Debora
Marani
*ab,
Leticia Poras Reis
Moraes
c,
Fabrizio
Gualandris
a,
Simone
Sanna
a,
Daniel Zanetti
de Florio
b,
Vincenzo
Esposito
a and
Fabio Coral
Fonseca
c
aDepartment of Energy Conversion and Storage, Technical University of Denmark (DTU), Frederiksborgvej 399, Roskilde 4000, Denmark. E-mail: debora.marani3@gmail.com
bCentro de Engenharia Modelagem and Ciências Sociais Aplicadas, Universidade Fedearl do ABC, Av. Do Estados 5001, Santo André (SP), 09210-580, Brazil
cNuclear and Energy Research Institute (IPEN-CNEN/SP), 05508-000, São Paulo, SP, Brazil
First published on 15th February 2018
Herein we report for the first time the synthesis of ceramic–organic three-dimensional (3D) layered gadolinium-doped cerium oxide (Ce1−XGdXO2−δ, CGO) and its exfoliation into two-dimensional (2D) nanosheets. We adopt a water-based synthetic route via a homogenous precipitation approach at low temperatures (10–80 °C). The reaction conditions are tuned to investigate the effects of thermal energy on the final morphology. A low temperature (40 °C) morphological transition from nanoparticles (1D) to two-dimensional (2D) nanosheets is observed and associated with a low thermal energy transition of ca. 2.6 kJ mol−1. For the 3D-layered material, exfoliation experiments are conducted in water/ethanol solutions. Systems at volume fractions ranging from 0.15 to 0.35 are demonstrated to promote under ultrasonic treatment the delamination into 2D nanosheets.
However, the solution-based approach poses the challenge of synthesizing the starting 3D layered materials with the desired composition. Several synthetic strategies have been proposed in the literature for the preparation of 3D layered compounds. The different methods span from solid state reactions14 to hydrothermal processes,15 including the precipitation approach.16 This latter synthetic route has been extensively used in the synthesis of layered double hydroxides (LDHs) as it allows obtaining micrometer-sized and highly crystalline structures.16 It is a water-based synthetic route that makes use of urea or hexamethylenetetramine (HMT) as a pH regulator.17 The slow and progressive hydrolysis of urea and HMT makes it possible to attain a homogenous and controlled release of hydroxyl ions in solution.17 The reaction likely occurs at the 2D-nucleation front where the layers are formed. Typically, the homogeneous precipitation of layered materials proceeds through the nucleation of positively charged nanosheets followed by their assembly as layered materials via intercalation with negatively charged counter anions. This method has been successfully applied to synthesize layered materials other than LDHs,18–21 thus enabling other strategic applications.22,23
In this work, for the first time, gadolinium-doped cerium (CGO) oxides were synthesized as 3D layered materials via the homogenous precipitation approach at low temperatures (<40 °C). CGO materials were selected because of their relevance in diverse applications, including biomedical24 catalysis and environment and energy related technologies.25 The use of the water-based homogeneous precipitation route for the preparation of ceria-based oxides has already been reported.19,26,27 However, to the best of our knowledge, no investigations about the effect of the reaction conditions on the morphology of the final product have been reported.
The nucleation front for the formation of 2D CGO nanosheets was observed to occur at a relatively low thermal energy (∼2.6 kJ mol−1). Exfoliation experiments were also successfully conducted using a co-solvent approach.7–9
The morphology of the CGO materials was observed by field emission scanning electron microscopy (FESEM, Supra, Carl Zeiss, Germany) and by transmission electron microscopy (TEM, JEM3000F, Oxford Instruments, UK). The chemical composition of the samples was determined by energy-dispersive spectroscopy (EDS) coupled with FESEM.
At decreased temperatures, the typical peaks of a lamellar structure are then identified and associated with the plane (00l).28 Specific features are observed at different reaction temperatures. Indeed, while the peaks for lamellar and fluorite structures coexist in the XRD pattern of the CGO material prepared at 40 °C, a lamellar structure dominates the material when CGO is prepared at lower temperatures (e.g. 30 and 10 °C). It is worth clarifying that in the XRD patterns of CGO prepared at 10 °C and 30 °C, the presence of the peaks of the lamellar structure might not exclude the presence of the fluorite peaks. The intensity of the peaks of the interlayer planes might have overpowered the fluorite peaks, resulting in their absence in the mean XRD pattern. In contrast, when the synthesized material exhibited no layered structure, the fluorite peaks are observable, and are associated (in the current work) with the CGO nanoparticle formation.
The XRD patterns of the layered material were analysed, and the peaks were assigned to the corresponding diffraction planes (Fig. 1b). The basal spacing for the layered materials was estimated using Bragg's equation using the theta value of the (001) reflection. In Fig. 1b, sharp peaks equidistant from one another suggest highly developed and regular lamellar structures with an ∼2.4 nm spacing, as calculated from the XRD data. Such a relatively large spacing is consistent with the intercalation of the dodecyl sulfate anions (DS anions)18 and it is independent of the reaction temperature (10 and 30 °C). Yet, the increment of the peaks intensities with decreasing temperatures is indicative of a corresponding increase in crystallinity.
Fig. 2a–d show the FESEM images for the CGO10 prepared at different temperatures. The FESEM images are reported at different magnifications to emphasize both the morphological features and the effect of the reaction temperature. Fig. 2a shows that the material synthesized at 80 °C is composed of agglomerated nanoparticles of 5–10 nm. The particles were embedded in a polymeric formation (the dark area in Fig. 2a). This soft chemistry route was found to result in an intense yellow powder with good sintering properties, as reported elsewhere.26,27Fig. 2b shows CGO10 synthesized at 40 °C, where a mix of nanoparticles and fibrous layered structures are observed. Both CGO10 samples synthesized at 30 °C (Fig. 2c) and 10 °C (Fig. 2d) possess pure layered morphologies characterized by tubular fibrous structures. A rather homogenous dimensional distribution of the layered structures was observed for the CGO10 prepared at 30 °C. Decreasing the reaction temperature to 10 °C resulted in larger nanostructures. The CGO materials characterized by a layered morphology (including CGO prepared at 40°) exhibited a whitish appearance. These results indicate a transition from nanoparticles to 2D layers controlled by the reaction temperature.
In Fig. 2e, the elemental analysis for CGO10 is reported. A uniform distribution of gadolinium (Gd) is observed, confirming the introduction of Gd into the fluorite structure of cerium oxide (CeO2).
The morphology and crystallinity of the materials were further investigated by transmission electron microscopy. Fig. 3a shows a TEM micrograph of CGO10 prepared at 80 °C.
Fig. 3 TEM micrographs for CGO10 prepared at (a) 80 °C and (b)–(d) 30 °C, at different magnifications. The insets in (a) and (d) are SAED patterns. |
CGO particles with sizes of around 5 nm can be observed. The selected area electron diffraction (SAED) pattern, inset in Fig. 3a, suggests the short range (nanoscale) ordering characteristic of the fluorite phase. The tubular structure for the layered materials (CGO10 prepared at 30 °C) is confirmed in the TEM micrograph (Fig. 3b). A well-ordered and regular disposition of the lamellas into a 3D structure is identified (Fig. 3c), with a regular distance from one layer to another of around 4 nm.
The distance was evaluated by analysing the TEM images. In Fig. 3c, to make it observable, the number of inter-layers in 50 nm are indicated. The value estimated includes both the thickness of a single CGO nanosheet (∼1 nm) and the thickness of a dodecyl sulfate (DS) anion (∼2.4 nm, as obtained from the XRD pattern). Further, in Fig. 3d, a top view of the 3D structure indicates that the 2D stacked layers exhibit a well-defined organization of the atoms. This arrangement corresponds to the fluorite phase, as indicated by the selected-area electron diffraction (SAED) pattern (inset, Fig. 3d) and supported by a fringe spacing of 0.31 nm indexed to the (111) plane of the fluorite phase.
Electron diffraction (ED) enables us to identify the texture of a single fluorite CGO layer, which was not detected by the XRD analysis.
A dependence of the morphology on the reaction temperature is definitely observed. Such an effect can be reasonably associated with the thermal energy of the system, expressed as NAvogadro × k × T. At the lowest temperature, the thermal energy of the system is such as to enable the materials to be arranged into atomically thin 2D nanosheets. At higher values of temperature (e.g., 80 °C), the CGO system fails to retain the planar morphology because of the higher thermal energy, and it collapses into nanoparticles (1D). In this 2D–1D morphological transition, the threshold temperature is identified to be 40 °C, corresponding to a thermal energy of around 2.6 kJ mol−1. At this temperature, both 2D and 1D morphologies are observed. This threshold can be associated with a sort of instability for the nucleation front of the 2D morphology.
Interestingly, regardless of the morphology, all the materials synthesized are polycrystalline with a fluorite arrangement of the atoms (see Fig. 3a and d). This excludes any influence of the growth mechanism of the crystals on the temperature-dependent morphological transition, and it is thus reasonably ascribed to the thermal energy of the system.
No effect of composition (e.g., Gd doping level) was observed either on the 2D–1D morphological transition or on the temperature at which the transition occurred. In Fig. 4a, the XRD patterns for CGO20 obtained at three different reaction temperatures (30 °C, 40 °C and 80 °C) are reported. As already pointed out for CGO10, at increasing temperatures a clear transition from a pattern originating from the lamellar structures to the typical peaks of the fluorite phase (that identifies the nanoparticles) is observed. Again, at 40 °C, a mix of lamellar and fluorite peaks is detected, suggesting this value of temperature as a threshold in the 2D–1D transition. For the layered materials, an interlayer distance of around 2.4 nm is obtained, which is in agreement with the interlayer distance estimated for CGO10. The TEM micrographs for the CGO20 materials confirm both the nature of the nanoparticles and the lamellar structures for the products prepared at temperatures higher and lower than 40 °C, respectively (not shown). For brevity, herein, only the TEM micrograph of CGO20 prepared at 30 °C is shown (see Fig. 4b). A well-ordered lamellar structure is definitely observed with an average distance of around 4 nm, which is in agreement with the interlayer distance obtained for the CGO10 materials with the dodecyl sulfate anion intercalation.
Preliminary exfoliation experiments were carried out by sonicating the CGO10 layered structures prepared at 30 °C in a water/ethanol solvent. A number of publications have demonstrated that an efficient exfoliation process is only achieved by using solvents that can minimize the interfacial energetic cost. This is usually obtained when the surface tension of the solvent matches the energy associated with the 3D structures (e.g. the energy required to exfoliate the layered structure).7,29–31 The typical translucent aspect and the Tyndall effect, characteristic of nanosheet colloidal suspensions,29,32,33 were observed for the solutions at water/ethanol volume ratios varying from 0.15 to 0.35 (see Fig. 5b).
Fig. 5b shows a TEM micrograph of the CGO nanosheets dispersed in the colloidal solution. Lamellar structures characterized by lateral dimensions of hundreds of nanometres are observed. It is worth specifying that the thin nanosheets obtained are likely nanopackets containing a small number (<10) of stacked monolayers, as previously reported (Fig. 5).32,33
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