Jordi
Aguilera-Sigalat
a,
Simon
Rocton
a,
Juan F.
Sánchez-Royo
b,
Raquel E.
Galian
*ac and
Julia
Pérez-Prieto
*a
aMolecular Science Institute (ICMOL), University of Valencia, Catedrático José Beltrán 2, 46980 Paterna, Valencia, Spain. Fax: 34-963543576; Tel: 34-963543050E-mail: julia.perez@uv.es
bMaterials Science Institute, University of Valencia, Dr. Moliner 50, 46100 Burjassot, Valencia, Spain
cDepartment of Analytical Chemistry, ICMOL/Research Building, University of Valencia, Dr. Moliner 50, 46100 Burjassot, Valencia. Fax: 34-963543273; Tel: 34-963544307E-mail: raquel.galian@uv.es
First published on 22nd December 2011
Highly fluorescent organic- and water-soluble CdSe/ZnS core-shell quantum dots (QDs) with thiol ligands chemisorbed on the QD surface were synthesized by the replacement of amine ligands by alkyl thiols under very mild conditions. The QDs exhibited an even greater photostability than the initial core-shell amine capped QDs.
CdSe/ZnS nanoparticles are further passivated with organic ligands to allow them to remain stable as colloidal solutions in organic solvent and water. Organic-soluble QDs are required for optoelectronic applications, while water-soluble QDs are needed for biological applications. Trioctylphosphine (TOP) and trioctylphosphine oxide (TOPO), as well as fatty amines, are the most common ligands used in the synthesis of QDs.2,3
Theoretical calculations have shown that thiols cannot bind to the ZnS surface.4 By contrast, functional deprotonated thiols (thiolates) have been used as a capping material to make QDs water soluble and to add functionality to the nanoparticle. Thiolate ligands can replace TOPO and amine ligands and thus bind to the surface of CdSe/ZnS QDs more strongly, but such exchange produces QDs with drastically diminished fluorescence quantum yield (ΦF of more than 50% reduction).5 This has been explained as being due to a spontaneous binding of thiolates to the ZnS surface, causing a significant alteration of the surface.4 In addition, it has been reported that QDs capped with thiolates are vulnerable to photooxidation.6
Here we report that the chemisorption of thiols to CdSe/ZnS core-shell QDs helped by the amine ligands of the QDs can even improve their emission performance. This strategy was applied to the preparation of highly fluorescent organic-and water-soluble QDs that exhibited a higher photostability than the initial amine-capped QDs.
Model heterobifunctional ligands, 11-mercaptoundecanol (MU), 11-mercaptoundecanoic acid (MUA), 3-mercaptopropionic acid (MPA), and the ester of ketoprofen with MU (KP-SH)7 were used for these studies (Scheme 1). In addition, different sized CdSe/ZnS core-shell QDs capped with long-chain primary amines were used. These QDs were homemade or were purchased from different commercial sources (Table S1, ESI†).
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Scheme 1 Heterobifunctional ligands used in this work and schematic preparation of the organic- and water-soluble QDs. |
The synthesis of core-shell QDs (CdSe/ZnS) was done following M. G. Bawendi's procedure with some modifications.2 For a typical reaction, 5 g of TOPO was heated up to 190 °C in a three-neck flask for 2 h under Ar flow. Then, the solution was cooled to 60 °C and 0.5 mL of TOP was added into the flask. After that, 2 mL of CdSe QD was added and the reaction was heated to 140 °C. Then, the shell was added drop-wise for 10 min.
For the shell, 440 μL of ZnEt2, 65 μL of (TMS)2S, and 2600 μL of TOP were mixed in a glove box under N2 flow. Then, the reaction was cooled to 90 °C and kept at this temperature for 3 h. For the purification, the CdSe/ZnS QDs were precipitated in MeOH several times. Finally, QD-CS6 was redissolved in toluene.
A chloroform solution (25 mL) of QD-CS1 (5.46 × 10−7 mmol) and KP-SH (2.65 × 10−3 mmol, [thiol]/[QD] = 4859 molar ratio) was heated to reflux under nitrogen atmosphere for 48 h. After almost total solvent evaporation (2 mL) and the addition of methanol (30 mL), the samples were centrifuged at 8000 rpm for 20 min at 25 °C and the supernatant was decanted. The nanoparticles (CS1@KP) were dissolved in toluene (1 mL) and the purification process was repeated three times. The 1H-NMR spectrum of CS1@KP (Fig. 1B) showed a broadening of the ligand signals together with those of freely soluble ligands; the presence of a triplet at 3.3 ppm, ascribed to the CH2 attached to the N of protonated amine ligands (Fig. 1) was detected. It is well known that a ligand strongly bound to colloidal nanocrystals shows broad 1H-NMR signals, especially those of the protons close to the QD surface.9
The UV-visible spectrum of CS1@KP QDs exhibited the first exciton peak at the same position as the QD-CS1 QDs, i.e., QD functionalization did not produce any change in the first exciton peak (Fig. 2). High resolution transmission electron microscopy (HRTEM) images showed that CS1@KP maintained the size and the crystallinity of QD-CS1 (Fig. 3 and Fig. S1 in the ESI†). Interestingly, these QDs exhibited a higher ΦF (+ 50%) than the amine capped precursor (Fig. 4, Table S1, ESI†),10,11,12 demonstrating that the chemisorption of the thiol to the QD surface does not have a detrimental effect on the QD emission.
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Fig. 2 UV- visible absorption spectrum of QD-CS1 and CS1@KP in toluene. |
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Fig. 3 High Resolution Transmission Electron Microscopy images of CS1@KP, (2.3 ± 0.2 nm). |
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Fig. 4 Comparative fluorescence spectrum of A: a deaerated toluene solution of QD-CS1 (■) and CS1@KP (•). |
Similar results were observed when reacting QD-CS2 (48.1 × 10−9 moles) with KP-SH (2.4 × 10−4 moles) to produce CS2@KP (Fig. S2, ESI,†ΦF increase of 16.5%) and when using MU as a capping ligand (Fig. S3, ESI,†). The increase of the ΦF was higher for the smaller QDs, which is probably associated with a higher surface ligand-to-QD size ratio in the case of smaller-sized nanoparticles.
The same strategy was applied for the preparation of QD-CS nanoparticles decorated with carboxy groups. Thus, a chloroform solution of QD-CS3 (1.4 × 10−7 moles) was heated under reflux in the presence of MUA and MPA (7.0 × 10−4 moles) for 48 h. After the above-mentioned work-up, the QDs were placed in water and their solubility was increased by addition of tetramethylammonium hydroxide (10:
1 v/vwater: salt solution 0.1M) and mild heating (40 °C) for several minutes, leading to stable colloids of CS3@MUA and CS3@MPA. The absorption spectrum of CS3@MUA showed a clear red-shifted exciton peak (7 nm shift), while such variation was only of 2 nm for CS3@MPA. The solvatochromic effect is expected to induce a redshift as the solvent dielectric constant (ε) increases from 4.8 (chloroform) to 78 (water).13 The HRTEM images showed an average size of 3.1 ± 0.3 nm and 3.3 ± 0.3 nm for QD-CS3 and CS3@MPA QDs, respectively, (Fig. S4, ESI†). The emission bandwidth of the new water-soluble QDs was narrower than that of their precursor (Table S1). In addition, the Stokes shift of the thiol capped QDs was greater than that of the amine capped QDs.
Interestingly, the water soluble QDs exhibited a ΦF of 54% (CS3@MUA, Fig. 5) and 45% (CS3@MPA, Fig. S5, ESI,†); i.e. ligand exchange and water solubilization led to a decrease in the ΦF of less than 29% (Table S1).
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Fig. 5 Comparative fluorescence spectra of a deaerated toluene solution of QD-CS3 (■) and a water solution of CS3@MUA(•). |
These results indicated that the replacement of the amine ligands by thiols under the described conditions resulted in well-passivated QDs. Lee et al.4 have reported that the replacement of TOPO ligands by MPA thiolates in considerably larger sized CdSe/ZnS QDs (5.2 nm, λmax at 610 nm) can give rise to QDs with a high photoluminescence performance if using an MPA thiolate soluble in chloroform and avoiding the presence of water. However, this only applied to small thiolate concentrations. In fact, high concentrations of thiolate were detrimental to ΦF and produced non-fluorescent QDs. We performed control experiments to determine the effect of the addition of such organic-soluble thiolates to QD-CS3 QDs, and found a drastic decrease of the QD fluorescence. Therefore, we reason that the exchange of the amine ligands by thiols in our studies could benefit from the basicity of the amines after their release from the QD surface, polarizing the thiol S–H bond14 and increasing the nucleophilicity of the thiol (Scheme 1). Consequently, chemisorption of the thiol to the core-shell QD surface would occur under very mild conditions.
To confirm the chemisorption of thiol to the core-shell QDs under the described mild conditions, the infrared spectra of KP-SH, CS2@KP, QD-CS2, and that of a freshly-prepared mixture of QD-CS2 and KP-SH were compared (Fig. S6, ESI,†). The stretching vibration mode of the thiol group of KP-SH at ca. = 2569 cm−1 was also present in the QD-CS/KP-SH mixture, but vanished in CS2@KP.
In addition, X-ray photoelectron spectroscopy (XPS) was used, since it provides the binding energy of a core-level electron of an atom in the solid.15 This energy depends on the potential energy at that position, which in turn depends on the chemical environment of the atom. Hence, an organic-soluble QD, CS2@KP, and a water-soluble QD, CS3@MUA, were analyzed by XPS and the data were compared with those for KP-SH, MUA, and a core-shell QD (QD-CS2), as well as those for a core-shell QD prepared by reacting QD-CS2 (48.1 × 10−9 moles) with KP-SH (2.4 × 10−4 moles) at room temperature, CS2@KPrt .
The Cd 3d spectrum splits by the spin-orbital coupling into the 3d 3/2 (404.7 eV) and 3d 5/2 (411.4 eV) components, with a typical splitting magnitude of 6.7 eV. The binding energy of the Cd was very similar for all the core-shell QDs, QD-CS2, CS2@KPrt , CS2@KP, and CS3@MUA (Fig. 6). Except for QD-CS2, deconvolution of the spectrum gave, besides the 3d 3/2 Cd contribution, a new component with a binding energy at ca. 403 eV. This was the main contribution for CS3@MUA, and it was ascribed to the presence of N1s of ammonium salts.16 In agreement with this, while the C 1s spectrum (not shown) of MUA exhibited a component at 288.8 eV that was attributed to the carboxylic moiety, CS3@MUA presented a peak at 287.8 eV, ascribed to the carboxylate group.17
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Fig. 6 XPS spectra of Cd 3d and N 1s for QD-CS2, CS2@KPrt, CS2@KP, and CS3@MUA. |
Regarding the S 2s spectrum, KP-SH presented a peak at 227.4 eV ascribed to the thiol group,17 while QD-CS2 exhibited a peak with binding energy of 225.7 eV, brought about by the ZnS shell (Fig. 7).18 This band was very similar in the case of CS2@KPrt, but shifted to a lower binding energy (225.3 eV) in the case of CS2@KP (Fig. 7). This can be explained by the contribution of the thiol ligand, chemisorbed on the QD shell. Therefore, this peak was deconvoluted into two separate peaks by using the S 2s spectrum of the initial amine-capped core-shell QD as the reference. The new component shifted considerably to a lower value than that of the unbound thiol (at 224.4 eV vs. 227.4 eV) and this may be attributed to the chemisorption of KP-SH to the QD surface;18 its high contribution (ca. 30%) showed a large coverage of the QD surface by KP-SH.
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Fig. 7 Top to bottom: XPS spectra of S 2s for QD-CS2, CS2@KPrt, CS2@KP, and KP-SH. |
The generality of the methodology to prepare highly fluorescent thiol-capped CdSe/ZnS core-shell QDs to QDs different from those manufactured by Evident was also studied, using homemade QDs as well as QDs purchased from another supplier, specifically from Ocean Nano Tech (QD-CS4: λmax at 503 nm, ΦF of 58% and QD-CS5: λmax at 544 nm, ΦF of 55%), see Table S1, ESI.†
Thus, a homemade TOPO-capped CdSe/ZnS core-shell QD (QD-CS6, 2.8 nm, λmax at 535 nm) was prepared following a previously reported procedure with some modifications (see experimental section). The TOPO ligands of QD-CS6 were replaced by amine ligands by heating a deaerated chloroform solution (25 mL) of QD-CS6 5.46 × 10−7 mmol and octadecylamine (ODA) ([amine]/[QD] = 4859 molar ratio) under reflux for 48 h. The amine-capped QDs (QD-CS7) exhibited its first exciton peak at 535 nm and a ΦF of 31%. The replacement of the capping ligands on QD-CS6 and QD-CS7 by KP-SH was carried out using the above-mentioned strategy to lead to CS6@KP (ΦF of 35%) and CS7@KP (ΦF of 30%), respectively. The S 2s spectrum of CS7@KP (not shown) presented a peak at 224.4 eV ascribed to the chemisorption of KP-SH to the QD, while neither CS6@KP, nor QD-CS6, nor QD-CS7 exhibited a peak with this binding energy. As expected, CS6@KP presented a peak at 227.4 eV ascribed to the thiol group.
In addition, the replacement of the capping ligands on QD-CS5 was performed with the thiol and thiolate form of KP-SH, leading to CS5@KP1 and CS5@KP2, respectively. The 1H-NMR spectrum of both QDs showed the characteristic broadening of the ligand signals. But, while the replacement of the QD capping ligand with the thiol led to a decrease in the ΦF of only 8%, the thiolate produced a drastic decrease (39%) of the QD emission. For further details of these and additional experiments regarding the effect on the emission properties of QD-CS4, QD-CS5, QD-CS6, and QD-CS7 after adding thiols, see Table S2 in ESI.†
The photostability of nanoparticles is of great importance in their applications; therefore, the photostability of several of the prepared thiol capped QDs was compared with that of their amine capped precursor. The samples were irradiated (400 nm < λ < 700 nm, λmax at 420 nm, 70 W/m2) in toluene or water, depending on the solubility of the corresponding QD, under nitrogen or air atmosphere for ca. five hours.
Surprisingly, the emission maximum of the QDs experienced only a small blue-shift (up to 6 nm) after 5 h irradiation under air atmosphere (Table 1).19 Blue-shifts up to 40 nm have been reported for TOPO capped CdSe/ZnS QDs and attributed to photooxidation of the CdSe core.20 For oxidation to take place, oxygen has to diffuse through the ZnS shell. Therefore, our data demonstrated that the CdSe core was well passivated by the ZnS shell in the QDs studied in this research work. The diminished ΦF of the organic-soluble QDs after their irradiation suggested photooxidation of mainly the ZnS layer,21 since it was accompanied by only a slight blue-shift of the emission maximum. In addition, the intensity decrease can be caused by the formation of lattice defects in the core-shell QDs.21
λ max exciton | λ max emission | Φ F | |||||||
---|---|---|---|---|---|---|---|---|---|
before irradiation | after irradiation under N2 Air | before irradiation | after irradiation under N2 Air | before irradiation | after irradiation under N2 Air | ||||
QD-CS2 | 521 | 520 | 520 | 539 | 537 | 538 | 0.61 | 0.31 | 0.22 |
CS2@KP | 520 | 515 | 515 | 540 | 535 | 533 | 0.70 | 0.44 | 0.47 |
QD-CS3 | 564 | 564 | 563 | 582 | 581 | 581 | 0.63 | 0.53 | 0.42 |
CS3@MUA | 571 | 572 | 570 | 595 | 594 | 592 | 0.54 | 0.52 | 0.39 |
CS3@MPA | 566 | 566 | 567 | 586 | 588 | 587 | 0.45 | 0.46 | 0.49 |
In addition, the photostability in air of the QDs covered with chemisorbed thiol ligands was higher than that of the amine-capped CdSe/ZnS QDs (see comparison between QD-CS3 (toluene) and CS3@MPA (water) in Fig. 8, and between QD-CS2 (toluene) and CS2@KP (toluene) in Fig. 9. Moreover, CS3@MPA exhibited an improved fluorescence (10%) after 5 h irradiation. This could be explained by the removal of recombination centers, created during the ligand exchange, by illumination.22
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Fig. 8 Normalized fluorescence spectra of aerated solutions of CS3@MPA (water), before (■) and after (•) 270 min irradiation at λ > 400 nm. Inset: comparative fluorescence spectra of QD-CS3 (toluene). |
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Fig. 9 Normalized fluorescence spectra of aerated toluene solutions of CS2@KP, before (■) and after (•) 270 min irradiation at λ > 400 nm. Inset: comparative fluorescence spectra of QD-CS2. |
The fluorescence of the amine-capped QDs also drastically decreased after irradiation under anaerobic conditions (though less than under air atmosphere conditions). However, irradiation of CS2@KP, CS3@MUA, and CS3@MPA in the presence or absence of oxygen made little difference and only slightly affected the QD fluorescence performance (Fig. 10, Fig. S7 and S8, ESI,† and Table 1).
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Fig. 10 Normalized fluorescence spectra of deaerated toluene solutions of CS2@KP, before (■) and after (•) 270 min irradiation at λ > 400 nm. Inset: comparative fluorescence spectra of QD-CS2. |
Footnote |
† Electronic supplementary information (ESI) available: additional emission spectra of the QDs before and after irradiation under nitrogen and air atmosphere, UV-visible spectra, HRTEM images, XPS spectra, and physical data of the QDs. See DOI: 10.1039/c1ra01005k |
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