Open Access Article
Lorenzo Branzi
*,
Sean Freeman,
Lucy Fitzimmons
,
Conor Burke
and
Yurii K. Gun’ko
*
School of Chemistry, Trinity College Dublin, Dublin, Ireland. E-mail: branzil@tcd.ie; igounko@tcd.ie
First published on 13th April 2026
The production of a range of multinary quantum dots (QDs), including both ternary phase silver indium sulfide (AIS) and copper indium sulfide (CIS), and their quaternary alloys with zinc sulfide (ZAIS and ZCIS), using a L-menthol and lauric acid deep eutectic solvent (DES) was investigated. This novel synthetic approach relies on the hydrophobic nature of the L-menthol–lauric acid DES to combine the typical reaction environment of hot-injection processes, commonly used for the production of high-quality QDs, with the highly desirable qualities of deep eutectics as green solvents. The deposition of a zinc sulfide shell was also investigated, achieving an improvement of the photoluminescence quantum yield up to 65%. Moreover, the incorporation of multinary QDs produced in the L-menthol–lauric acid DES into polymethyl methacrylate (PMMA) matrices was investigated, yielding both bulk slabs and colour-converting layers for white and monochromatic LEDs. These studies clearly demonstrate the feasibility and advantages of DES-based synthesis for the production of high-quality multinary QDs and their incorporation into luminescent polymeric composites with strong potential for photonic and energy applications.
I–III–VI ternary quantum dots and their quaternary zinc alloyed I–II–III–VI phases are a promising class of nanomaterials with visible to near infrared emission. Due to their unique optical properties and composition-dependent tunability, multinary QDs are rapidly becoming popular low-toxicity alternatives to binary II–VI QDs.10 For these reasons, multinary QDs have been widely investigated in photonics,10 energy11 and biomedical applications12 as well as recent studies have reported efficient hot-electron photocatalysis13 and tunable chirality.14,15 In particular, the intrinsic broad photoluminescence and large Stokes shift characteristics of the photoluminescence of multinary QDs make them promising candidates for applications as luminescent active materials in luminescent solar concentrators (LSCs)16,17 and as downconverter phosphors in colour conversion layers used for white light-emitting diodes (LEDs).10,18 Despite their promising optical properties and the wide range of technologically relevant applications, synthetic strategies for the production of multinary QDs in DESs have not been reported to date.
In this work, we developed a new robust synthetic procedure using a L-menthol–lauric acid DES for the production of a broad family of luminescent multinary QDs. Our investigation covers ternary I–III–VI compounds such as silver indium sulfide (AIS), copper indium sulfide (CIS) and their quaternary I–II–III–VI phases, including silver indium zinc sulfide (ZAIS) and copper indium zinc sulfide (ZCIS). Hydrophobic DESs represent a relatively novel class of green solvents after the first report in 201519 and are becoming rapidly popular, unlocking a wide range of novel applications,20 among which is their use as solvents for the synthesis of inorganic nanomaterials.21 The hydrophobic nature of the L-menthol–lauric acid DES mimics the reaction environment typical of hot-injection processes commonly used for the production of high-quality QDs. Moreover, L-menthol and lauric acid are inexpensive natural products characterised by high biocompatibility and natural abundance.22–24 In particular, L-menthol is produced via biosynthesis in plants of Mentha species and it is manufactured on a large scale (likely exceeding 700 metric tons per year) for application in industries like oral health care products, the food industry, cosmetics and pharma.22,23,25 On the other hand, lauric acid is the main component of coconut and palm oil, and vegetable oils and fatty acids are some of the most suitable resources for the development of sustainable processes.24 To further improve the optical properties of the multinary QDs produced using DES, a one-pot process for the deposition of a ZnS layer and the production of multinary core–shell QDs using the L-menthol–lauric acid DES has been successfully developed, achieving a substantial increase in the photoluminescence quantum yield to values as high as 65%. The hydrophobic nature of the multinary QDs produced via this strategy guarantees high compatibility with polymeric matrices like polymethyl methacrylate (PMMA) without any surface modification. Thus, the production of luminescent QD–PMMA bulk nanocomposites via in situ radical polymerisation, as well as the fabrication of colour converting layers for application in white and monochromatic LEDs, was investigated.
The mixture of L-menthol and lauric acid with a 2
:
1 molar ratio forms a DES which is liquid at room temperature (Fig. S11a and b) and mimics the hydrophobic environment of the high boiling point solvents conventionally used for QD synthesis via the hot-injection process.21,26,27 The use of metal laurate precursors for silver, indium, and zinc enables high solubility of all the different cationic components in the L-menthol–lauric acid DES, allowing for homogeneous solutions even at low temperatures. This was found to be particularly relevant, since a low injection temperature (40 °C) was identified as ideal for the production of QDs with superior optical properties (see later). The injection of the sulfur precursor solution into the metal cation solution in DES induces a rapid particle nucleation, and the nanocrystals’ growth can be promoted by further heating at a higher temperature. Fig. 1b shows the typical absorption and photoluminescence spectra of the AIS QD reaction mixture collected at different reaction times. The emission maximum shifts from 636 nm, observed for QDs collected immediately after injection, to around 732 nm after 60 minutes of growth at 120 °C, in agreement with the red-shift of the absorption profile along with an increase in PL intensity (Fig. S11c and d). The QDs’ photoluminescence is dramatically affected by the reaction conditions; in particular, injection at 40 °C and a successive heating at 120 °C have been identified as ideal conditions for the synthesis of AIS QDs. Using a higher temperature for the injection step produces QDs with lower PL intensity and a broader emission profile (Fig. S11e), suggesting a poor homogeneity in the QD sample produced at higher temperatures.
TEM images of AIS QDs reveal the presence of nanocrystals with an average size of approximately 2.8 ± 0.9 nm (Fig. 1c and Fig. S12a), while after the deposition of the ZnS shell layer, an increase in the nanocrystal size to 3.5 ± 1.2 nm (Fig. 1d and Fig. S12b) was observed. HR-TEM images reveal diffraction fringes with a spacing of 0.32 nm, corresponding to the (112) planes of the chalcopyrite lattice (I-42d). Changing the composition of the cation mixture enabled the production of different multinary QDs; in this way, ternary AIS and CIS, as well as their quaternary counterparts with zinc sulfide, ZAIS and ZCIS, QDs were produced using L-menthol–lauric acid DES. The UV/vis absorption of the different multinary QDs is shown in Fig. 1e, and the optical band-gaps were estimated using the Tauc plot method (Fig. 1f), giving band gap values of around 2.14 eV, 2.16 eV, 2.43 eV and 2.58 eV for CIS, ZCIS, AIS and ZAIS QDs, respectively. The increase of the optical band-gap with the incorporation of zinc in the QD cores is consistent with the formation of AgInS2 and CuInS2 alloys with ZnS, forming the respective quaternary systems (Fig. S13).28
The PL properties of the multinary QDs produced in L-menthol–lauric acid DES reflect the variations in their chemical composition. PL and PLE spectra of multinary QD cores are shown in Fig. 2ai. Emission at 658 and 595 nm was observed for AIS and ZAIS QDs, while CIS and ZCIS showed emission at 705 and 690 nm, respectively. All systems displayed a broad excitation range that corresponds to the band-gap of the different nanocrystal compositions, as well as the typical emission profile of multinary QDs, characterised by large Stokes shifts and broad emission peaks; these features are associated with the presence of intragap states involved in the radiative recombination mechanism.29–33 Further details on the optical properties of multinary QDs produced in the L-menthol–lauric acid DES are presented in Table S1. The deposition of the ZnS shell using the L-menthol–lauric acid DES-based approach improves the PLQY (Table S1) for all the multinary QDs. In particular, the PLQY of ZAIS QDs increased from 18% to 65% with the deposition of the ZnS shell (Fig. S14). This enhancement is attributed to the passivation of surface defects such as dangling bonds with a layer of a larger bandgap semiconductor, suppressing non-radiative recombination pathways.34 Moreover, the ZnS shell deposition causes a further blue shift of the emission profiles, as shown in Fig. 2aii, which can be associated with a partial diffusion of Zn2+ ions in the QD core.35 The incorporation of Zn2+ into the QD core via the direct synthesis of quaternary I–II–III–VI systems or via diffusion is expected to mitigate the effect of cationic disorder and further improve optical properties.36 The effect of the ZnS shell deposition on the exciton recombination mechanism was further supported by the analysis of the PL lifetime observed at the PL maximum. All the I–III–VI multinary QDs produced showed photoluminescence decays on the order of 100–500 ns (Fig. S15), and these are typical values for I–III–VI QDs where the exciton recombination mechanism is mediated by intragap donor–acceptor states. An increase of the average lifetime of around 90 ns was observed for ZAIS, CIS and ZCIS QDs after the passivation process with ZnS (Table S2), supporting the suppression of non-radiative recombination processes with the deposition of an inorganic shell. In contrast, AIS QDs did not show any appreciable variation in the PL lifetime; however, this system is characterised by the longer decay time (〈τ〉 of around 480 ns) and variation in the average lifetime may not as evident as that of the other multinary QDs discussed here. Moreover, the observed lifetime of multinary QDs is wavelength dependent due to the complex mechanism involved in the exciton recombination and this could further complicate this analysis.37 The effect of the ZnS shell deposition on QDs’ optical properties was demonstrated in the photoluminescence thermal stability. The PL of ZAIS QDs decreases to 58% when the nanocrystals are heated at 60 °C (Fig. S16a and c), while 85% of the PL is preserved for the ZAIS/ZnS QDs (Fig. S16b and c). This observation further supports the critical role of the ZnS shell deposition in device applications such as LEDs.
XRD analysis revealed diffraction patterns that correspond to the tetragonal chalcopyrite phase, I
2d space group (Fig. 2bi) for all multinary core QD systems, in agreement with the TEM observations. The effect of Zn incorporation on the quaternary QDs is highlighted by the shift of all the peaks to slightly larger angles due to the smaller ionic radius of Zn2+ compared to that of In3+.38 In particular, the (112) peak is located at 27.2° for AIS QDs and 27.9° for ZAIS QDs. Similarly, the (204) and (312) peaks are shifted from 46.1° to 46.8° and from 53.0° to 53.9° (Fig. S17a and c), respectively. This evidence suggests a contraction of the d-spacing from 3.28, 1.97 and 1.73 Å observed for AIS QDs to 3.20, 1.94 and 1.70 Å in the case of ZAIS QDs. After the deposition of the ZnS layer, the diffraction patterns are dominated by the contribution of the sphalerite ZnS phase, space group F
3m (Fig. 2bii and Fig. S17b), as supported by Rietveld refinement (Fig. S18). The shelling step introduced an additional shift of all the diffraction peaks toward larger angles in comparison with the pattern of the core QDs (Fig. S19),34,39 along with a reduction of the peak broadening that can be associated with an increase in the crystalline size. Scherrer analysis of the broadening of the (112) peak gave crystalline sizes of 2.0 and 2.7 nm for ZAIS and ZAIS/ZnS QDs, respectively, further supporting the TEM evidence.
Energy dispersive X-ray spectroscopy (EDS) analysis of the multinary core QDs (Fig. 2ci) was performed to investigate the nanocrystals’ chemical composition. For the purpose of this work, we targeted the production of indium-rich QDs, since these systems are known for their superior optical properties associated with the formation of intrinsic defects.40,41 The EDS spectra of AIS QDs confirmed an Ag
:
In ratio of around 1
:
3.5, close to the composition used in the reaction mixture of 1
:
4. The quaternary ZAIS QDs showed a lower indium content with a ratio of 1
:
1
:
2.5 for Ag
:
Zn
:
In, respectively, suggesting that Zn2+ mostly replaced In3+ in the core QD structure (Fig. S20a). Similar observations were made for the copper-based QDs with the Cu
:
In ratio of 1
:
3.1 for the ternary CIS QDs, while a Cu
:
Zn
:
In ratio of 1
:
1.1
:
2.5 was observed for the quaternary ZCIS QDs (Fig. S20a). The deposition of ZnS significantly increased the zinc contribution for all the QDs (Fig. 2cii), and a ratio of around 1
:
2.8 was observed between the sum of the contributions from the monovalent and trivalent cations and Zn (Fig. S20b) for AIS/ZnS QDs and 1
:
2.6 for CIS/ZnS QDs.
To evaluate the potential applications of multinary QDs produced in the L-menthol–lauric acid DES, the production of luminescent multinary QD–PMMA nanocomposites was investigated. PMMA is an ideal candidate for the production of luminescent QD–polymer nanocomposites for application in photonics, due to its high optical transparency, stability and mechanical properties.42 For this purpose, multinary core–shell QDs were used, due to their superior optical properties, for the preparation of QD–PMMA bulk slabs via in situ radical polymerisation of methacrylic acid, as well as the production of QD–PMMA coating layers starting from PMMA solution in toluene.
For the production of multinary QD–PMMA bulk slabs, a two-step process was employed where the methyl methacrylate monomer was polymerised to a syrup in the first step, before the addition of the multinary QD solution and transfer into a sheet reactor mould to complete the polymerisation. Fig. 3 shows the optical characterisation of multinary QD–PMMA composite slabs (2.5 × 2.5 × 0.2 cm) produced using a QD loading of around 0.025 wt%. The QD–PMMA composites obtained by this procedure were highly transparent and homogeneous, preserving the optical properties of the multinary QDs used (Fig. 3a). The transmission spectra (Fig. 3b) show a maximum of transmittance of around 90% (at wavelengths higher than 700 nm), indicating a low degree of scattering caused by QD aggregation in the polymeric composite. The loss of around 10% in transmission is expected due to reflections from the two surfaces of the polymeric slab, while the absorption at shorter wavelengths reflects the chemical composition of the multinary QD used.43,44 More importantly, the photoluminescence properties of the multinary QDs (PL and PLE) are preserved in the PMMA nanocomposites (Fig. 3c), with emission maxima centred at 585 nm, 635 nm, 650 nm and 702 nm for ZAIS/ZnS, AIS/ZnS, ZCIS/ZnS and CIS/ZnS QDs, respectively. These types of composites are of great interest for potential application in LSC devices, where the large Stokes shift of multinary QDs ensures minimal energy losses due to reabsorption processes.16,17
The potential application of multinary QDs produced in L-menthol–lauric acid DES as colour converting phosphors for LEDs was investigated by preparing different QD–PMMA mixtures using a QD loading concentration of around 2.5 wt% on top of an LED chip to produce colour conversion layers with different optical properties. QDs have recently become a promising alternative to solid-state phosphors to produce white LEDs, especially multinary QDs, due to their intrinsic broad emission spectra.10,18 In particular, coating a 475 nm blue LED (forward voltage and current applied to the LED chip: 3.0 V and 80 to 140 mA, respectively) with ZAIS/ZnS (Fig. 4a) resulted in white light with CIE coordinates of X = 0.423 and Y = 0.3911 (Fig. 4c), a colour rendering index (CRI) of 77 and a correlated colour temperature (CCT) of 3100 K corresponding to warm white light. Similarly, AIS/ZnS QDs (Fig. 4b) produced warm white light with a larger contribution from the red spectral range, with CIE coordinates X = 0.503 and Y = 0.4038 (Fig. 4c), a CRI of 80, and a CCT of around 2100 K. Details on the effect of varying the current applied to the LED chip are shown in Fig. S21. A comparison with commercial white LEDs (Fig. S22) revealed that colour conversion layers produced using multinary QDs prepared in L-menthol–lauric acid DES have comparable CIE coordinates with commercial systems.
However, the colour rendering properties of multinary QD-based LEDs are still limited; commercial white LEDs showed a CRI of 97 and 92, mainly due to the stronger luminescence contribution in the green spectral range of their phosphor materials. The application of these QDs in the production of colour conversion layers for the production of monochromatic LEDs was investigated as well. In particular, yellow and red emissions were produced by coating a 400 nm LED chip with ZAIS/ZnS (Fig. 4d) and ZCIS/ZnS (Fig. 4e) QDs, respectively. The colour conversion layers produced light with CIE coordinates X = 0.564 and Y = 0.432 for ZAIS/ZnS QDs, while light with CIE coordinates X = 0.649 and Y = 0.343 was obtained using ZCIS/ZnS (Fig. 4f).
000 was purchased from Aldrich. The LED chips ILH-XO01-S390-SC211-WIR200 (400 nm LED), ILH-OW01-BLUE-SC211-WIR200 (475 nm), and ILH-OT01-HW90-SC221-WIR200-1 hot white (2700 K) and white (5000 K) were purchased from Intelligent LED Solutions ILS.
| ΦQD = ΦstFQDfstnQD2/FstfQDnst2 | (1) |
| fQD,st = 1 − 10−AQD,st. | (2) |
TEM images were collected using a JEOL 2100 microscope operating at 200 kV. EDS spectra were collected on a ZEISS Ultra Plus SEM equipped with a Bruker XFlash 7 7100 EDS detector with a 100 m2 window using a 15 kV electron beam. For each type of multinary QDs, EDS spectra were acquired over an area of 100 × 100 µm and the chemical composition was calculated as the average of three measurements. XRD patterns were collected using a Bruker D2 Phaser X-ray Powder Diffractometer working with the Cu Kα radiation source. FullProf software was used for the Rietveld refinement. LED colour converting layer characterisation was performed, powering the LED source at 100 mA and collecting the emission spectra using an integration sphere.
Supplementary information (SI): FTIR, UV-Vis, PL and NMR spectra, photoluminescence decay curves, XRD patterns, EDS analysis, additional TEM and HR-TEM images of QDs and luminescence spectra of LEDs. See DOI: https://doi.org/10.1039/d6tc00832a.
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