Characterisation of different polymorphs of tris(8-hydroxyquinolinato)aluminium(III) using solid-state NMR and DFT calculations
© Goswami et al 2009
Received: 12 May 2009
Accepted: 09 November 2009
Published: 09 November 2009
Organic light emitting devices (OLED) are becoming important and characterisation of them, in terms of structure, charge distribution, and intermolecular interactions, is important. Tris(8-hydroxyquinolinato)-aluminium(III), known as Alq3, an organomettalic complex has become a reference material of great importance in OLED. It is important to elucidate the structural details of Alq3 in its various isomeric and solvated forms. Solid-state nuclear magnetic resonance (NMR) is a useful tool for this which can also complement the information obtained with X-ray diffraction studies.
We report here 27Al one-dimensional (1D) and two-dimensional (2D) multiple-quantum magic-angle spinning (MQMAS) NMR studies of the meridional (α-phase) and the facial (δ-phase) isomeric forms of Alq3. Quadrupolar parameters are estimated from the 1D spectra under MAS and anisotropic slices of the 2D spectra and also calculated using DFT (density functional theory) quantum-chemical calculations. We have also studied solvated phase of Alq3 containing ethanol in its lattice. We show that both the XRD patterns and the quadrupolar parameters of the solvated phase are different from both the α-phase and the δ-phase, although the fluorescence emission shows no substantial difference between the α-phase and the solvated phase. Moreover, we have shown that after the removal of ethanol from the matrix the solvated Alq3 has similar XRD patterns and quadrupolar parameters to that of the α-phase.
The 2D MQMAS experiments have shown that all the different modifications of Alq3 have 27Al in single unique crystallographic site. The quadrupolar parameters predicted using the DFT calculation under the isodensity polarisable continuum model resemble closely the experimentally obtained values. The solvated phase of Alq3 containing ethanol has structural difference from the α-phase of Alq3 (containing meridional isomer) from the solid-state NMR studies. Solid-state NMR can hence be used as an effective complementary tool to XRD for characterisation and structural elucidation.
In organic based semiconductor devices, molecular solids of organic molecules are used in active layers . The properties of amorphous solid thin films can be different from the properties of isolated molecule, due to interaction among the molecules in solid state. The properties of amorphous solid thin films are mainly decided at the molecular level and modulated by intermolecular interactions and other bulk properties. Hence, it is important to have information about the structure of the organic molecule, charge distribution on the molecular framework, and intermolecular interactions as they collectively govern the performance of the device.
Following the experimental demonstration by Tang et al.  Tris(8-hydroxyquinolinato)- aluminium(III), known as Alq3, has become a workhorse material for organic light emitting devices (OLED) and/or electron transporting material in OLED. Alq3 is an octahedrally coordinated chelate complex, with an Al3+ ion in the center and three 8-hydroxyquinolinate ions octahedrally coordinated around it. It has mainly two types of geometrical isomeric forms, meridional and facial. Brinkmann et al. investigated the light emitting properties of the isomeric states and the polymorphs of Alq3 and determined that molecular packing plays a significant role . X-ray diffraction studies showed that the two crystalline polymorphs of Alq3, α and β forms, are mainly composed of the meridional isomer . Recently a new crystalline phase of Alq3, namely δ-Alq3, was discovered . It shows blue luminescence which is markedly different from the meridional isomer which shows green luminescence. The quantum yield is also higher in the δ-phase. These results suggest that there is a clear correspondence between the crystal structure of Alq3 and the photoluminescence property. Extensive studies on the δ-phase of Alq3 have been carried out and it was suggested that δ-Alq3 is composed purely of facial Alq3 [5, 6]. Again in the case of charge carrier transport in Alq3, intermolecular interactions play the most crucial role . Also, it has been a practice to use different dopants in Alq3 emitting layers to obtain desired colours . Such Alq3 systems which accommodate small solvent molecules within its crystal matrix are in general known as solvated Alq3. It was also reported that the unit crystal structure and the crystal packing change in Alq3 when it hosts small solvent molecules, which resulted in a small red shift in the fluorescence spectra .
Considering the above stated facts, it becomes important to have insight about the structure of Alq3 in both the solvated and the unsolvated form and about the in-tramolecular and intermolecular interactions. Though X-ray diffraction is a powerful tool to yield insight into the structure of crystalline material, solid-state NMR can be as good in providing similar information. In addition, solid-state NMR is particularly suitable for studying disordered or amorphous materials [8–13]. Since Alq3 has an Al3+ ion in the centre, one can make use of it as a probe to monitor the electronic distribution in the molecule. 27Al is well suited for solid-state NMR because of its high natural abundance (100%) and relatively large gyromagnetic ratio. Since 27Al has spin I = 5/2, it possesses a quadrupolar moment . It is possible to record and analyse solid-state 27Al MAS NMR spectra, observing the central m = +1/2↔-1/2 magnetic transition under magic-angle spinning (MAS), which, for well-resolved spectra, exhibits a characteristic second-order order broadening. High-resolution quadrupolar spectra can be obtained with two-dimensional (2D) methods such as multiple-quantum MAS (MQMAS) . This can help in identifying the various quadrupolar sites in a system and in obtaining the quadrupolar parameters [16, 17]. The study of quadrupolar parameters with solid-state NMR can provide a wealth of information about the local environment around quadrupolar nuclei, as the quadrupolar parameters show strong dependence on the neighbouring electronic environment [14, 18].
Octahedral chelate complexes, which are structurally similar to Alq3, were studied by Schurko and co-workers using one-dimensional (1D) 27Al MAS NMR spectroscopy . They showed that the change of structural environment about the aluminium centres can be easily investigated by studying the quadrupolar parameters of 27Al nuclei of the organic chelate complexes. They also reported how the distortion in the chelate rings leads to larger value of quadrupolar coupling constant in one of the complexes.
Recently Utz et al. [10, 11] have successfully used 1D MAS 27Al spectroscopy to differentiate between the α phase and the δ phase of Alq3 and to characterize the structural disorder of amorphous Alq3 deposited from vapour phase at different rates. They also estimated the EFG tensor on the basis of point charge model and predicted the asymmetry parameters of the α and the δ phase . Kaji et al. have done a similar study by recording 1D 27Al spectra under static and MAS condition to characterise the α phase, the δ phase, and the γ phase of Alq3 and also amorphous Alq3 . However unlike Utz et al. they have used DFT based quantum-chemical calculations to theoretically predict the value of the asymmetry parameters of the α phase and the γ phase. Their study suggested that whilst the α phase contains a non axially symmetric isomer both the δ phase and the γ phase of Alq3 contain an axially symmetric form.
Here, we have investigated three types of Alq3 samples: (a) α phase (containing the meridional isomer), (b) δ phase (containing the facial isomer), and (c) solvated phase (containing ethanol in the crystal lattice) using solid-state NMR combined with density functional theory (DFT)  based quantum chemical calculation. We show with MQMAS experiments that in all the polymorphs, 27Al is present in a single crystallographic site. We further demonstrate that the local environment around 27Al in solvated phase is different from that in the α phase with the use of both 1D MAS and 2D MQMAS experiments. We also made use of DMFIT  program to model the 1D MAS spectra of all the polymorphs to extract the quadrupolar parameters and we have compared the results with the previous works. In addition the anisotropic slices of the peaks in 2D MQMAS spectra were modelled using the DMFIT program to extract the quadrupolar parameters and isotropic chemical shifts. We further report the result obtained from DFT based quantum-chemical calculation done on isolated molecule and show that the correspondence with the experimental results improve when the calculation is done under the solvation model.
Preparation of Alq3and X-ray diffraction measurements
Alq3 was prepared from 8-hydroxyquinoline and Al(NO3).9H2O using an aqueous route by a standard procedure . Briefly the procedure adopted was as follows: 1 g of aluminium nitrate (Al (NO3)3).9H2O was dissolved in 100 ml of water. The solution was warmed to 60°C. 1.5 g of 8-hydroxyquinoline was dissolved in a solvent mixture of 20 ml of water and 4 ml of glacial acetic acid. 8-hydroxyquinoline solution was slowly added to aluminium nitrate solution. The pH of the resulting solution was then increased to 8 by the addition of ammonia to precipitate Alq3 out. The resulting precipitate was washed by hot (60°C) water. The bright yellow powder was dried in oven for overnight. Yield of Alq3 obtained by this method was 95-100% with a melting point > 300°C. This procedure was adapted from Vogel .
Steady-state fluorescence of powdered Alq3 samples was recorded at room temperature using a Spex Fluorolog fluorimeter. The excitation wavelength was 340 nm and scanned at a step of 1 nm.
Thermo-gravimetric analysis (TGA) and differential thermal analysis (DTA) were performed with a NETZSCH instrument. The temperature was varied at 5 K/min under nitrogen atmosphere.
All NMR experiments were carried out on a Bruker Avance 500 MHz spectrometer operating at a field strength of 11.7 T with a Bruker 4 mm triple-resonance probe. Experiments were performed observing the central transition of 27Al (I = 5/2) resonance of the different forms of Alq3 sample at a Larmor frequency of 130.28 MHz. Magic-angle spinning was performed at 10 kHz. The nutation frequency of the excitation pulse for the 1D MAS experiments was 120 kHz. For the 2D experiments the split-t1 sequence proposed by Brown and Wimperis was used . A nutation frequency of 80 kHz was applied for excitation and conversion pulses. The echo time was 2.5 ms. The pulse width of the selective 180° pulse was 27.8 μs. Further experimental details are given in the figure captions of Figs. Three-Six. The chemical shifts were referenced to aqueous 1 M AlCl3 solution. The isotropic quadrupolar shifts from the MQMAS spectra, , were calculated using the method given in Ref. . In all the experiments swept-frequency two pulse phase modulation (SW f -TPPM)  heteronuclear dipolar scheme was applied to remove the 1H-27Al dipolar couplings .
The 27Al quadrupolar parameters obtained from the DFT quantum-chemical calculation under the isolated molecule and the isodensity polarisable continuum model (IPCM).
δ iso (ppm)
where α is the isotropic polarisability, ρ is the density, M is the molecular mass, N A is the Avogadro number, and ε is the dielectric constant. Isotropic polarisability (α) and reciprocal of Molar volume (ρ/M) were calculated from geometry optimised structure of the isomers using the DFT method (B3LYP/6-31G (d)). The experimentally determined value of ε for thin film, which predominantly contains the meridional isomer, was found to be 3.0 ± 0.3 . As the computationally determined values for both the isomers were nearly the same, the experimentally determined value of ε for thin film was used in the IPCM calculation for both the isomers. The levels of basis functions were the same for both the gas phase and the solid solvated phase.
Results and discussion
We present here the results obtained from the α and the δ forms of Alq3 and also from the solvated phase of Alq3 using 1D MAS and 2D MQMAS NMR experiments. The quadrupolar parameters were obtained by fitting the 1D MAS spectra and the anisotropic slices of the 2D spectra of the three phases using the DMFIT program. We also report the theoretically calculated values of the quadrupolar parameters using the DFT calculations of the α and the δ forms of Alq3.
NMR and XRD of isomeric forms of Alq3
The 27Al quadrupolar parameters obtained from the 1D MAS and the 2D MQMAS experiments using the DMFIT program.
δ iso (ppm)
55.4 ± 1.0
0.80 ± 0.04
7.0 ± 0.1
43.6 ± 1.0
0.18 ± 0.03
4.9 ± 0.1
50.5 ± 1.0
0.62 ± 0.04
6.4 ± 0.1
Solvated Alq3 after the removal of ethanol
55.1 ± 2.0
0.85 ± 0.05
6.5 ± 0.3
54.7 ± 1.0
0.85 ± 0.04
6.9 ± 0.1
43.1 ± 1.0
0.15 ± 0.03
5.1 ± 0.1
50.4 ± 1.0
0.60 ± 0.04
6.4 ± 0.1
Solvated Alq3 after the removal of ethanol
55.0 ± 2.0
0.81 ± 0.04
6.9 ± 0.3
The quadrupolar parameters in Table 2 indicate that the α phase of Alq3 contains only the meridional isomer as reported from the XRD study  and the δ phase of Alq3 is composed of purely facial isomer as reported from the XRD study .
DFT calculation of EFG principal values were done for isolated Alq3 molecule. The asymmetry parameter η Q obtained for the α-form was 0.77 while η Q for the δ-phase of Alq3 came to be 0.03. Previously Kaji et al.  also did similar kind of DFT calculations where they predicted that the η Q values for the α-form and the γ form of Alq3 are 0.72 and 0.0 respectively. They also reported that the DFT calculation for the δ-phase yielded inconsistent results. Utz et al.  carried out a simple calculation for the estimation of EFG tensor on the basis of the assumption that the EFG tensor is determined by three point charges of -e at the oxygen sites. However, the values of η Q predicted by this model (0.91 for meridional and 0.26 for facial) overshoot the experimental values obtained by us for both the isomers.
Here we propose a model for DFT calculation where molecules are considered under the influence of a continuum dielectric medium (IPC model) which is a more realistic situation. Under this model it is observed that the theoretically predicted values (0.81 for meridional and 0.10 for facial) show a relatively good agreement with the experimental values. In the case of solvated Alq3, it was not possible to take a suitable model for the DFT calculation.
We have performed 1D MAS and 2D MQMAS experiments to obtain high-resolution spectra of meridional (α-phase) and facial (δ-phase) isomers of Alq3. We have determined the quadrupolar parameters from 1D MAS spectra using the DMFIT program. The 2D MQMAS experiments have shown that all the different modifications of Alq3 have 27Al in single unique crystallographic site which is evident from the single isotropic peak along F1 dimension. The quadrupolar parameters were also predicted using the DFT calculation under isolated molecule assumption and also under the IPC model. The theoretically calculated values of quadrupolar parameters improve and come close to the experimentally obtained values when calculations are done under the IPC model where an Alq3 molecule is assumed to be solvated in a surrounding of similar Alq3 molecules, which is the closest to the actual situation. Solid-state NMR data indicate that the solvated phase of Alq3 containing ethanol has structural difference from the α-phase of Alq3 (containing meridional isomer). This was also confirmed by the XRD features, though the fluorescence spectra did not show any significant difference between them which again reaffirms the fact that fluorescence is determined at molecular level in Alq3 and does not depend on the crystal structure. Further the isotropic projection of the solvated Alq3 is much narrower than all the other polymorphs, which could be due to dynamic exchange processes. Thermo-gravimetric analysis show that there is one ethanol molecule per Alq3 in the solvated form. After the removal of ethanol the solvated Alq3 becomes structurally similar to the α-phase of Alq3. However, due to the possible introduction of more than one polymorph during re-crystallisation, broader ridges appear in the 2D 3QMAS spectrum of the apohost Alq3. Solid-state NMR can hence be used as an effective complementary tool to XRD for characterisation and structural elucidation. A more realistic approach to the calculation of the EFG tensor would be to consider the molecule to be solvated by similar molecules (IPC model).
During the review process of this manuscript similar findings were published by Nishiyama et al. . They report two distinct sites for α-Alq3 which is at variance to our observation. This could be due to the differences in the sample preparation conditions as it seems Nishiyama et al. have collected all the portions from the train sublimations whilst we have collected the portions from a hot region (~170°C) and near the sublimation boat. The α-Alq3 sample in the current work was also characterised by powder XRD.
We acknowledge the use of National Facility for High-Field NMR, TIFR, for the use of the Bruker AV500 spectrometer, Thomas Bräuniger for discussions and a careful reading of the manuscript, and M. V. Naik for technical assistance.
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