Introduction

Morphology control is an important technique in materials science.1, 2, 3, 4 Biominerals are inorganic–organic composites with controlled morphologies. In biomineralization, crystal morphologies are controlled by biological macromolecules under mild conditions. Inspired by the biological processes, a variety of inorganic–organic fusion materials have been prepared through molecular-control techniques.5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16 In molecular-control processes, the organic molecules influence crystallization of inorganic materials by a variety of interaction schemes. The interaction between the crystal faces and the additive molecules induces morphology changes through habit modification.17, 18, 19, 20 The oriented nanocrystals, namely mesocrystals, are obtained through the sequential crystal growth with the interaction of the additive organic molecules.21, 22, 23, 24, 25, 26 The organic macromolecules serve as templates for growth of inorganic crystals.27, 28, 29, 30, 31, 32 The diffusion-controlled conditions for crystal growth are achieved in the polymer matrices. Morphology variation emerges from the combination of these interaction schemes. If these effects are tuned in a synthetic system, inorganic-organic fusion materials with complex morphologies can be designed by molecular-control processes.

A variety of morphologies have been observed on crystals grown in a polymer and gel matrices.27, 28, 29, 30, 31, 32, 33, 34, 35, 36, 37, 38, 39, 40, 41 In general, kinetically controlled growth of crystal proceeds under low supersaturated conditions in the absence of polymer matrices.42 In contrast, diffusion-controlled growth is achieved in the polymer matrices because the diffusion of the solutes is limited in the presence of macromolecules.9, 14, 31 Kato and co-workers reported on the crystallization of calcium carbonate (CaCO3) in a variety of polymer matrices.5, 7, 27, 28, 29, 30, 43, 44, 45, 46, 47, 48, 49, 50, 51, 52, 53 The patterned inorganic-organic composites were obtained in the polymer matrices on substrates. Our group has studied morphological variation in crystals from polyhedrons to dendritic morphologies with an increase in the density of polymer matrices.31 The two-dimensional patterns of barium nitrate were prepared in a polymer matrix.40, 41 When the unit crystals formed the polyhedral shapes with the lower symmetry, the twisted accumulation of the unit crystals were observed in the polymer matrices.36, 37, 38, 39 These previous works suggest that the diffusion-controlled condition has an important role for crystal growth in polymer matrices. In general, patterned architectures are fabricated by top-down approaches, such as lithography. However, they could also be obtained easily by crystal growth in polymer matrices as a bottom-up approach. Our intention here is the use of the dendritic crystals grown in polymer matrices as a self-template for morphogenesis of the other materials. The dendritic morphologies of a metal oxide and a metal were prepared from the dendrites of a transition metal salt. The present method can be applied as a bottom-up approach for the morphogenesis of materials.

Conductive polymer materials have attracted much interest in recent years. It is not easy to achieve simultaneous control of the synthesis and morphogenesis of conductive polymers.54, 55, 56, 57 The morphology control was achieved by using templates, such as self-assembled molecules and nanospace host materials.58, 59 In a previous report, the composites of monovalent copper oxide (Cu2O) and PPy were prepared by the oxidative polymerization on the divalent copper oxide (CuO) nanoplates.60 In the present work, we adopted the vapor-phase polymerization technique for such morphogenesis. The dendritic crystals of Cu(CH3COO)2·H2O, a transition metal salt, were used as both a template and an oxidative agent. PPy is synthesized by oxidative polymerization from Py. Because Py vapor was supplied to the dendritic crystals of Cu(CH3COO)2·H2O, PPy was formed by the oxidative polymerization on the dendritic crystals. The dendritic morphology of PPy was maintained after the dissolution of the copper-related compounds. The present approach using the morphology-controlled reactive template can be regarded as a new method for the morphogenesis of conductive polymer materials.

Figure 1 summarizes the scheme of the present work. The original dendrites of Cu(CH3COO)2·H2O crystals were grown in a matrix of poly(vinyl alcohol; PVA). The thermal treatment of the original Cu(CH3COO)2·H2O with the PVA film provided the CuO dendritic morphology with a porous structure (Figures 1a and b). The dendritic shapes of metallic Cu were formed by the subsequent reduction of the CuO (Figure 1c). When the original Cu(CH3COO)2·H2O dendrite with the PVA film was set in a sample bottle with the neat liquid of Py monomer, the diffusion of Py vapor induced the oxidative polymerization around the dendrite (Figures 1a and d). The composite film of PPy and PVA with the dendritic morphology was eventually obtained after the dissolution of the original dendrite (Figures 1d and e). The present work shows a new bottom-up approach for the morphogenesis of materials, such as metal oxides, metals and conductive polymers.

Figure 1
figure 1

Schematic illustrations of the dendritic morphologies obtained in the present work. (a) Precursor Cu(CH3COO)2·H2O dendrite grown in a poly(vinyl alcohol; PVA) matrix. (b) CuO synthesized via the thermal treatment of the precursor Cu(CH3COO)2·H2O. (c) Metallic Cu prepared via the reduction of CuO by immersion in aqueous dimethylamine borane (DMAB) solution as a reducing agent. (d) PPy formed with the Cu(CH3COO)2·H2O dendrite in the PVA matrix. (e) PPy/PVA composite obtained after the dissolution of the copper-related compounds by HCl.

Experimental procedure

Preparation of Cu(CH3COO)2·H2O crystals in PVA matrices

The precursor solutions containing 0.5–5.0 g of Cu(CH3COO)2·H2O (Kanto, Tokyo, Japan, 99.0 %; CCu g−1 in 100 g of water) and 0–3.0 g of PVA (Jusei, Tokyo, Japan, Mw=22 × 103; CPVA g−1 in 100 g of water) were prepared in 100 g of purified water. The aqueous solution of PVA was prepared in purified water at 80–100 °C. After cooling, Cu(CH3COO)2·H2O was added in the PVA aqueous solution at room temperature. Upon dissolution of the materials, 5 cm3 of the precursor solution was poured in a polystyrene (PS) vessel (64 mm in length, 35 mm in width and 9 mm in height). A cleaned glass slide (62 mm in length and 26 mm in width) was set at the bottom of the vessel. The PS vessel was maintained at 25 °C, with a slope of 1°, without sealing and under ambient pressure and moisture. After the evaporation of water, the crystals were deposited on the surface of glass substrates.

Syntheses of CuO and Cu from the original dendrite of Cu(CH3COO)2·H2O

The resultant dendrite of Cu(CH3COO)2·H2O formed at CCu=1.0 and CPVA=1.0 on the substrate was placed in a furnace set at 500 °C without the temperature elevation steps under air atmosphere. After 1 h, the substrate was withdrawn from the furnace immediately. The gradual heating and cooling processes were not included in the present treatment. The resultant CuO on the substrate was immersed in an aqueous solution containing 10 mmol dm−3 of dimethylamine borane (DMAB, Wako, Osaka, Japan, 97.0%) as a reducing agent for 3 h.

Syntheses of PPy on the original dendrite of Cu(CH3COO)2·H2O

The resultant Cu(CH3COO)2·H2O dendrite crystals on a substrate were immersed in a glass vessel containing an excess amount of Py neat liquid in a separate sample bottle. The sample bottle was sealed and then maintained at 60 °C for 24 h. The withdrawn substrate was dried at 60 °C under ambient pressure to evaporate the excess monomers adsorbed on the surface. The remaining copper-related compounds were dissolved by immersion of the substrate in an aqueous solution containing 0.1 mol dm−3 hydrochloric acid (HCl) for 15 h.

Characterization

The morphologies of the structures were observed by optical microscopy (Keyence, Osaka, Japan, VHX-1000 and Olympus, Tokyo, Japan, BX-51-FL), scanning electron microscopy (Keyence VE-9800) and field-emission scanning electron microscopy (FEI, Hillsboro, OR, USA, Sirion and Hitachi, Tokyo, Japan, S-4700). Amorphous osmium was coated on the surface of the sample to ensure the conductivity. Energy dispersive X-ray (Bruker AXS, Yokohama, Japan, Quantax) spectroscopy was performed on the field-emission scanning electron microscopy observation. The crystal structure and growth direction were analyzed by X-ray diffraction (XRD; Rigaku, Tokyo, Japan, MiniFlexII) with a CuKα radiation. The formation of PPy and the presence of the acetate groups in Cu(CH3COO)2·H2O and the OH groups in PVA were analyzed by Fourier-transform infrared absorption (FT-IR; JASCO, Tokyo, Japan, FT-IR 4200ST). The FT-IR analyses were performed by the KBr method.

Results and Discussion

Morphology variation of Cu(CH3COO)2·H2O crystals in PVA matrices

The Cu(CH3COO)2·H2O crystals were obtained with the PVA film on a glass substrate after the evaporation of water from the precursor solution. The morphology of Cu(CH3COO)2·H2O crystals was changed by the CCu and CPVA (Figure 2). The polyhedral crystals several hundred micrometers in size were formed in the lower concentration of PVA or in the absence of PVA (Figures 2a and b). As the PVA concentration increased, the dendritic morphologies were obtained throughout the substrates (Figures 2a, c and d). The dendrites with the regularly branched angles were observed in the lower concentration region of Cu(CH3COO)2·H2O (Figures 2a and c), whereas the irregularly branched dendritic shapes were grown in the higher concentration region of Cu(CH3COO)2·H2O (Figures 2a and d). The isolated particles were only observed in the region of the lower Cu(CH3COO)2·H2O concentration and the higher PVA concentration (Figures 2a and e). The morphologies were altered from the polyhedrons to the dendritic shapes with an increase in the PVA concentration, which was consistent with our previous studies of crystal growth in polymer matrices.31 These facts suggest that the diffusion-controlled conditions were achieved on crystal growth of Cu(CH3COO)2·H2O in the PVA matrices.

Figure 2
figure 2

Variation in the morphology of Cu(CH3COO)2·H2O crystals grown in poly(vinyl alcohol; PVA) matrices. (a) Summary diagram showing morphology variation from polyhedral shapes (triangles) to regular dendrites (circles), irregular dendritic shapes (squares) and microparticles (diamonds) with changes in CCu and CPVA. (be) Optical microscope images of polyhedral shapes (b), regular dendrites (c), irregular dendritic shapes (d) and microparticles (e), respectively. A full color version of this figure is available at Polymer Journal online.

In the present work, we focused on the Cu(CH3COO)2·H2O dendrites with regularly branched angles as the templates (Figure 3). The dendrites have branches that are 0.5–5 μm in width depending on the growth conditions. The dendrite used as the template was prepared from the precursor solution containing 1.0 g of Cu(CH3COO)2·H2O and 1.0 g of PVA in 100 g of purified water (Figure 2a). The corresponding dendrite consisted of unit branches ~1 μm in width (Figures 3a and b). The XRD pattern of the Cu(CH3COO)2·H2O dendrites shows the intensified peaks related to the (010) plane (Figure 3c), with three types of branched angels, namely 63°, 61° and 56°. On the basis of these observations, the growth directions of the branches were estimated to be (001), (100) and (101) directions of monoclinic Cu(CH3COO)2·H2O crystals.

Figure 3
figure 3

Scanning electron microscopy (SEM) images (a, b) and X-ray diffraction (XRD) pattern (c) of a regular dendrite wherein (i) is the resultant Cu(CH3COO)2·H2O dendrite and (ii) shows the peak positions listed in the ICDD card as a template for morphogenesis formed at CCu=1.0 and CPVA=1.0.

Conversion from Cu(CH3COO)2·H2O dendrites to CuO dendritic shapes

The resultant Cu(CH3COO)2·H2O dendrites on a substrate were placed in a furnace maintained at 500 °C for 1 h in an air atmosphere. The color of the substrate changed from blue-green to black after the treatment (Figure 4a). The peaks of the XRD pattern were assigned to those of CuO (Figure 4a). The FT-IR spectra showed no absorption peaks resulting from the acetate group in the precursor Cu(CH3COO)2·H2O and hydroxy group in PVA (Figure 4b), suggesting that CuO was obtained with the combustion of PVA and decomposition of Cu(CH3COO)2·H2O. The macroscopic dendritic morphologies were maintained on the resultant CuO (Figure 4c). The magnified field-emission scanning electron microscopy images showed the branches consisting of the nanoparticles <100 nm in size (Figures 4d and e). The decomposition of the Cu(CH3COO)2·H2O crystal led to the granular CuO structures in the branches. When the precursor dendrite of Cu(CH3COO)2·H2O was heated from room temperature to 500 °C by a slower heating rate of 1°C min−1, the macroscopic dendritic shape collapsed with the combustion of PVA. Therefore, the rapid heating operation without the temperature rising step is required for the simultaneous removal of the acetate groups and PVA to keep the dendritic morphology. In the slower heating process, the prior combustion of PVA led to the collapse of the Cu(CH3COO)2·H2O dendritic morphology. The rapid heating process facilitated the decomposition of Cu(CH3COO)2·H2O to CuO prior to the combustion of PVA.

Figure 4
figure 4

Dendritic morphology of CuO. (a) X-ray diffraction (XRD) patterns of the resultant CuO dendritic shape (i) and the peak positions listed in the ICDD card (ii). (b) Fourier-transform infrared absorption (FT-IR) spectra of the resultant CuO (i), Cu(CH3COO)2·H2O (ii), and commercial poly(vinyl alcohol; PVA) (iii). (ce) Scanning electron microscopy (SEM) images of the CuO dendritic morphologies.

Conversion from CuO dendritic shapes to metallic Cu ones

The resultant CuO dendritic morphologies on a substrate were immersed in an aqueous solution containing 10 mmol dm−3 of DMAB for 3 h at room temperature. After the reaction, the color of the substrate changed from black to brown (the inset of Figure 5a). The macroscopic dendritic morphologies consisting of the nanocrystals <100 nm in size were maintained after the immersion in DMAB aqueous solution (Figures 5a and b). The Cu peaks were observed on the XRD pattern (Figure 5c), the reduction from CuO to Cu proceeded without the collapse of the dendritic morphologies. When hydrazine (N2H4) was used as a reducing agent, the morphologies were not maintained after the immersion in the solution. The morphology is not maintained in the aqueous solution of N2H4 as ammonia that is generated in the reduction processes promotes the dissolution of CuO, the low solubility of CuO in an aqueous solution of DMAB facilitates the gradual reduction to Cu without morphology alteration.

Figure 5
figure 5

Dendritic morphology of Cu. (a, b) Scanning electron microscopy (SEM) images of the resultant Cu dendritic shape. (c) X-ray diffraction (XRD) pattern of the resultant Cu dendritic shape (i) and the peak positions listed in the ICDD card (ii).

Formation of PPy on the surface of Cu(CH3COO)2·H2O dendrites

The resultant Cu(CH3COO)2·H2O dendrites on the substrate were put in a glass bottle containing a neat liquid of pyrrole (Py) at 60 °C for 24 h (Figures 1a and d). The vapor of Py monomer was supplied to the surface of Cu(CH3COO)2·H2O dendrites. The color of the substrate changed from blue-green to black. The FT-IR spectra showed the formation of PPy after the reaction (Figure 6a). The characteristic absorptions of PPy were observed on the resultant PPy.61, 62 After the dissolution of the copper-related compounds by HCl, the absorptions assigned to PPy and PVA were observed on the FT-IR spectra (the spectra (i) and (iii) in Figure 6a).63, 64, 65 The absorptions of PVA in the FT-IR spectra indicate the presence of the remaining PVA (the spectra (i) and (iv) in Figure 6a). In addition, the energy dispersive X-ray spectra show that the copper-related compounds were dissolved after the HCl treatment (Figure 7). The dendritic morphologies of Cu(CH3COO)2·H2O were maintained after the polymerization and subsequent dissolution of the original dendrite (Figures 6b–g), and the cross-sectional images suggest polymerization behavior (Figures 6h–j). The original Cu(CH3COO)2·H2O dendrites were formed in the PVA matrix film ~1 μm in thickness on the substrate (Figures 6e and h). After the polymerization, the thickness was increased to ~5 μm with the formation and incorporation of PPy in the PVA matrix film (Figures 6f and i). The oxidative polymerization of Py proceeds around the Cu(CH3COO)2·H2O dendrite including the PVA matrices through the diffusion of Py and the reduction of Cu(CH3COO)2·H2O (Figure 6i). The remaining unreacted Cu(CH3COO)2·H2O crystals and PVA matrices near the substrate are dissolved by the HCl treatment (Figures 6i and j). In contrast, the composite film of PPy and PVA remains after dissolution by HCl. The composite films of PPy and PVA with the hollow interior are obtained (Figures 6f, g, i and j). The formation of the composite with PVA involves the preservation of the PPy dendritic shape. In this way, the dendritic morphologies of the original Cu(CH3COO)2·H2O were replicated to PPy.

Figure 6
figure 6

Morphologies of polypyrrole (PPy) dendrites synthesized from the precursor Cu(CH3COO)2·H2O dendrite. (a) Fourier-transform infrared absorption (FT-IR) spectra of the polymerized sample before and after the dissolution of copper-related compounds with hydrochloric acid (HCl, i, ii), the commercial PPy (iii) and the commercial poly(vinyl alcohol; PVA) (iv). (bj) Scanning electron microscopy (SEM) images (bg) and schematic illustrations (hj) of the precursor dendrite of Cu(CH3COO)2·H2O (b, e, h) and the polymerized sample before (c, f, i) and after (d, g, j) the dissolution of copper-related compounds. The absorptions in the FT-IR spectra were assigned to the following vibrations of PPy (black arrows in a–e) and PVA (white arrows in f–h): (a) N-H stretching, (b) C=C stretching, (c) C-C in-ring stretching, (d) C-H ring out-of-plane bending, (e) C=C stretching, (f) O-H stretching vibrations in the polymeric species, (g) CH2 asymmetric stretching vibration and (h) CH2 deformation. A full color version of this figure is available at Polymer Journal online.

Figure 7
figure 7

Energy dispersive X-ray (EDX) spectra (a) and field-emission scanning electron microscopy (FESEM) image (b) of the polymerized samples before (i) and after (ii) dissolution of the copper-related compounds with hydrochloric acid (HCl). The Si and Na peaks were caused by glass substrates. The Os peak is ascribed to the conductive coating of amorphous osmium. The Cu peak was not detected after HCl treatment. The FESEM image in panel b corresponds to the area for the collection of the EDX spectrum in panel a.

Conclusion

The dendrites of Cu(CH3COO)2·H2O, a transition metal salt, were grown in a PVA matrix, which was facilitated by the diffusion-controlled condition within a polymer matrix. The dendritic morphologies of CuO with the porous structures were obtained by the thermal treatment of the original Cu(CH3COO)2·H2O dendrite. The subsequent reduction of the resultant CuO by using DMAB provided the metallic Cu with the dendritic shapes. The oxidative polymerization of Py was achieved on the Cu(CH3COO)2·H2O dendrites through the reduction of copper ions in the PVA matrix film. The dendritic morphology of PPy was obtained with the PVA matrix film after the dissolution of the copper-related compounds. In this way, the dendritic morphologies of CuO, Cu and PPy were obtained from the dendrites of Cu(CH3COO)2·H2O as the template. The present study shows that the approach can be applied to morphogenesis of a variety of metal oxides, metal and conductive polymers by using the morphology-controlled crystals of transition metal salts.