A protocol for the synthesis of In37P20(O2C14H27)51 clusters and their conversion to indium phosphide quantum dots is presented.
This text presents a method for the synthesis of In37P20(O2C14H27)51 clusters and their conversion to indium phosphide quantum dots. The In37P20(O2CR)51 clusters have been observed as intermediates in the synthesis of InP quantum dots from molecular precursors (In(O2CR)3, HO2CR, and P(SiMe3)3) and may be isolated as a pure reagent for subsequent study and use as a single-source precursor. These clusters readily convert to crystalline and relatively monodisperse samples of quasi-spherical InP quantum dots when subjected to thermolysis conditions in the absence of additional precursors above 200 °C. The optical properties, morphology, and structure of both the clusters and quantum dots are confirmed using UV-Vis spectroscopy, photoluminescence spectroscopy, transmission electron microscopy, and powder X-ray diffraction. The molecular symmetry of the clusters is additionally confirmed by solution-phase 31P NMR spectroscopy. This protocol demonstrates the preparation and isolation of atomically-precise InP clusters, and their reliable and scalable conversion to InP QDs.
Colloidal semiconductor quantum dots have seen an acceleration in synthetic development over the previous three decades owing to their potential in a variety of optoelectronic applications including displays1, solid-state lighting2,3, biological imaging4,5, catalysis6,7, and photovoltaics8,9,10. Given their recent commercial success in the area of wide-color gamut displays, the quantum dot market is expected to exceed 16 billion dollars by 202811. A significant shift in material focus from the II-VI (and IV-VI) to the III-V family has occurred in the last several years as the search for less toxic, Cd and Pb-free alternatives for use in highly distributed electronics applications has begun. Indium phosphide in particular has been identified as a leading drop-in replacement for CdSe12. It has become apparent, however, that optimization of InP-based quantum dots is more difficult and does not always benefit from the same methods used for the more well-established chalcogenide materials. This is primarily because the nucleation and growth profile of InP nanoparticles follows a non-classical, two-step mechanism13. This mechanism is invoked due to the intermediacy of locally stable, atomically precise intermediates known as “magic-sized” clusters14,15,16. In particular, In37P20(O2CR)51 has been identified as one key, isolable intermediate in the synthesis of InP from P(SiMe3)3, indium carboxylate, and carboxylic acid17.
The presence of this intermediate on the reaction coordinate has many tangible effects on the growth of InP nanostructures. The existence of cluster intermediates themselves invalidates classical concepts of nucleation and growth based on the La Mer model and means that optimizing reaction conditions such as concentration, temperature, and precursor may not achieve sufficiently uniform ensemble properties. Rather, it has been shown that the use of the InP cluster as a single-source precursor results in highly monodisperse quantum dots with narrow optical features13. Recent literature has suggested that monodispersity, however, is not the only factor limiting InP’s parity with other optoelectronic materials18. Surface defects, oxidation, and alloying are critical factors still under intense research that will require significant innovation for optimized InP architectures19,20,21,22,23,24. The atomically precise nature of clusters, such as In37P20(O2CR)51, makes them ideal platforms for probing the consequences of many post-synthetic surface modifications. Normally, ensemble inhomogeneity of nanoparticles makes determining surface and compositional effects difficult, but because the cluster of InP is known to be atomically precise, both compositionally and crystallographically, it is an ideal model system.
The synthesis of the In37P20(O2CR)51 cluster is no more difficult than the synthesis of more widely used nanoparticles such as CdSe, PbS, or ZnO. It requires only standard glassware, widely available chemicals, and basic knowledge of air-free Schlenk and glovebox techniques. The procedure itself can be done on the gram scale and with yields in excess of 90%. As we will show, the successful synthesis of InP cluster is not “magic” but rather an exercise in fundamentals. Pure reagents, dry glassware, proper air-free techniques, and attention to detail are all that is required to access this atomically precise nanocluster. Moreover, we also elaborate on ideal methods for its conversion to highly crystalline InP quantum dots with narrow size distributions.
CAUTION: Proper personal protective equipment should be worn at all times and the material safety data sheet (MSDS) should be read for each chemical prior to use. All steps should be done air-free, because exposing clusters to air and/or water will degrade clusters or prevent proper formation. Any point at which the reaction flask is open to air, N2 should be flowing vigorously to create a protective blanket over the reagents in the flask. All N2 used should be 99.9% or greater in purity.
1. Preparation of molecular precursors
2. Synthesis of In37P20(O2CR)51
3. Workup of In37P20(O2CR)51
NOTE: All solvents used in the purification steps are anhydrous and stored over 4 Å sieves in the N2-filled glovebox.
4. Synthesis of InP quantum dots using In37P20(O2CR)51 as a single source precursor
NOTE: Indium phosphide quantum dots can be synthesized from purified InP clusters using a heat-up or hot injection method.
5. Characterization of In37P20(O2CR)51 and InP quantum dots
InP clusters and quantum dots are characterized by UV-Vis absorption and PL spectroscopy, XRD, TEM, and NMR spectroscopy. For the InP clusters, an asymmetric absorption feature is observed, with a peak maximum at 386 nm (Figure 1a). Despite the true monodispersity of the sample, this lowest energy peak exhibits a broad linewidth, which narrows upon decrease in temperature. This has been attributed to a set of discrete electronic transitions that are specific to the vibrational motions of the low-symmetry nanocluster lattice17. No appreciable PL QY is observed for clusters at 298 K despite the lack of obvious trap states that would arise from undercoordinated indium or phosphorus ions.
The non-stoichiometric, In-rich cluster (where In is present in a 1.85:1 ratio relative to phosphorus) results in a structure that corresponds with neither the zinc blende nor the wurzite XRD patterns of bulk InP (Figure 1b). Instead, the InP clusters attain a low-symmetry, pseudo-C2v structure that is best described by a set of intersecting polytwistane units25. The core diameter is in the 1-2 nm range depending on the axis from which it is viewed (Figure 1c). This low symmetry structure is reflected in the solution-phase 31P NMR spectrum of the cluster. The 31P NMR spectrum of myristate-capped InP clusters shows 11 distinct peaks (2 P atoms on the C2 axis that each give a unique peak and the remaining 18 P each have a symmetry equivalent, resulting in an additional 9 peaks) ranging from -187 to -242 ppm (Figure 1d)26. The broadness observed in the 31P NMR spectrum varies as a function of solvent and concentration, and purification method as has been recently described for related nanoscale systems27.
The optical spectra of InP QDs synthesized from clusters using the method described here display a lowest energy excitonic transition (LEET) at 564 nm and the corresponding PL emission peak at 598 nm with a full width at half maximum of 52 nm and trap emission evident at redder wavelengths (Figure 2a). It is worth noting that while the two synthetic methods (heat-up and hot-injection) yield InP QDs of comparable optical quality, the hot injection method typically leads to a sample with higher monodispersity due to the rapid nucleation at elevated temperature13. The typically low PL quantum yields obtained directly from the synthesis without further surface treatment (shelling, F- etching, or Lewis acid coordination) are hypothesized to result from a mixture of hole and electron traps present at the surface of these nanocrystals18,28. The XRD pattern of the resultant InP QDs confirms the zinc blende phase (Figure 2b). Peak broadening in the XRD data occurs due to the finite size of the highly crystalline structures, which in the case of InP QDs is 3.1 nm +/- 0.5 nm in diameter (Figure 2c, a size histogram can be found in ref. 13).
Figure 1. Representative characterization data for InP clusters. (A) UV-Vis spectrum of InP clusters. (B) XRD pattern for purified InP clusters showing deviation from the expected bulk zinc blende (black trace) and wurtzite (grey trace) InP pattern. (C) TEM image of isolated InP clusters. (D) 31P NMR spectrum of InP clusters collected at 202 MHz in C6D6 at 298 K. Please click here to view a larger version of this figure.
Figure 2. Representative characterization data for InP quantum dots prepared from InP clusters. (A) UV-Vis (solid) and PL (dotted) spectra of InP QDs prepared from myristate-capped InP clusters using the hot-injection protocol. (B) XRD pattern of purified InP QDs showing agreement with the bulk zinc blende InP pattern. (C) TEM images of InP QDs grown from clusters using the hot-injection protocol. Please click here to view a larger version of this figure.
The synthesis of InP magic-sized clusters and their conversion into quantum dots follow straightforward procedures that have been shown to consistently produce high quality samples. The ability to synthesize and isolate InP clusters as an intermediate has distinct advantages in terms of subjecting these nanostructures to modifications that can be well-characterized and consequently be incorporated in the final QDs. The atomically precise nature of the clusters and the high reproducibility provide a platform for innovative studies in surface modifications, defects, and alloying of the InP systems and open doors to a wide range of applications such as in displays, solid-state lighting, catalysis, and photovoltaics.
In the synthesis of InP clusters, it is critical that all reagents are of high purity and thoroughly dried, as the success of the synthesis is contingent upon water- and air-free experimental conditions and purity of the precursors for uniform growth in high yields. Additionally, it is recommended that sufficient precautions are taken when handling P(SiMe3)3, which is light-sensitive and pyrophoric. This reagent should be stored in a light-, air-, and water-free environment and caution should be taken to prevent air and water exposure before and during the reaction. For efficient growth of the clusters, the temperature range should be 100-110 °C; at room temperature, the growth is extremely slow, and a higher temperature will result in conversion into quantum dots of varying sizes depending on the temperature. The presented protocol is also highly scalable and versatile, allowing synthetic control and modifications through a breadth of parameters. The myristic acid used as the ligands for InP clusters and subsequent QDs can be replaced by phenylacetic acid, oleic acid, or other short and long-chain carboxylic acids. Post-synthetic addition of P(SiMe3)3 to solutions of InP clusters that have slightly perturbed absorption features (red-shifted and/or broadened) has been observed to result in a size focusing effect where the consumption of excess indium myristate results in a ~3 nm blueshift in the absorption spectra29.
The purification method of the clusters has been empirically optimized in our lab to avoid oxidation and to isolate the highest possible yields. The choice of acetonitrile as the antisolvent and its volume ratio with toluene fulfill these goals. Finally, the clusters are resuspended in minimal amount of toluene and centrifuged to remove any solid impurities that may have resulted during synthesis. Removing toluene from the final solution gives a yellow paste that can be stored for at least 36 months under air- and water-free conditions. It should also be noted in regard to preparing NMR samples for characterization of the purified product that the precise chemical shifts for the 11 distinct resonances in 31P NMR spectrum vary depending on the identity of the indium precursors. Furthermore, insufficient purification and variation in cluster concentration can result in line broadening. In order to obtain a clean spectrum with sharp features, it is suggested that at least 40 mg of the cluster is dissolved in a minimal amount of anhydrous C6D6 (~0.7 mL).
Similarly, the synthesis of InP QDs via clusters must be performed under water- and air-free conditions. Previous studies have shown that the presence of water in indium precursors and the addition of trace amounts of water or hydroxide lead to significant changes in the growth of InP QDs and the surface chemistry of the final product25. When running the reaction at a different scale than described in the protocol, it should be noted that for the hot-inject method, the cluster solution for injection should be sufficiently concentrated and the volume should be smaller compared to the heated solvent in the flask. This is to minimize the abrupt decrease in temperature as the reaction temperature profile plays a nontrivial role in the synthesis. Detailed work on the conversion mechanism of InP clusters to QDs has been recently reported where the effects of the addition of different precursors (i.e., carboxylic acid, indium carboxylate), temperatures, and concentration have been explored30. Through these studies, it has been revealed that thermolysis temperatures > 220 °C are required for obtaining high yields of optimal quality QDs. The purification of InP QDs follows similar logic and process as mentioned above for the clusters, except that the storage of purified QDs is recommended in solution with a solvent such as toluene. In solid form, the QDs have been observed to form aggregates over time, preventing homogeneous colloidal dispersion. One final note regarding the protocol is that removing 1-octadecene by vacuum distillation after the synthesis of InP QDs rather than by only precipitation-redissolution is a recommended first step of QD purification. This is to limit the volume of solvent required in the workup and because the residual ODE may interdigitate with the long-chain carboxylate ligand shell, causing difficulties with sample preparation for characterization and subsequent use.
We have demonstrated the synthesis and characterization of atomically-precise InP magic-size clusters, In37P20(O2CR)51, and their use as single source precursors for the synthesis of InP quantum dots using both heat-up and hot-injection methods. The reported synthesis of InP clusters is versatile and can be generalized to a wide range of alkyl carboxylate ligands. The synthesis of the InP QDs from the clusters provides a highly reproducible method for the synthesis of these challenging nanostructures with high quality in terms of size distribution and crystallinity. Opportunities abound for further elaboration of this method through post-synthetic modification of the clusters themselves and for engineering the cluster to quantum dot conversion strategy. Because of this, we believe these methods are useful and potentially technologically meaningful for the synthesis of InP and related emissive materials for display and lighting applications.
The authors have nothing to disclose.
We gratefully acknowledge support from the National Science Foundation under grant CHE-1552164 for development of the original synthesis and characterization methods presented in this manuscript. During preparation of this manuscript, we acknowledge the following agencies for support of student and postdoctoral salaries: Nayon Park (National Science Foundation, CHE-1552164), Madison Monahan (US Department of Energy, Office of Science, Office of Basic Energy Sciences, as part of the Energy Frontier Research Centers program: CSSAS–The Center for the Science of Synthesis Across Scales under Award Number DE-SC0019288), Andrew Ritchhart (National Science Foundation, CHE-1552164), Max R. Friedfeld (Washington Research Foundation).
Acetonitrile, anhydrous, 99.8% | Sigma Aldrich | 271004 | Dried over 4Å sieves |
Adapter, Airfree, 14/20 Joint, 0 – 4mm Chem-Cap (T-adapter) | Chemglass Life Sciences LLC | AF-0501-01 | |
Adapter, Inlet, 14/20 Inner Joint | Chemglass Life Sciences LLC | CG-1014-14 | |
Bio-Beads S-X1, 200-400 mesh | Bio-Rad Laboratories | 152-2150 | |
Cary 5000 UV-Vis-NIR | Agilent | ||
Column, Chromatography, 24/40 Outer Joint, 3/4in ID X 10in E.L., 2mm Stpk | Chemglass Life Sciences LLC | CG-1188-06 | |
Condenser, Liebig, 185mm, 14/20 Top Outer, 14/20 Lower Inner, 110mm Jacket Length |
Chemglass Life Sciences LLC | CG-1218-A-20 | |
Distilling heads, short paths, jacketed | Chemglass Life Sciences LLC | CG-1240 | |
Eppendorf Microcentrifuge 5430 | Fisher Chemical | 05-100-177 | |
Falcon 15mL Conical Centrifuge Tubes | Fisher Chemical | 14-959-49B | |
Flask, Round Bottom, 50mL, Heavy Wall, 14/20 – 14/20, 3-Neck, Angled 20° | Chemglass Life Sciences LLC | CG-1524-A-05 | |
ImageJ | Developed at National Institutes of Health and the Laboratory for Optical and Computational Instrumentation | Open source Java image processing program | |
Indium acetate, 99.99% | Sigma Aldrich | 510270 | |
Myristic acid, 99% | Sigma Aldrich | M3128 | |
Temperature controller | Fisher Chemical | 50 401 831 | |
Thermometers, non-mercury, 10/18 | Chemglass Life Sciences LLC | CG-3508-N | |
Thermowell, 14/20 Inner Jt, 1/2" OD above the Jt, 6mm OD Round Bottomed Tube below the Jt, for 25ml RBF | Chemglass Life Sciences LLC | UW-1205-171JS | Custom ordered |
Toluene, anhydrous, 99.8% | Sigma Aldrich | 244511 | Dried over 4Å sieves |
Trimethylindium, 98% | Strem | 49-2010 | Heat sensitive, moisture sensitive |
Tris(trimethylsilyl)phosphine | Ref #31, 32 | Pyrophoric | |
Ultrathin Carbon Film on Lacey Carbon Support Film, 400 mesh, Copper | Ted Pella Inc. | 1824 | |
Vacuum gauge 1-STA 115VAC 60Hz | Fisher Chemical | 11 278 | |
Vacuum pump 115VAC 60Hz | Fisher Chemical | 01 096 | |
1-Octadecene (ODE), 90% | Sigma Aldrich | O806 | Technical grade, distilled and dried over 4Å sieves |