Ultrathin PbS Sheets by Two-Dimensional Oriented Attachment

See allHide authors and affiliations

Science  30 Jul 2010:
Vol. 329, Issue 5991, pp. 550-553
DOI: 10.1126/science.1188035


Controlling anisotropy is a key concept in the generation of complex functionality in advanced materials. For this concept, oriented attachment of nanocrystal building blocks, a self-assembly of particles into larger single-crystalline objects, is one of the most promising approaches in nanotechnology. We report here the two-dimensional oriented attachment of lead sulfide (PbS) nanocrystals into ultrathin single-crystal sheets with dimensions on the micrometer scale. We found that this process is initiated by cosolvents, which alter nucleation and growth rates during the primary nanocrystal formation, and is finally driven by dense packing of oleic acid ligands on {100} facets of PbS. The obtained nanosheets can be readily integrated in a photodetector device without further treatment.

Controlled assembly leading to anisotropic nanostructures poses a conceptual challenge in the field of materials research. Penn and Banfield et al. (1, 2) described crystal growth, in which oxide nanoparticles coalesce in well-defined crystalline orientations. Their method of oriented attachment of nanocrystals is now one of the most favorable techniques to grow linear or zig-zag–type one-dimensional (1D) nanostructures. In addition to strong size-quantization effects occurring in these structures, their big advantage is solution processability, which makes them attractive candidates for optoelectronic and thermoelectric applications in low-cost integrated systems. 1D assemblies of oriented attachment have been reported, and, in most cases, the anisotropy during self-assembly is caused by crystal planes with preferred reactivity and dipole moments in the crystallites. However, systems with cubic-crystal symmetry (such as PbS and PbSe), in which beautiful 1D oriented attachment occurs, are somewhat more difficult to explain. Oriented attachment, in this case, should result in 3D networks rather than 1D structures. The common explanation assumes that, despite the strict monodispersity of the samples, inhomogeneities in the chemical composition of surface planes exist and result in dipole moments within the nanocrystals. On the other hand, organic ligand molecules play a crucial role in such processes by capping nanoparticle surfaces selectively and may hinder, modify, or trigger an oriented attachment (3). In this work, we show that the formation of ordered and densely packed ligand surface layers of oleic acid on {100} PbS surfaces can drive the normally isotropic crystal growths into a 2D oriented attachment of nanocrystals. In addition, the presence of chlorine-containing cosolvents during the initial nucleation and growth process of the nanocrystals plays a prominent role.

Syntheses of lead chalcogenide nanoparticles (47) can lead to a large variety of particle shapes through slight changes of the reaction conditions. The mechanism of how small traces of organo-phosphine compounds may alter the course of the reactions has been reported, which underlines their complexity (8). For other systems, like CdS nanoparticles, shape control has been reported by the addition of small amounts of HCl (9) or chlorine-containing solvents such as 1,2-dichloroethane (DCE); for example, in the case of CdSe nanorods attached to carbon nanotubes (10). Reported strategies to generate 2D nanostructures are based on the use of lamellar-like templates (11) or thin superstructures by assembly (1214).

Our approach is based on a standard synthetic procedure to generate nearly spherical PbS nanoparticles (15). After 3 min, the resulting dotlike particles have a mean diameter of ~5 nm. In contrast, ultrathin PbS nanosheets, as depicted in Fig. 1, are formed in the presence of chlorine-containing compounds such as DCE or similar linear chloroalkanes (fig. S1). The nanosheets have lateral dimensions of several hundred nanometers and stack showing Moiré patterns caused by the interference between the crystalline lattices of the individual sheets (see fig. S2 for Moiré patterns and corresponding simulations). The formation of the sheets occurs within the first 1 to 3 min of the reaction. To investigate the mechanism of formation, we followed the temporal evolution of the sheets by optical spectroscopy and high-resolution transmission electron microscopy (HRTEM). For practical reasons, we slowed down the sheet formation by reducing the reaction temperature to 70°C immediately after the thioacetamide injection [see the supporting online material (SOM)]. Figure 2A shows the absorption and emission spectra at various stages of the reaction. Within the first 50 s, the solution turned reddish brown, and clearly structured spectra evolved with an absorption maximum at 675 nm and a narrow emission band at 790 nm. These features indicate small, isolated quantum dots of 2.8 ± 0.5 nm, which can clearly be identified by TEM (fig. S3). As the reaction evolved, the fluorescence band of the quantum dots decreased, and an unstructured absorption of sheets arose, partially due to the occurrence of turbidity. However, the spectral position of the original bands, and, thus, the size of the particles, do not change during this process, proving that sheets are formed directly from the nanoparticles by oriented attachment. The growth of either ultrathin sheets or larger particles (in the absence of chlorine-containing compounds) is determined by the behavior of the PbS nanocrystals that originally formed.

Fig. 1

TEM image of stacked PbS nanosheets using 1,1,2-trichloroethane.

Fig. 2

(A) Absorption and emission spectra of the nanoparticles with reaction time. The absorption spectra were normalized to the absorption at 400 nm, and the emission spectra to the maximum of each curve. a.u., arbitrary units. (B) TEM image of an ultrasmall PbS nanoparticle at early stages of the reaction. (Inset) Model structure of a truncated cuboctahedron. (C) First step of attachment. (D) Later, the structures merge with some holes due to nonideal attachment. (E) At the end of the synthesis, quasi-continuous sheets are formed. (Inset) Electron diffraction pattern of the PbS sheets.

Nanocrystals as small as 2.8 nm could not be isolated if DCE (or a similar chlorine-containing compound) was not added to the reaction mixture. A TEM sample taken during the rapid process of oriented attachment shows various stages of sheet formation. The original particles (Fig. 2B) can be recognized together with fused aggregates (Fig. 2C), as well as porous structures similar to the one shown in Fig. 2D. In Fig. 2B, in which an individual particle in a slightly tilted [100] orientation is depicted, an angle of 135° at the crystalline edges can be identified. This is taken as an indication of the presence of {110} surface planes. A reasonable model for such a small crystallite is shown in the inset of this figure. A close inspection of Fig. 2C identifies this structure as an aggregate of three nanocrystals fused in two dimensions. Even in the porous framework structure of Fig. 2D, the size and shape of the original particles, as well as their crystalline orientation, is visible (figs. S4 to S6). Uniform nanosheets, however, can be obtained several minutes after the sulfur precursor injection (Fig. 2E; see SOM for synthetic details). The HRTEM image of a sheet region depicted in Fig. 2E shows a single-crystalline structure with crossed (200) lattice planes displaying an angle of 45° relative to the sheet edges. This indicates a sheet growth parallel to the <110> axes. Although most of their edges in <110> directions are atomically flat over large distances, some regions clearly show a zig-zag pattern with exposed {100} facets with dimensions corresponding to those of the original quantum dots. Selected-area electron diffraction pattern of individual sheets confirms this observation, showing a monocrystalline galena structure in [100] orientation with pronounced (200) and (220) reflexes. The x-ray diffraction pattern shows that the HRTEM characterization of individual sheets is representative of the entire sample (fig. S8).

In the crystalline-equivalent PbSe and PbTe systems, Murray et al. discovered that truncated cubes with sizes of ~10 nm evolve from ~5-nm cuboctahedrons with six {100} and eight {111} facets. They explained this result by a faster growth-rate perpendicular to the {111} facets (16, 17). Their findings also suggest that {110} facets are highly reactive and, therefore, are preferentially consumed during the nanoparticle growth. The structure of PbS nanocrystals that merge into PbS sheets is shown in Fig. 3. The shape is that of a truncated cuboctahedron with 6 {100}, 8 {111}, and 12 {110} facets. Upon crystal growth, the particles try to minimize the most energetically unfavorable surface facets by fast growth perpendicular to the respective facet. In the case of PbS particles larger than 10 nm (18), this results in truncated cubes with mainly {100} surface planes (path A in Fig. 3). We do not observe the formation of PbS sheets in the absence of DCE (or a similar chloride compound), whereas in the presence of chloride compounds, which are known to act as lead complexing agents (19), the kinetics of nucleation and growth are altered, leading to ~3-nm particles (as shown in Fig. 2B), which should still exhibit the reactive {110} surfaces. Because Ostwald ripening plays only a negligible role during PbS nanoparticle formation, these small crystallites stabilize by oriented attachment via the {110} facets (path B in Fig. 3). The expected egg tray–like structure is unlikely to be stable and will undergo a surface reconstruction (path C in Fig. 3), resulting in a flat sheet (Fig. 2E). The ensuing sheet should be thinner than the original building blocks by up to 30%. This reconstruction, understood as the diffusion and accommodation of the atoms under favorable thermodynamic conditions (100°C), also contributes to a decrease in the porosity of the sheets. We performed small-angle x-ray scattering (SAXS) of the stacked PbS layers (Fig. 4). The sample was positioned in a coplanar configuration with the SAXS beam to obtain information about the sheet thickness and orientational distribution. A highly anisotropic dumbbell-type scattering pattern characteristic for sheets oriented nearly parallel to the qx direction can be seen in the upper-left inset of Fig. 4. The best simulation fit was calculated assuming a regular stacking of disks with a long period of 5.8 nm and PbS sheet thickness of 2.2 nm. The resultant distance between the sheets of 3.6 nm is attributed to an oleic acid bilayer. This behavior strongly supports the notion of an interplanar crystalline oleic acid bilayer, which is not interpretable by randomly coiled and interpenetrating chains. The formation of the stacked layers occurs most probably by an attachment of quantum dots or small-sheet structures on top of already formed nanosheets, which then act as a nucleus for further 2D attachment. The stacked structure can also be observed by atomic force microscopy (fig. S9).

Fig. 3

Schematic illustration of large-particle (A) and sheet formation (B and C) from small PbS quantum dots.

Fig. 4

Cross section of the scattering intensity along the qy axis (black points) and simulated diffraction curve (red). The scattering image is depicted in the upper-left inset. The highly anisotropic dumbbell-type scattering pattern is characteristic for sheets oriented nearly parallel to the qx direction. The result could be modeled with assumed disks of 2.2-nm thickness and a spacing ligand of 3.6 nm, as depicted in the lower-right diagram.

One question remains, however, as to why oriented attachment leads to 2D structures rather than 3D structures. Our results strongly support the idea that the assembly of oleic acid in a highly ordered monolayer on the {100} surfaces plays a key role in the formation and further stacking of PbS sheets. Oleic acid is well known to assemble vertically on various substrates and to form bilayer structures (2022). The thickness of a monolayer was determined from single-crystal data and ranges from 1.7 to 2.4 nm in the reported crystal structures. The latter mainly varies by the conformation next to the double bond and the relative orientation of the oleic acids within one monolayer. These reported values fit well with the observed interplanar distance of 3.6 nm in stacked sheets. The formation of a dense and highly ordered oleic acid layer covering the PbS nanosheets also allows the system to bind a maximum number of oleic acid molecules. The resulting release of adsorption enthalpy, combined with the stabilization by interalkyl van der Waals forces, obviously overcompensates for the decrease in entropy and results in a net release of Gibbs energy. The 2D oriented attachment and the reconstruction from the egg-tray structure to flat sheets would, from this point of view, not only be driven by minimizing high-energy surfaces, but also by structural changes caused by the oleic acid molecules. Whereas one expects the ligands to exist in a randomly coiled state on the highly curved surface of small particles, they instead appear in a highly ordered phase on the flat {100} planes. In general, we believe that similar effects may hold in shape control, self-assembly, and templated growth of nanocrystals. For example, ligand-driven self-assembly of nanocrystals into aggregated wires (1D) and vesicles (curved 2D) was recently observed for amphiphilic CdSe quantum dots (23).

The thin-film structure of the sheets should decisively affect the quantum confinement of photogenerated carriers. In accordance with the reported dimensions, no confinement is expected in the lateral direction, whereas the structures should be strongly confined vertically. Differences in layer thickness and confinement in one dimension may strongly influence the optical features. Correlated confocal microscopy and TEM inspections (fig. S10) confirm this assumption by showing an emission signal coming from two different individual stacks of PbS sheets at a wavelength of ~720 nm.

Nanoparticle arrays are currently in the spotlight for low-cost device fabrication, like photodetectors (2429). Typical 2D assemblies require physical or chemical treatments to remove the insulating organic shell capping. The lack of ligands in the in-plane dimensions of raw PbS 2D sheets produces intrinsically outstanding photoconductive properties, as shown in Fig. 5. PbS sheets bridging two gold electrodes on a SiO2 substrate exhibit low, dark conductance between ±0.1 V without substantial hysteresis. Upon illumination with a 532-nm laser, however, the conductance increases by more than two orders of magnitude at an illumination intensity of 2.0 mW/cm2. This yields an efficiency value (actual photocurrent divided by the theoretical maximum current due to photon impact) of ~1.1 at 0.1 V (which corresponds to a responsivity of 0.472 A/W). Taking into account that the number of absorbed photons is only a small fraction of the incident, this value shows that the increase in current cannot be due to harvesting of photogenerated charge carriers only. The filling of trap states is most probably responsible for the current gain. In contrast to currently investigated devices made from ligand-stabilized PbS nanocrystals, the ready-made, nontreated nanosheets reported here are remarkably conductive due to missing in-plane ligands and continuous connection through the monocrystal.

Fig. 5

Current-voltage curves of PbS sheets with (red) and without (blue) illumination with a green laser. The thin film of stacks of PbS sheets covers a detection area of 0.5 by 6 μm between two gold electrodes. (Inset) Current-voltage curves on logarithmic scale.

We have shown that chlorine-containing cosolvents can direct the colloidal synthesis of PbS nanoparticles into 2D nanosheets by oriented attachment. We believe that this is a consequence of the size of the nanoparticles and, hence, the presence of {110} reactive facets, which disappear as the nanoparticles grow. The presence of DCE or similar chlorine-containing compounds yields small nanoparticles of ~3 nm in diameter, exposing the highly reactive {110} facets so as to trigger an oriented-attachment process. Both the oriented attachment and the strong crystalline correlation between the nanosheets in stacked aggregates are most likely driven by the formation of a highly ordered oleic acid bilayer between the PbS nanosheets. The absence of ligands in the in-plane direction of the ultrathin sheets yields a prominent photoconductivity response in the pristine dried nanomaterial.

Supporting Online Material

Materials and Methods

Figs. S1 to S11


References and Notes

  1. B.H.J. thanks the European Commission for grant ERG FP7-PEOPLE-ERG-2008 and the Spanish Ministry of Science and Innovation for grant RYC-2007-01709.
View Abstract

Navigate This Article