Introduction

Thiolate-protected noble metal (e.g., Au and Ag) nanoclusters (NCs) are ultrasmall particles with a core size of 2 nm and lower1,2,3. They can be denoted as Mn(SR)m where n and m are respectively the numbers of metal atoms and thiolate ligands. Particles in this size range have strong quantum confinement effects2,4 and exhibit interesting molecular-like properties such as strong luminescence5,6,7,8,9,10,11,12 and enhanced catalytic activity13,14,15. Hence noble metal NCs could increase the diversity in functional materials for biomedical and catalytic applications. The physical and chemical properties of the NCs are dictated by their composition, size and structure. Recent advances in NC chemistry have provided effective synthesis methods which can produce NCs with specific and tailorable attributes (e.g., composition16,17,18,19, size10,20,21,22,23,24,25,26,27 and structure28,29).

Further customizations of cluster properties could be realized by constructing a higher order nanostructure via the assembly of discrete NCs. It is well-documented in the nanoparticle (NP, with core size > 3 nm) literature that close-packed assemblies of NPs may lead to enhanced and/or new collective properties30,31,32. Other than a means for property tuning, NC assembly also contributes to the total structure determination of NCs since the ordered assembly (crystallization) of NCs into a perfect single crystal enables the cluster structure analysis by X-ray crystallography33,34,35,36,37. Therefore, the development of effective and general approaches to assemble metal NCs is of interest to both basic and applied research.

The assembly of the relatively large metal NPs (>3 nm) is relatively well-established. A large number of NP assemblies with different diameters, geometries and hierarchies have been demonstrated38,39,40,41,42,43,44,45,46,47. By comparison the assembly of ultrasmall metal NCs is a more recent development. Only a few Au NC species protected by aromatic thiolate/phosphine ligands have been assembled in organic solvents to date33,34,35,36,37,48. There are still no reports on the assembly of hydrophilic metal NCs in aqueous solution. The hydrophilic thiolate ligands on the NC surface do not contain the rigid aromatic rings which drive the assembly of Au NCs in organic solution through strong π-π interactions9,25,49. On the other hand the hydrophilic thiolate ligands on the NC surface may contain functionalities such as the carboxyl group (–COOH) which, upon deprotonation, can impart the NCs with a negative charge in aqueous solution20,21. Due to a very high ligand-to-metal ratio (~0.4 to 1 typically)25,50 and an ultrasmall size (<2 nm), a high charge density can be developed on the surface of the NCs. The high charge density and well-defined (atomically precise) size and structure (e.g., spherical) qualify the hydrophilic metal NCs as a new family of ion mimics (“nanoions”) in the aqueous phase. We hypothesize that the ion-like features (high charge density and well-defined size and structure) could promote strong electrostatic interactions between the hydrophilic metal NCs and counter cations, in ways similar to the formation of ionic crystals from real ions.

Herein, we report a facile method to assemble negatively-charged metal NCs in water via the electrostatic interactions between the dissociated carboxyl groups on the NC surface and divalent counter cations (e.g., Zn2+ and Cd2+) which are introduced to the solution. The divalent metal cations are used to electrostatically cross-link the negatively-charged NCs into large assemblies. An interesting ion-like behavior of the charged NCs was observed, where the assembly of NCs occurred in a step fashion and only when the metal-ion-to-thiolate-ligand ratio (denoted as R[M]/[-SR]) exceeded specific threshold values. The NC assemblies formed as such were spherical, fractal-like; and monodisperse in shape and size. The difference from the random aggregation of large colloidal NPs by counter ions is distinct and also suggests a high order of regularity in the assembly structure which is more akin to the formation of ionic crystals from real ions in solution. More interestingly, photoluminescence (PL) of the NCs was significantly enhanced after assembly, implying the existence of strong synergistic effects between the close-packed NC building blocks.

Results

Zn2+-induced assembly of Au NCs

As a proof-of-concept, highly luminescent Au NCs protected by the tripeptide glutathione (GSH or GS-H) were chosen as the model nanoion. The as-synthesized Au NCs showed strong orange emission which peaked at a wavelength of ~610 nm. As shown in Figure 1a, the orange-emitting Au NCs were small spheres with a core size below 2 nm. The Au NCs synthesized as such had a high GSH content on the NC surface (the GSH-to-Au-atom ratio was ~0.84 as reported in a previous study)8. The GSH ligands are likely to be present as oligomeric GS-[Au(I)-SG]n motifs8 on the NC surface and determine the charge and surface properties of the Au NCs. Each GSH moiety carries two carboxyl groups with pKa below 451. Hence at the near neutral condition of pH 6.5 in our experiments, all of the carboxyl groups on the NC surface were deprotonated to give rise to a negative charge on the Au NCs. The ζ-potential plot in Supplementary Fig. S1 (see Supplementary Information) illustrates the pH dependence of the charge on the Au NCs.

Figure 1
figure 1

(a–d) TEM images of Au NCs assembled in different Zn2+concentrations: R[Zn2+]/[-SG] = 0 (a), 0.3 (b), 0.6 (c) and 0.9 (d); the insets in (c) and (d) show the corresponding HR-TEM images (scale bar = 20 nm); (e) DLS analysis of Au NCs assembled at R[Zn2+]/[-SG] = 0 (black), 0.3 (red), 0.6 (blue) and 0.9 (green); the inset shows the dependence of the hydrodynamic diameter of the assembly on R[Zn2+]/[-SG].

Zn2+ was the counter cation used in this study. Zn2+ carries two positive charges and can electrostatically bind to two monovalent –COO anions. Therefore, Zn2+ can be used as a bifunctional cross-linker to electrostatically bridge between two negatively-charged Au NCs to build large NC assemblies. In a typical Zn2+-induced NC assembly, 1 mL of Au NCs at an optimized concentration of 0.46 mM [on Au atom basis as determined by inductively coupled plasma mass spectrometry (ICP-MS)] was mixed with 0.25 mL of ZnCl2 solution at a given concentration. The pH of the mixture was brought to ~6.5 by the addition of 0.1 M NaOH. The solution was well-mixed in a vortex mixer (1500 rpm, 30 s) and kept at room temperature for ~15 min to allow the reaction to complete. The procedure was repeated by using different concentrations of ZnCl2 while keeping the concentration of the Au NCs constant.

The size of the assembled NCs formed with different concentrations of Zn2+ was analyzed by transmission electron microscopy (TEM) and dynamic light scattering (DLS). The degree of assembly was determined by the ratio of divalent cations (Zn2+) to negatively-charged NCs (poly-anions). Since the latter depends on the GSH ligands on the NC surface, a controllable experimental variable would be the ratio of divalent cation (Zn2+) to GSH on the Au NC surface (taking into account that there are two carboxylate anions in one GSH moiety), termed as Zn2+-to-SG ratio or R[Zn2+]/[-SG]. If no Zn2+ ions were added to the Au NC solution [or R[Zn2+]/[-SG] = 0], the Au NCs were well-dispersed in water and remained separated, as shown in the TEM image (Figure 1a). The discrete nature of the Au NCs was also supported by DLS measurements, where a hydrodynamic diameter (HD) of ~2.7 nm was calculated (Figure 1e, black line). When R[Zn2+]/[-SG] was increased to 0.3, some small and irregularly-shaped NC assemblies began to appear in the TEM image (Figure 1b). The slight increase in HD in the DLS measurements (Figure 1e, red line) is consistent with the formation of small NC assemblies. The small amount of counter cations introduced to the NC solution at a low R[Zn2+]/[-SG] value (0.3) could only induce controlled aggregation of the negatively-charged NCs to a limited extent; and only NC assemblies smaller than 10 nm were formed (Figure 1b). The small size of the NC assemblies was also corroborated by UV-vis spectroscopy (Supplementary Fig. S2) where scattering intensity increase (indication of a significant particle size increase)8 was not found relative to the discrete Au NCs.

Fractal-like spheres displaying limited self-similarity52 (spherical nanoion to spherical colloidal assembly at the scale of ~1 and 100 nm, respectively) were present in the TEM image when R[Zn2+]/[-SG] was increased to 0.6 (Figure 1c). The spherical assemblies had a uniform core size of 136.2 nm (100 colloidal spheres counted) and a HD of ~137.6 nm (Figure 1e, blue line). The assembled structure at a higher R[Zn2+]/[-SG] value of 0.9 was visually similar (Figure 1d). The diameter of the NC assemblies was however smaller, at ~92.8 nm (100 colloidal spheres counted) and likewise the measured HD decreased to ~93.5 nm (Figure 1e, green line). An increase in the scattering intensity of the NC assemblies was noted when R[Zn2+]/[-SG] was increased from 0.6 to 0.9 (Supplementary Fig. S2). This is an indication of the increase in the number of NC assemblies at R[Zn2+]/[-SG] of 0.9. Hence at the higher R[Zn2+]/[-SG] value of 0.9, there were more NC assemblies formed but the size was smaller (vs R[Zn2+]/[-SG] = 0.6). This finding can be understood based on the common nucleation-growth mechanism53. At a higher R[Zn2+]/[-SG] (0.9), more Zn2+ ions were available as electrostatic cross-linkers, leading to a faster formation of “assembly nuclei”. More “nucleation sites” were available for growth through continuous assembly of NCs. Consequently smaller NC assemblies were formed when the same NC concentration was used. The dependence of the NC assembly size on the concentration of the counter cations (Zn2+) is summarized in the inset of Figure 1e, where the maximum in the size of the NC assemblies was found to be around ~137.6 nm.

The structure and composition of fractal-like NC assemblies assimilated by Zn2+ were also examined by high-resolution TEM (HR-TEM). The HR-TEM images of assemblies formed at R[Zn2+]/[-SG] of 0.6 and 0.9 are shown as insets in Figure 1c and 1d respectively, where NCs smaller than 2 nm are clearly visible within the assembly. UV-vis spectroscopy also provided supporting evidence for the assimilation of primary NCs (Supplementary Fig. S2). The characteristic absorption peak of isolated (primary) Au NCs at ~400 nm was mostly retained in the UV-vis spectra of the NC assemblies. The surface plasmon resonance (SPR) of large spherical Au NPs, which absorbs at ~520 nm (for ~50 nm Au NPs)54 was conspicuously absent, suggesting that the size and structure of the Au NC building blocks were preserved in the assemblies. No increase in the size of the NC building blocks was detected in the assemblies, confirming that the ion-induced NC assembly is a soft approach. The relatively weak electrostatic interaction between the NCs and the counter ions was unable to alter the size and structure of the NC building blocks. The chemical composition of the NC assemblies was analyzed by energy dispersion X-ray spectroscopy (EDX). Line scan analysis across the diameter of a representative assembly (Figure 2a) and the elemental maps of the latter confirm the uniform distribution of Au (Figure 2b) and Zn (Figure 2c) throughout the colloidal sphere, suggesting that the spherical assembly was formed by the assimilation of Au NCs by Zn2+ ions.

Figure 2
figure 2

(a) Scanning transmission electron microscopy (STEM) image of a representative Au NC colloidal sphere assembled at R[Zn2+]/[-SG] = 0.6; (b–c) EDX elemental maps of the circular region in (a) in terms of Au (b) and Zn (c); the insets in (b) and (c) show respectively the Au and Zn signals in the EDX line scan across the yellow line in (a).

Ion-like behavior of Au NCs

The assembly of Au NCs exhibited an intriguing ion-like behavior, where a step-wise dependence on the concentration of counter cations (Zn2+) was observed, as shown in the insets of Figure 1e and Supplementary Fig. S2. The negatively-charged NCs were initially inert to the addition of a small amount of Zn2+ up to a threshold value of R[Zn2+]/[-SG] (~0.3). Increase in the R[Zn2+]/[-SG] value beyond this threshold value (e.g., 0.3 < R[Zn2+]/[-SG] < 0.6) triggered the formation of spherical NC assemblies, similar to the formation of precipitates beyond the solubility limit defined by the solubility product Ksp. In precipitation, taking A+ + B = AB↓ as an example, the ionic product Q = [A+][B] is always a constant (Ksp) in a solution saturated with the precipitate AB. Similarly, a constant Q value ( = [COO]2[Zn2+] considering the formation of –COO···Zn2+···OOC– ion pairs) was also observed in the “saturated solutions” of negatively-charged NCs and counter cations (Zn2+). The Q values (determined by ICP-MS) obtained in R[Zn2+]/[-SG] of 0.6 and 0.9 were 3.31 × 10−11 and 3.35 × 10−11 M3 respectively. The Ksp was therefore estimated to be 3.33 × 10−11 M3. The high ligand-to-metal ratio (the SG-to-Au ratio is ~0.84) and the uniform size and structure of the Au NCs are key contributions to their ion-like properties (step-like assembly). The possession of ion-like structural features in the Au NCs not only made it possible for the step-like assembly, but also produced an ordered structure mimicking the formation of ionic crystalline compounds. In nature oppositely charged ions are often packaged into crystalline ionic compounds with long-range order. Similarly, the NC assemblies here adopted a fractal-like spherical geometry (Figure 1c and 1d). It should be reiterated that such fractal-like assembly was different from the counter-ion-induced assembly of large NPs (>3 nm) where the aggregates display only a low symmetry55,56. However, it should be noted that the spherical NC assemblies did not exhibit long-range crystalline order. This could be attributed to the relatively large difference in size between the negatively-charged NCs and the counter cations (Zn2+).

The counter cations Zn2+ exerted their influence on the assembly of negatively-charged Au NCs through principally two effects. The first was the screening effect where Zn2+ reduced the negative charge on the Au NC surface through the formation of intra-cluster –COO···Zn2+···OOC– electrostatic linkage (referred to henceforth as intra-EL). The second was the bridging effect forming inter-cluster –COO···Zn2+···OOC– electrostatic linkages (inter-ELs). The bridging effect brought two separate NCs together while intra-EL did not bring about NC assembly per se. These two effects are illustrated schematically in Figure 3. At low R[Zn2+]/[-SG] (~0.3), the amount of Zn2+ in the NC solution was small and Zn2+ tended to bind to carboxylate anions on the same NC, thus leading to the formation of intra-ELs. This was the phase I stage in the assembly of NCs. Charge screening effect was dominant in this stage, as evidenced by the rapid increase in the ζ-potential of the NCs with the increase in the Zn2+ concentration (R[Zn2+]/[-SG] from 0 to 0.3, Supplementary Fig. S3). The formation of intra-ELs gradually approached saturation with the continuing increase in Zn2+ concentration. At the threshold value of R[Zn2+]/[-SG] (determined to be ~0.3 in this study), inter-ELs began to form resulting in the formation of small and irregularly-shaped NC assemblies due to partial bridging effect (Figure 1b). Further increase in the Zn2+ concentration increased the extent of inter-ELs (ionic cross-linking) until the step-like assembly of the Au NCs occurred, the inception of which is identified as phase II in Figure 3. For example, at R[Zn2+]/[-SG] = 0.6, the Au NCs were extensively assimilated into colloidal spheres (Figure 1c). However, the ζ-potential of the NCs (Supplementary Fig. S3) was nearly unchanged when R[Zn2+]/[-SG] was increased from 0.3 to 0.6. This observation suggests that in the concentration range of 0.3 < R[Zn2+]/[-SG] < 0.6, the charge screening of Zn2+ was nearly constant and the bridging effect of Zn2+ was more important than the screening effect. A further increase in the Zn2+ concentration from R[Zn2+]/[-SG] = 0.6 to 0.9 led to the gradual depletion of Au NCs in the solution and the completion of the NC assembly process. The gradual depletion of NCs was accompanied by the accumulation of excess Zn2+ through adsorption on the surface of NC assemblies, which resulted in a second series of ζ-potential increase of the NC solution (Supplementary Fig. S3).

Figure 3
figure 3

Proposed mechanism for Zn2+-induced assembly of Au NCs.

Several independent measurements also suggest the bridging effect of divalent Zn2+ ions as the primary factor in the assembly of Au NCs. First, common monovalent cations such as Na+ ions (from dissolved NaCl), which could also screen the surface charge of Au NCs, were unable to cause a similar assembly of the Au NCs. Au NCs remained separate in 0.6 mM NaCl solution (same ionic strength as the 0.2 mM ZnCl2 used to provide R[Zn2+]/[-SG] = 0.6, please refer to the Methods section for the details of the ionic strength calculation). The HD measurement in Figure 4 (second column) indicated likewise. A further increase in the ionic strength of the NaCl solution (e.g., by increasing the NaCl concentration to 0.5 M) also did not help to bring about the assembly of Au NCs (Figure 4, third column). Hence the screening effect of cations on the surface charge of the NCs is not critical to the assembly of NCs. The increase in the solution ionic strength could however disrupt the electrostatic interaction between Zn2+ and carboxylate anions. The presence of NaCl in large excess in the Au NC solution (~0.5 M in the final reaction mixture) prior to ZnCl2 addition could suppress the assembly to a great extent. The HD of the NCs in the presence of both Na+ and Zn2+ was also the same as that of discrete NCs, thereby suggesting no significant assembly of the Au NCs (Figure 4, fifth column).

Figure 4
figure 4

Measured hydrodynamic diameters of assembled/disassembled Au NCs at different pH and in the presence of different ions.

The assembly with Zn2+ was carried out at R[Zn2+]/[-SG] = 0.6.

Excess H+ had the same effect as Na+ in disrupting the assembly of NCs by Zn2+. For example, by adjusting the pH of the NC solution to ~2.7 (a value lower than the isoelectric point of Au NCs, Supplementary Fig. S1), the assembly of Au NCs was significantly inhibited, as shown by the nearly invariant HD of the NCs in the presence and absence of Zn2+ at pH ~2.7 (Figure 4, the last two columns). More interestingly, the assembly and disassembly of the Au NCs could be reversed by cycling the pH of the solution between 6.5 and 2.7. The zigzag changes in the HD of the Au NCs under pH cycling (Figure 5a) indicate that the Au NCs could undergo repeated assembly and disassembly at pH 6.5 and 2.7 respectively.

Figure 5
figure 5

Effects of pH cycling on the hydrodynamic diameters (a) and photoemission spectra (b, excited at 365 nm) of Au NCs assembled by Zn2+.

The Au NCs were initially assembled at pH ~6.5 (#1) and then pH was varied in the sequence of ~2.7 (#5) -- 6.5 (#2) -- 2.7 (#6) -- 6.5 (#3) -- 2.7 (#7) -- 6.5 (#4). In a separate experiment, solution #7 was dialyzed overnight followed by reassembly with Zn2+ at pH 6.5. The hydrodynamic diameter of the reassembled “refreshed” Au NCs was recorded as the red dot in (a). The inset in (b) shows the expanded view of the circled area. All assemblies were carried out at R[Zn2+]/[-SG] = 0.6.

There was irreversibility shown, however, as the HD of the Au NCs at pH 6.5 gradually decreased with the increase in the cycle number. This trend could be attributed to the slow accumulation of ionic strength due to the way pH cycling was implemented: The pH of the solution was adjusted by the addition of a given amount of 0.1 M HCl or 0.1 M NaOH, leading to the gradual buildup of ionic strength with the increase in the cycle number. A higher ionic strength of the solution increased the screening effect on the electrostatic interactions between Zn2+ and negatively-charged NCs, thus leading to a smaller degree of assembly (decreasing size of the NC assemblies). The ionic-strength-induced irreversibility could be eliminated by removing the excess small ions. We “refreshed” the Au NC solution at the lower pH of cycle 3 (corresponding to point 7 in Figure 5a) by dialysis, where a semipermeable membrane with a molecular weight cut off (MWCO) of 3500 Da was used to filter away the small ions (e.g., H+, Na+, Zn2+ and Cl). After pH adjustment to 6.5 and Zn2+ addition, a HD of 124.4 nm (the red dot in Figure 5a) could be obtained from the “refreshed” Au NC solution, similar to the HD assembled at pH = 6.5 in cycle 1 from a fresh Au NC solution (137.6 nm, point 1 in Figure 5a). This observation led us to conclude that the reversibility of assembly and disassembly could be greatly improved through the control of the ionic strength.

Assembly induced photoluminescent enhancement

The physical and chemical properties of the Au NCs could be altered by proximity effects in an ionically cross-linked close-packed structure. One most interesting property of the Au NCs is their strong optical luminescence, as shown in Figure 6 (black line). The as-synthesized Au NCs had a unique Au(0)@Au(I)-thiolate core-shell structure, where the intra-cluster aurophilic interaction [Au(I)-Au(I)] contributed to the PL of the NCs8,57,58. The distance between the Au NCs could be significantly shortened after assembly to promote inter-cluster aurophilic interaction. The increase in inter-cluster aurophilic interaction could increase the PL of the NCs. The assembly of Au NCs could also reduce non-irradiative relaxation of excited electrons, which also enhances the PL of the NCs59,60. For example, the bridging Zn2+ between neighboring carboxylate anions (via either an intra- or inter-EL) could inhibit the vibration or rotation of the thiolate ligands, which is one of the non-irradiative relaxation pathways8. Experimentally the PL (at 610 nm) of the NC assemblies (Figure 6) was significantly higher than that of discrete Au NCs. In order to rule out the possibility of PL enhancement through the formation of Zn2+-thiolate (-SG) complexes, a control experiment was carried out by mixing Zn2+ and GSH in water. The resultant Zn-SG complexes did not exhibit any luminescence (data not shown). Two other experimental observations also provided supporting evidence on proximity-induced properties in the NC assemblies. First, as shown in the inset of Figure 6b, the PL enhancement effect also displayed a similar step-like trend with the increase of the Zn2+ concentration, which corresponds well with the step-like assembly of the Au NCs. Second, the PL enhancement could also be turned on or off corresponding to the assembly or disassembly of Au NCs in pH cycling (Figure 5b).

Figure 6
figure 6

(a) Digital photos of Au NCs assembled at various R[Zn2+]/[-SG] values: 0 (#1 and #5), 0.3 (#2 and #6), 0.6 (#3 and #7) and 0.9 (#4 and #8); #1 ~ 4 were taken under normal light while #5 ~ 8 were taken under UV illumination (365 nm); (b) Photoemission spectra (exited at 365 nm) of Au NCs assembled under different R[Zn2+]/[-SG] values: 0 (black), 0.3 (red), 0.6 (blue) and 0.9 (purple); the inset shows the emission intensity maximum as a function of R[Zn2+]/[-SG].

Discussion

The ion-induced assembly of NCs developed in this study is expected to be generic and hence should be applicable to other charged metal NCs and divalent counter ions. For example, other divalent cations, such as Cd2+, may be used to substitute for Zn2+. Similar spherical NC assemblies were indeed obtained by using Cd2+ as the counter cations (Supplementary Fig. S4). Similarly, the PL intensity of the NCs assimilated by Cd2+ was also significantly higher than that of discrete Au NCs (Supplementary Fig. S4). The ion-induced assembly of NCs could also be extended to other nanoions; e.g., red-emitting Ag NCs protected by GSH. As shown in Supplementary Fig. S5, the addition of Zn2+ to the Ag NC solution also induced the assembly of Ag NCs, leading to the formation of spherical NC assemblies. Enhanced PL was also detected for the Ag NC assemblies (Supplementary Fig. S5).

In summary, we have developed a facile and general method to assemble charged noble metal NCs in water based on the electrostatic interaction between oppositely-charged entities. Negatively-charged Au NCs were assembled into monodisperse and fractal-like spherical assemblies by divalent counter cations such as Zn2+ and Cd2+, via the formation of inter-cluster electrostatic linkages (inter-EL) of the type –COO···M2+···OOC–. Owing to their high charge density, ultrasmall size and structural uniformity, the Au NCs may be regarded as an ion-mimic nanomaterial, exhibiting ion-like properties of step-like assembly dictated by Ksp and a high structural order in the assembly. The bridging effect of the divalent cations is essential to the formation of NC assemblies. A strong synergy between the NCs due to the close-packed order in the assembly resulting in the PL enhancement of NCs was also demonstrated in this study. The NC assemblies and the assembly methods in this study are of interest not only because they provide a simple and general method to generate a superstructure of functional noble metal NCs, which is of interest to both basic and applied research; but also because they exemplify a NC surface with charged hydrophilic ligands as three-dimensional nanoions, with the potential to mimic some of the useful behavior of real ions in various practical settings.

Methods

Materials

Hydrogen tetrachloroaurate(III) trihydrate (HAuCl4·3H2O), L-glutathione reduced form (GSH) and sodium borohydride (NaBH4) from Sigma Aldrich; hydrochloric acid (HCl) from J. T. Baker; zinc chloride (ZnCl2), silver nitrate (AgNO3) and sodium hydroxide (NaOH) from Merck; and cadmium chloride (CdCl2) from Strem were used as received without further purification. Ultrapure Milipore water (18.2 MΩ) was used in the preparation of all aqueous solutions. All glassware was washed with aqua regia and rinsed with ethanol and ultrapure water before use.

Synthesis of orange-emitting Au NCs

A more detailed description of the synthesis method can be found in the original work8. Briefly, 0.5 mL of 20 mM HAuCl4 and 0.20 mL of 100 mM GSH aqueous solutions were mixed with 4.35 mL of ultrapure water at room temperature (25°C). After incubation under gentle stirring (500 rpm) at 70°C for 24 h, bright orange-emitting Au NCs were formed.

Synthesis of red-emitting Ag NCs

Red-emitting Ag NCs were prepared by a cyclic reduction-decomposition method detailed elsewhere10. Briefly, 125 μL of 20 mM AgNO3 and 150 μL of 50 mM GSH aqueous solutions were added to 4.85 mL of ultrapure water under vigorous stirring (~1200 rpm) to form Ag(I)-thiolate complexes. 50 μL of 112 mM NaBH4 aqueous solution was then introduced to reduce the Ag(I)-thiolate complexes, giving rise to a deep-red solution of Ag NCs within 5 min. The As-formed Ag NC solution (deep-red) was allowed to decompose to Ag(I)-thiolate complexes (colorless) after ~3 h of incubation at room temperature (25°C). 50 μL of 112 mM NaBH4 aqueous solution was then added to this colorless solution under vigorous stirring (~1200 rpm). The color of solution turned from colorless to light-brown within 15 min. This light-brown Ag NC solution was allowed to stand (without stirring) at room temperature (25°C) for 8 h to form red-emitting Ag NCs in aqueous solution.

Ion-induced assembly of orange-emitting Au NCs

ZnCl2 and CdCl2 aqueous solutions in specific concentrations were freshly prepared by dissolving calculated amounts of ZnCl2 and CdCl2 in ultrapure water respectively. The pH of each metal salt solution was adjusted to ~6.5 by adding 0.1 M NaOH. The As-prepared Au NC aqueous solution was diluted 4 times (4× diluted) and the pH was adjusted to ~6.5 before use. In a typical assembly (taking R[Zn2+]/[-SG] = 0.6 as an example), 0.25 mL of 1 mM ZnCl2 was quickly added to 1 mL of the diluted Au NC solution, followed by mixing on a vortex mixer (1500 rpm for 30 s). The pH of the mixture was maintained at ~6.5. Subsequently, the mixture was kept still at room temperature (25°C) for 15 min to allow the assembly to complete. Assembly of Au NCs by Zn2+ in other concentrations and by Cd2+ solution were also carried out likewise, using different metal salt solutions before mixing.

Ion-induced assembly of red-emitting Ag NCs

The pH of Ag NC as well as 2 mM ZnCl2 aqueous solution was brought to ~6.5 before use. Similar to the Zn2+ induced assembly of Au NCs, 1 mL of Ag NC and 0.25 mL of 2 mM ZnCl2 aqueous solutions were mixed while pH was maintained at ~6.5, followed by still incubation at room temperature (25°C) for 15 min.

Dialysis of NC solution

5 mL of NC solution was sealed in a dialysis bag made of a semipermeable membrane (MWCO = 3500 Da, Spectra/Por®), followed by immersion into 5 L of ultrapure water. The dialysis process lasted overnight under moderate stirring (1000 rpm).

Estimation of the ionic strength of ZnCl2 and NaCl in the solutions

The ionic strength of NaCl or ZnCl2 solution was calculated by the equation, I = 0.5 ∑ cizi2, where I is the ionic strength, ci is the concentration of a specific ion and zi is the specific charge number of the ion.

Characterization

pH was monitored by a Mettler Toledo FE 20 pH-meter. UV-vis absorption and photoluminescence (PL) spectra were recorded by a Shimadzu UV-1800 spectrometer and a PerkinElmer LS-55 fluorescence spectrometer respectively. Transmission electron microscopy (TEM), scanning transmission electron microscopy (STEM) and Energy-dispersive X-ray spectroscopy (EDX) elemental analysis were performed on a JEOL JEM 2010 microscope operating at 200 kV. The size and ζ-potential of NCs before and after assembly were measured by dynamic light scattering (DLS) and electrophoresis light scattering (ELS) on a Malvern Zetasizer Nano ZS, respectively. The samples were centrifuged by an Eppendorf Centrifuge 5424. The Au and Zn contents in the samples were analyzed by inductively coupled plasma mass spectrometry (ICP-MS) measurement on an Agilent 7500A. The GSH and carboxyl group contents were calculated based on the Au content via the relation Au:GSH:COOH = 1:0.84:1.688.