X. Y. Xu and
B. Yan*
Department of Chemistry, Tongji University, State Key Lab of Water Pollution and Resource Reuse, Siping Road 1239, Shanghai 200092, China. E-mail: byan@tongji.edu.cn; Fax: +86-21-65981097; Tel: +86-21-65984663
First published on 5th August 2014
In this paper, series of luminescent hybrid materials (alumina, titania) functionalized with both lanthanide complexes and metal organic frameworks (MOF, Al-MIL-53-COOH) through coordination bonds. In these hybrid systems, both MOF and lanthanide (Eu3+, Tb3+) complexes with beta-diketonates (2-thenoyltrifluoroacetonate (TTA), 1,1,1-trifluoroacetylacetone (TAA), 2,4-pentanedionate (AA)) and pyridine-3,5-dicarboxylic acid (PDA) are coordinated to alumina and titania through their carboxylic groups. Al-MIL-53-COOH possesses the active –COOH group and can be linked to metallic alkoxides (Ti[OCH(CH3)2]4 and Al[OCH(CH3)2]3), by a post-synthesis path. Ternary complexes of beta-diketonates and PDA can be further bonded with metallic alkoxides through PDA as a bridge for its carboxylic group coordination. After hydrolysis and a condensation process, the final multi-component hybrid materials can be assembled and characterized. The photophysical properties of these hybrid materials were studied in detail, and their luminescent color can be tuned by controlling the composition of different units in the hybrid system. Especially with the hybrids of europium complexes and MOF, the white luminescence can be obtained by integrating the emission of both europium complex and MOF. Furthermore, the luminescent films that were prepared show both uniformity and transparency. These results provide some useful data for the multi-component assembly and luminescent integration of photofunctional hybrid materials based on MOF and lanthanide units, which can be expected to have some potential applications in luminescent devices for display or lighting.
Furthermore, the amorphous organically modified silica network hybrids can be transferred to ordered mesoporous silica with special surfactants or other templates, whose regular pore structure, high photostability and thermal stability provide a suitable host for guest–host assembly chemistry of photoactive species. Nowadays, lanthanide hybrids based on a functionalized mesoporous host have been prepared, involving MCM-41(48), mesoporous silica (SBA-15(16)) and polyoxometalates (POMs), and so on.11–13 The highly ordered structures and uniform tunable pore sizes mean that the applications of these photofunctional hybrids can be expanded into the optical or electronic areas.
But the silica-derived hybrid materials including mesoporous hybrids mainly belong to the group of amorphous-state materials, whose non-crystalline nature makes it very difficult to study their composition and structure in the hybrid system. In order to address this problem, one approach is to introduce a crystalline unit into the hybrid system to keep the exact coordination environment around lanthanide ions, such as lanthanide polyoxometallates as the central species.14,15 A more extensive strategy is to functionalize the crystalline host, such as traditional microporous zeolite, and some host–guest hybrid materials based on zeolite were developed.16 Metal organic frameworks (MOFs) are crystalline materials with regular porous networks constructed from organic linker molecules and metal ions.17 Luminescent MOFs possess high, well-defined porosity and show intense fluorescence, and have gained considerable attention because of their potential applications in chemical sensors, light emitting devices and biomedicine.18 The abundant groups in the MOFs make it possible for them to be modified by the so-called post-synthesis strategy.19 This provides great potential for constructing a hybrid system based on MOFs.
Al-MIL-53-COOH has a high crystalline framework that consists of regular one-dimensional channels (Fig. S1 in ESI†), which show high structural flexibility.20 The presence of a non-coordinating carboxyl group, as well as the high thermal and chemical stabilities makes it a good candidate for assembling hybrid materials with other photoactive units. So in this paper, we report on the fabrication of Al-MIL-53-COOH and lanthanide complexes in inorganic matrices (alumina or titania) using co-ordination bonds to assemble the multi-component hybrid materials, whose physical characterization and luminescent properties are studied in detail.
Fig. 2a depicts the FTIR spectrum of compound MOF. The peak at 3454 cm−1 is in a high frequency region and corresponds to the adsorbed water molecules. The absorption peaks at 1675 cm−1 (νas) and 1453, 1419 cm−1 (νs) suggest the presence of carboxylic acids and carboxylate. The absorption peaks at 1170 and 785 cm−1 are ascribed to the C–H deformation vibrations of the aromatic ring. Fig. 2b shows the selected FTIR spectra of the final hybrids: Eu-TTA/TAA-Ti/Al-MOF. The characteristic stretching vibrations of the coordinating carboxylate groups are easily visible, νas at 1613 and νs at 1402 or 1379 cm−1, revealing that the further coordination to Ti or Al in the hybrids produces the red-shift of frequency of the COO− group in MOF. The presence of water molecules can be shown by the broad band in a high frequency region over 3200 cm−1.
Fig. 3 shows the selected SEM images of the hybrids TAA-Tb-PDA-Al-MOF (a) and TTA-Eu-PDA-Ti-MOF (b), respectively. Both of them show little difference between their morphology. Compared to the bulk Tb-TAA-Al-MOF hybrids, Eu-TTA-Ti-MOF shows a softer and finer microstructure. This may be related to the different sol–gel reaction behaviour of Al and Ti precursors.
Fig. S3† shows the XRD patterns (from 10 to 70°) of hybrid materials L-Eu/Tb-PDA-Al/Ti-MOF (a) alumina system and (b) titania system (Eu3+, L = TTA, TAA; Tb3+, L = TAA, AA). Both of the alumina and titania hybrids present in the dominant broad band belong to alumina or titania gels (Al–O network and Ti–O network) in the amorphous state. Because there is a limited amount of MOF in the hybrids for fabrication, the crystalline diffraction peaks for MOF cannot be identified clearly in these XRD patterns. Comparing the two figures, the Eu-TTA/TAA-Al-MOF hybrids seem to show slightly better crystallization than the Eu-TTA/TAA-Ti-MOF systems, which is consistent with the SEM of the product obtained. Considering the same Al3+ ion component in both MOF and alumina, the corresponding crystalline state may be good. It needs to be made clear that in the hybrid system, the host is titania or alumina and the lanthanide complex or MOF are all active units in the titania or alumina host. Therefore, MOF and the lanthanide complex are both present in a small amount in the larger amount of the host titania or alumina. So the final powder X-ray diffraction (PXRD) patterns present the main features of the host titania or alumina and it is hardly worth checking the characteristics of the lanthanide complex or the MOF. Naturally, it is impossible to show clearly the crystalline character of MOF from the PXRD pattern. In addition, for the previously mentioned reason, the structure of TTA-Eu-PDA-Ti@MOF and TTA-Tb-PDA-Ti@MOF, TAA-Tb-PDA-Al@MOF and TAA-Eu-PDA-Al@MOF obtained from XRD analysis should show mainly the characteristics of amorphous titania for TTA-Eu-PDA-Ti@MOF and TTA-Tb-PDA-Ti@MOF and of alumina for TAA-Tb-PDA-Al@MOF and TAA-Eu-PDA-Al@MOF, respectively, but no characteristics are present from MOF as it is limited in its content.
Fig. 4 presents the N2 adsorption–desorption isotherms of the compounds: Al-MIL-53-COOH (MOF) and TTA-Eu-PDA-Al/Ti-MOF hybrids. It indicates that the final hybrid material can show porosity toward N2. Unlike other microporous materials, both show a type I adsorption curve, and these samples display typical type IV curves with hysteresis loops at high relative pressure. The steric hindrance of the free non-coordinated carboxyl groups in the channels of MOF leads to the atypical hysteresis of the N2 adsorption isotherms, which reduces the access of N2 molecules. TTA-Eu-PDA-Al/Ti-MOF samples exhibit similar sorption behavior with MOF. The BET surface area of Al-MIL-53-COOH(MOF) is 394 m2 g−1, whereas the hybrid TTA-Eu-PDA-Al/Ti-MOF samples exhibit similar sorption behavior to Al-MIL-53-COOH (MOF). The BET surface areas of TTA-Eu-PDA-Al-MOF and TTA-Eu-PDA-Ti-MOF are 345 m2 g−1 and 339 m2 g−1, respectively, and show a reasonable reduction in comparison with the surface area of Al-MIL-53-COOH (MOF); this may be because the uploading of some small molecules exists in the hybrid alumina or titania host. MOF is fabricated in an alumina or titania host and can easily be affected by other components within the host.
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Fig. 4 N2 adsorption–desorption isotherms of compound Al-MIL-53-COOH (MOF) and TTA-Eu-PDA-Al/Ti-MOF. |
The excitation and emission spectrum and the International Commission on Illumination (CIE) chromaticity diagram of MOF (Al-MIL-53-COOH) are shown in Fig. S4.† The maximum excitation and emission wavelengths are 372 nm and 420 nm, respectively. These can be ascribed to the excitation and emission of the trimellitic acid ligand. The corresponding CIE chromatic coordinate of MOF is located in the light blue region, which can be composed of the luminescent species in the yellow-orange-red region to white emission. This predicts what can be proved from the following hybrids of fabricated Eu3+ complexes.
Fig. 5 shows the luminescent excitation and emission spectra of Tb hybrids: TAA-Tb-PDA-Al-MOF (A), AA-Tb-PDA-Al-MOF (B), TAA-Tb-PDA-Ti--MOF (C) and AA-Tb-PDA-Ti-MOF (D). Their excitation bands are similar with wide range of 250–350 nm, corresponding to the excitation of the beta-diketonates and the carboxylic acid unit of MOF. No excitation peaks to the f–f transitions of Tb3+ can be detected. In the titania hybrid system, the excitation bands become narrow and another wide excitation band in the visible region can be observed. This may be because the titania is not so favourable as alumina for luminescence of Tb3+ complexes, which were found in many previous studies.20 Organic ligands absorb the energy and then transfer it to the accepting energy level of the lanthanide ions. The wide excitation bands are favourable for the energy transfer and luminescence of Tb3+. The corresponding emission spectra of all terbium hybrids present the characteristic luminescence of Tb3+, while no emission of MOF could be detected. The emission lines are assigned to the 5D4 → 7FJ transitions of Tb3+, locating at around 490, 545, 587 and 623 nm, for J = 6, 5, 4 and 3, respectively. The most striking green luminescence is for the 5D4 → 7F5 transition. In addition, it can be seen that no excitation and emission bands for MOF can be detected, suggesting that there is no overlap and energy transfer between the MOF and terbium complexes.
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Fig. 5 The excitation and emission spectra of terbium hybrid materials TAA-Tb-PDA-Al-MOF (A), AA-Tb-PDA-Al-MOF (B), TAA-Tb-PDA-Ti-MOF (C) and AA-Tb-PDA-Ti-MOF (D). |
Fig. 6 shows the luminescent excitation and emission spectra of hybrids TAA-Eu-PDA-Al-MOF (a) and TTA-Eu-PDA-Al-MOF (b), respectively. Different from the previous terbium hybrids, the excitation spectra by monitoring the emission of Eu3+ at 614 nm show both excitation of organic ligands and the f–f transition of Eu3+. A broad excitation band from 250 to 380 nm centered at about 320 nm (TAA-Eu-PDA-Al-MOF) and 340 nm (TTA-Eu-PDA-Al-MOF) in the UV region, which is attributed to the absorption from the organic ligands to form the charge transfer state (CTS) of Eu–O. The shoulder excitation bands at a low wavelength of 270 or 280 nm suggests the excitation of TTA or TAA ligands. At the same time, there exist peaks at around 396 and 467 nm because of the narrow f–f absorption transition (7F0 → 5L6 and 7F0 → 5D2) of the Eu3+ ion, whose intensity is much weaker than the absorption from organic ligands. The emission bands of the two hybrid materials are assigned to the 5D0 → 7FJ (J = 0–4) transitions of Eu3+ at 580, 591, 614, 652, and 700 nm under two different kinds of excitation wavelengths (320/340 nm, 330/348 nm). It is worth noting that different excitation wavelengths may have an influence on the emission spectra, which is apparently shown in Fig. 6a. At excitation of 340 nm, both emission of MOF and the Eu-TAA complex can be observed and the different luminescence spectral position in the visible region may be expected to adjust the final luminescence color of the hybrids. This will be shown clearly in the following CIE diagrams. For the excitation at 320 nm, there is no apparent luminescence of MOF observed but the red emission of europium TAA complexes is present. From these results, it can be found that the excitation at 320 nm is mainly from the ligands of TTA forming the CTS, however, this is not true for MOF. The absorption at 340 nm does not produce the strong emission of Eu3+ and it overlaps with the excitation of MOF in Fig. S4.† So the emission of MOF can be observed. For TTA-Eu-PDA-Al-MOF hybrids, no distinction appears for the two different excitation wavelengths, where two emissions of MOF and Eu-TTA are both observed.
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Fig. 6 The excitation and emission spectra of the hybrids TAA-Eu-PDA-Al-MOF (a) and TTA-Eu-PDA-Al-MOF (b). |
The luminescent spectra of titania hybrids are shown in Fig. 7. The excitation spectra by monitoring the emission of Eu3+ at 614 nm from europium hybrids shows both excitation of the organic ligands and the f–f transition of Eu3+, which causes the apparent distinction. For Eu-TAA-Ti-MOF hybrids, the excitation spectrum consists of a broad excitation UV band from 250 to 350 nm centered at about 300 nm and a series of sharp excitation peaks from 350 to 500 nm in the UV-vis region. The former is ascribed to the absorption from the organic ligands forming the CTS of Eu–O. The latter belongs to the f–f absorption transition (327 nm, 7F0 → 5H6; 363 nm, 7F0 → 5D4; 383 nm, 7F0 → 5G2; 394 nm, 7F0 → 5L6, strongest; 415 nm, 7F0 → 5D3; 467 nm, 7F0 → 5D2) of the Eu3+ ion.23 It is worth pointing out that the intensity of them is strong, even stronger than the absorption from organic ligands, whereas for Eu-TTA-Ti-MOF hybrids, the CTS excitation from the organic ligand is much stronger than the f–f transition so that only two narrow f–f absorption transition (7F0 → 5L6, 396 nm and 7F0 → 5D2, 466 nm) of Eu3+ ion can be seen. The excitation at 396 nm appears as a shoulder peak in the broad excitation bands of CTS (300–450 nm range, centered at 370 nm). Both of the two hybrids show the similar shape of emission spectra consisting of the Eu3+ ion and MOF. The emission to the 5D0 → 7FJ (J = 0–4) transitions of Eu3+ is located at 580, 591, 614, 652, and 700 nm. The appearance of a wide emission of MOF at 400 to 580 nm may be expected to integrate with the emission of Eu3+, which is shown in the following CIE diagrams.
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Fig. 7 The excitation and emission spectra of hybrid materials TTA-Eu-PDA-Ti-MOF (a) and TAA-Eu-PDA-Ti-MOF (b). |
Fig. 8 shows, from left to right, photographs of four hybrid materials TAA-Tb-PDA-Al-MOF, TAA-Eu-PDA-Al-MOF, TTA-Eu-PDA-Al-MOF and TAA-Eu-PDA-Ti-MOF, respectively. Of these, three hybrids are based on alumina, and the TAA-Tb-PDA-Al-MOF and TAA-Eu-PDA-Al-MOF hybrids show the typical bright green for Tb3+ and the red emission for Eu3+, whereas Eu-TTA-Al-MOF hybrids present an emission that is a pink-white color. For Eu-TAA-Ti-MOF hybrids, there is a luminescence with a color which is close to white. So these hybrids can realize the multi-color light output by adjusting the component and excitation wavelengths.
Fig. S5† shows the CIE diagrams of the spectra in Fig. 6 and 7, TAA-Eu-PDA-Al-MOF (a), TTA-Eu-PDA-Al-MOF (b), TTA-Eu-PDA-Ti-MOF (c) and TAA-Eu-PDA-Ti-MOF (d), respectively. From these four diagrams, it can be found that selecting the excitation with a suitable wavelength can realize the output of luminescence with a color which is close to white. For TAA-Eu-PDA-Al-MOF hybrids, the white colored luminescence can be obtained using a λex of 320 nm, whereas the blue-white emission is obtained using a λex of 340 nm. For TTA-Eu-PDA-Al-MOF hybrids, the two excitation wavelengths show the CIE coordinates in a color which is close to white (330 nm) and pink-white (348 nm) region. For the two kinds of hybrid materials based on titania (TTA-Eu-PDA-Ti-MOF, TAA-Eu-PDA-Ti-MOF), they both show the typical white luminescence. The parent MOF and the other hybrid systems present blue and green colored emission, respectively, and their CIE diagrams of spectra are shown in Fig. S6.† The detailed CIE coordinates are summarized in Table 1.
Materials | λem (nm) | λex (nm) | Color (CIE-X, Y) | η (%) |
---|---|---|---|---|
Al-MIL-53-COOH (MOF) | 420 | 372 | Blue (0.1669, 0.1398) | 17.0 |
TTA-Eu-PDA-Al-MOF | 614 | 330 | Close white (0.3456, 0.2604) | 3.3 |
614 | 348 | Pink-white (0.3160, 0.2261) | 3.7 | |
TAA-Eu-PDA-Al-MOF | 614 | 320 | White (0.3602, 0.3186) | 11.1 |
614 | 340 | Blue-white (0.2692, 0.2379) | 13.2 | |
TAA-Tb-PDA-Al-MOF | 545 | 321 | Green (0.2972, 0.6030) | 8.2 |
AA-Tb-PDA-Al-MOF | 545 | 315 | Green (0.3062, 0.5984) | 15.6 |
TTA-Eu-PDA-Ti-MOF | 614 | 330 | White (0.3525, 0.2844) | 0.9 |
TAA-Eu-PDA-Ti-MOF | 614 | 360 | White (0.3272, 0.2804) | 4.5 |
TAA-Tb-PDA-Ti-MOF | 545 | 302 | Green (0.2807, 0.5061) | 0.7 |
AA-Tb-PDA-Ti-MOF | 545 | 314 | Green (0.2901, 0.5358) | 0.4 |
Furthermore, the absolute luminescence quantum yield data are obtained with an integrating sphere and a calibrated detector setup for solid materials. The resulting absolute luminescence quantum yields are listed in Table 1. The luminescent quantum yields of the hybrids based on alumina are higher than those with titania, which is in agreement with the results reported for other lanthanide hybrids functionalized with alumina and titania.21,22 Alumina is more favourable for the luminescence of lanthanide species than tiania.21,22 The rule of the η values of them is not apparent for the complicated hybrid system, TAA-Eu-PDA-Al-MOF hybrid material shows white color luminescence and 11.1% quantum efficiency (λex = 320 nm), which would benefit from further study. For comparison, we selectively measured the luminescent quantum yields of four lanthanide hybrid (alumina or titania) materials themselves without MOF: they are 21.4% (TAA-Eu-PDA-Al), 6.2% (TAA-Eu-PDA-Ti), 17.0 (TAA-Tb-PDA-Al) and 2.1% (TAA-Tb-PDA-Ti). These values are all higher than those of hybrids with both lanthanide complexes and MOF, which is because of the much lower content of lanthanide complexes in the hybrids with MOF than those of hybrids without MOF.
Furthermore, we then tried to prepare the hydrogel thin films based on TTA-Eu-PDA-Ti-MOF (a, left) and TAA-Eu-PDA-Ti-MOF (b, right) hybrids, whose pictures are shown in Fig. S7.† Both of the two hybrid thin films were uniform and transparent, suggesting that it is feasible to prepare such hybrid thin films for further optical application. Fig. S8† shows the excitation and emission spectra of hybrid thin films fabricated with TTA-Eu-PDA-Ti-MOF (a) and TAA-Eu-PDA-Ti-MOF (b), which present similar features as the spectra of their powder samples. Their luminescent spectra consist of the emission from both europium beta-diketonates (TTA, TAA) and a MOF functionalized titania host in the red region and blue-green one, respectively, integrating the white color luminescence. Fig. 9a and (b) show the photograph and CIE diagrams of the two hybrid thin films.
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Fig. 9 The photograph (left) and CIE chromaticity diagram (right) of the thin films prepared with TTA-Eu-PDA-Ti-MOF (a, λex = 330 nm) and TAA-Eu-PDA-Ti-MOF (b, λex = 360 nm) hybrids. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra05704j |
This journal is © The Royal Society of Chemistry 2014 |