that no obvious oxidation of the particle surfaces occurred, which can also be confirmed by XRD patterns. At the preheating time of 5 min, convex surfaces and coalescence of particles can be obviously observed (Fig. 3b). With the increase of preheating time, coalescence of particles leads to tight connections between particles (Fig. 3b–e). According to the XRD analysis shown in Fig. 3f, there are apparent diffraction peaks of cuprous oxide (Cu2O) besides those of metallic copper after the oxidative preheating process, indicating that the convex surfaces are related to the generation of Cu2O.
Fig. 3 SEM images of copper A films oxidatively preheated at 200 °C for various periods: (a) 0 min, (b) 5 min, (c) 30 min, (d) 2 h, and (e) 4 h. (f) Corresponding X-ray diffraction patterns. |
Fig. 4a–d show the SEM images of copper A films oxidatively preheated at 250 °C for various heating periods. With the increase of preheating time, convex surfaces and coalescence of some fine particles, which are the same as the results of copper A films oxidatively preheated at 200 °C, can also be observed (Fig. 4a–d). It should be noted that nanorods appeared besides the convex surfaces. The generated nanorods lead to the formation of denser films (Fig. 4b–d). XRD analysis of copper A films oxidatively preheated at 250 °C for various heating periods is shown in Fig. S4 (ESI†). Similar to the case of oxidative preheating at 200 °C shown in Fig. 3, copper fine particles started to be oxidized mainly to Cu2O and small amounts of CuO at the preheating time of 5 min. With the increase of preheating time, the oxidation process continued with the decrease of intensity of metallic copper peaks. In combination with the results of SEM images (Fig. 4a–d), it can be concluded that the formation of copper oxides (Cu2O or CuO) leads to the generation of convex surfaces at the beginning of the preheating process and nanorods as the oxidation procedure proceeds.
Fig. 4 SEM images of copper A films oxidatively preheated at 250 °C for various periods: (a) 5 min, (b) 30 min, (c) 2 h, and (d) 4 h. |
The other study in which copper B films were oxidatively preheated at 250 °C was also carried out. By contrast, their SEM and XRD results (Fig. 5a–f) show different results. Interestingly, what appeared on the convex surfaces in morphology was not nanorods but smaller nanoparticles (Fig. 5c–e). The XRD results exhibit that peaks representing metallic copper, Cu2O and Cu8O were detected at the preheating time of 5 and 30 min. Cu8O, Cu2O and CuO coexisted in the films oxidatively preheated for 2 and 4 h. Copper oxides have many forms, including well-known Cu2O and CuO and other metastable phases (Cu8O,41 Cu64O,42etc.). These metastable phases can be formed in the copper phase in certain depth during the atomic diffusion process.
Fig. 5 SEM images of copper B films oxidatively preheated at 250 °C for various periods: (a) 0 min, (b) 5 min, (c) 30 min, (d) 2 h, and (e) 4 h. (f) Corresponding X-ray diffraction patterns. |
The mechanism of the oxidative preheating process can be illustrated in Fig. 6. The main reactions during the oxidative preheating process can be explained by the following equations.
4Cu + O2 → 2Cu2O | (1) |
2Cu2O + O2 → 4CuO | (2) |
Fig. 6 Schematic illustration of the oxidation preheating process which can be used for generating convex surfaces, nanorods or nanoparticles and finally promote the sintering of particles. |
The oxidation process involves copper ion diffusing from the copper matrix to the surface22,43 and oxygen diffusion.44 It can be divided into two stages. During the first stage, the diffusion of copper ions and oxygen results in the formation of convex surfaces (Fig. 3b–e, 4a and 5b). When the oxidative temperature is low, copper fine particles can only be oxidized to Cu2O (eqn (1)). When the oxidative temperature is high enough, small amounts of formed Cu2O as a catalyst can transform into a more stable CuO (eqn (2)).23,45 If copper particles are surrounded by lots of protonated octylamine, the protonated octylamine may limit effective contact between copper ions and oxygen, which leads to the formation of Cu8O which was found in XRD (Fig. 5f), and inhibits the generation of CuO. During the second stage, the growth of nanorods (Fig. 4b–d) or the formation of nanoparticles (Fig. 5c–e) happens. About the mechanism of nanorods or nanowires, it is often explained by the vapour–liquid–solid (VLS),46 vapour–solid (VS),47 or diffusion mechanism.24,43 For the VLS mechanism, a catalyst is needed and droplets on the top of nanorods or nanowires are left. For the VS mechanism, our oxidative preheating process runs at low temperatures which are much lower than the melting point of copper and copper oxides.22 The plausible reason for growth of nanorods might be that the local electric field established by the oxygen ions at the solid/gas interface enhances the diffusion of the copper ions23 and reactions between copper ion and oxygen ions happen. This process during which reactions (1) and (2) take place simultaneously can only happen at a high oxidative temperature. If the copper particles are surrounded by plenty of protonated octylamine, the electrostatic force will interfere with the electric field. This interference may affect the diffusion of copper ions from the initial nuclear site to the tip of nanorods, resulting in the small nanoparticles. In addition, metastable Cu8O, Cu2O and CuO coexist in the films as a result of protonated octylamine.
Fig. 7 shows SEM images of copper A films preheated in air for 4 h (Fig. 7a, c and e) and copper A films annealed through a two-step process (Fig. 7b, d and f) at 200 °C, 250 °C and 300 °C, respectively. The morphologies of copper films oxidatively preheated at 200 °C, 250 °C and 300 °C for 4 h present that coalescence between particles took place significantly, leading to the formation of compact films. Moreover, the higher the preheating temperature was, the denser the obtained oxidative film was (Fig. 7a, c and e). After the reductive sintering process at various temperatures, the oxidative films were completely reduced to copper films (Fig. S5, ESI†) and highly dense copper films without obvious cracks were formed (Fig. 7b, d and f). And the copper film obtained at higher temperature became denser. Fig. 8 exhibits the resistivities of copper A films annealed through the two-step annealing process. The copper A films annealed at 200 °C, 250 °C and 300 °C exhibit excellent low resistivities of 12.2, 7.8 and 5.6 μΩ cm, respectively. The resistivity decreases as the annealing temperature increases, which is consistent with the SEM results in Fig. 7b, d and f. The resistivity of copper film annealed at 200 °C is only 7 times of that of bulk copper (1.7 μΩ cm). The outstanding electrical conductivity of annealed copper films can be attributed to the critical role of the oxidative preheating process. During the preheating process, generated convex surfaces are conducive to the tight connections between particles. Nanorods grow toward various directions, causing further connection of adjacent particles and formation of more compact network structures. Hence the sintering of particles was greatly facilitated. For copper B films, owing to the effects of small nanoparticles in the oxidative preheating process, these films which contain plenty of organics can also achieve relatively low resistivities of 82 and 86 μΩ cm at 250 °C and 300 °C, respectively (Fig. S6, ESI†). It is widely understood that small particles can facilitate the sintering of particles.11,12 Furthermore, in our experiment, the produced nanoparticles lead to close contacts between particles and the formation of films with closely packed structure, which can promote the sintering of particles. Finally, after the reductive sintering process, sintered copper films with high conductivities can be obtained with the assistance of convex surfaces, nanorods or nanoparticles (Fig. 6).
Fig. 8 Resistivity as a function of the annealing temperature of copper A films annealed through a two-step process. |
It is generally recognized that the sintering process of copper particles takes place when the organic layers have been removed and the necks start to form between the particles.11 Currently, most of the reports use the sintering process directly to remove the organic layers without carrying out the oxidative preheating process.2,12,34 However, it is worth noting that the role of oxidative preheating is not only to remove the organic layers, but also to build close connections between particles and form highly compact films by the role of convex surfaces, nanorods or nanoparticles. Importantly, there are two advantages for using our method. Firstly, our method which uses copper fine particles can avoid or mitigate the problems caused by copper nanoparticles. The utilization of strong reductants can be avoided and copper fine particles are much easier to be stored than copper nanoparticles. As we know, the oxidation of copper nanoparticles under ambient conditions is severe, especially their size gets smaller. Secondly, in contrast with the method which needs to control the size of copper nanoparticles or form copper/silver core–shell nanoparticles48 precisely and complicatedly, our thermal oxidation process is more facile and can also lead to excellent conductivity at low temperature.
Footnote |
† Electronic supplementary information (ESI) available: Illustration of the detailed experimental process, data of copper B particles, and cross-sectional images of the copper A films, as well as XPD patterns after sintering. See DOI: 10.1039/c5tc00745c |
This journal is © The Royal Society of Chemistry 2015 |