Susana
Castelar
a,
Pilar
Romero
a,
José-Luis
Serrano
b,
Joaquín
Barberá
*a and
Mercedes
Marcos
*a
aDepartamento de Química Orgánica, Facultad de Ciencias-Instituto de Ciencia de Materiales de Aragón, Universidad de Zaragoza-CSIC, 50009 Zaragoza, Spain. E-mail: mmarcos@unizar.es; jbarbera@unizar.es
bDepartamento de Química Orgánica, Facultad de Ciencias, Instituto de Nanociencia de Aragón, Universidad de Zaragoza, 50009 Zaragoza, Spain
First published on 28th July 2015
Two novel series of dendrimers synthesised by the ionic grafting of poly(propylene imine) PPI-(NH2)n (n = 4, 8, 16, 32, 64 primary amines on the surface) with bifunctional dendrons of two generations (G1COOH, G2COOH) derived from 2,2-bis(hydroxymethyl)propanoic acid (bis-MPA) were prepared. The dendrons contain a carboxyl group at their apex and electroactive carbazole groups and mesogenic units on their periphery. The occurrence of proton transfer from the carboxylic acid to the amine groups was confirmed by IR and NMR measurements. The liquid crystalline behavior has been investigated by means of differential scanning calorimetry (DSC), polarizing optical microscopy (POM) and X-ray diffractometry (XRD). All ionic dendrimers were liquid crystalline (nematic, smectic or columnar mesophases). The type of mesophase depends on the dendrimer generation as well as on the dendron generation. The electrochemical behavior of the ionic dendrimers was investigated by cyclic voltammetry (CV). Scanning electron microscopy (SEM) studies revealed that electrochemical deposition of the material on the conducting substrate takes place. The UV-vis absorption and emission properties of the ionic hybrid dendrimers have been investigated. All the compounds are luminescent at room temperature and the intensity is related to the number of carbazole units present in the molecule.
In these materials, using a similar approach to that used in side chain liquid crystals polymers (SCLCP), the incorporation of promesogenic units on the periphery of the dendrimeric structures allow us to obtain liquid crystals dendrimers.5 The majority of these mesogenic dendrimers have been obtained using a covalent attachment of the molecules,6 but also the ionic attachment of molecules bearing a carboxylic group to the amine terminal groups of the poly(propylene imine) (PPI) and poly(amidoamine) (PAMAM) dendrimers has demonstrated to be an easy and versatile strategy to produce mesomorphic materials.7 Using this method the incorporation of different functional units could be used in order to prepare multifunctional materials for specific applications. Thus the incorporation of photoactive molecular units, such as carbazole, into liquid crystalline polymers may offer advantages over conventional polymers.8 It is important to take account that carbazole is one of the most familiar electron donors and it has been widely used in the design of fluorescent and hole-transporting materials.9 Thus Preece et al.10 describe in 2001 the first columnar liquid crystal containing carbazole units and in 2002 Velasco et al.11 describe the first carbazole-based lamellar liquid crystal system. Later other liquid crystals functionalized with carbazole units have been reported in the literature.12 In 2012 Manickam et al. have published an interesting review concerning carbazole-based photorefractive liquid crystal materials.13
Recently we have described two families of supramolecular liquid crystal dendrimers based on the self-assembly of carbazole-derived dendrons as the electron-donating group and an electron accepting 1,3,5-triazine core. The photoconductivity of these materials was studied. It was concluded that all of the compounds, both dendrons and complexes, exhibited photoconductivity of the same order of magnitude.14
To date, hybrid dendrimers consisting of two different dendritic polymeric segments are very scarce.8d,15 As a continuation of our investigations, the aim of this work is prepare, through ionic bonding, functional ionic hybrid liquid crystal dendrimers to use the mesomorphic properties as a tool to organize these materials and to evaluate the luminescence and electrochemical properties. Two novel families of dendrimers were synthesized from poly(propylene imine) (PPI) dendrimer generations 1 to 5 (bearing 4, 8, 16, 32, 64 NH2 terminal groups). The PPI was surrounded by carboxylic acid dendrons of two generations G1 and G2 (in future we will denoted as D1 and D2 in order to avoid a mistake with the generations of PPI G = 1–5) bifunctionalized with promesogenic units (family A derived from 5-[4-(4-butoxybenzoyloxy)phenyloxy]pentanoic acid and family B derived from cholesteryl hemisuccinate) and carbazole groups as peripheral hole-transporting moieties and fluorescent units.
The structure of ionic hybrid dendrimers and dendrons are shown in Scheme 1.
The corresponding carbazole-containing dendritic carboxylic acid CzXm (n equiv.) was dissolved in anhydrous tetrahydrofuran (THF). The solution was added to a solution of the corresponding generation (PPI-(NH2)n) (1 equiv.) in anhydrous THF and the mixture was sonicated for 5 minutes. The solvent was then slowly evaporated at room temperature and the resulting solid was dried in vacuum to constant weight for ca. 12 h at 40 °C.
It can be seen, as an example, which the carbonyl group region of the dendron two nearly overlapped bands can be observed at 1737 and 1729 cm−1, assigned to the carbonyl groups of the carboxylic acid and ester, respectively. When the ionic pairs are formed, the signal at 1737 cm−1 disappears and two bands at 1576 and 1405 cm−1 corresponding, respectively, to the asymmetric and symmetric stretching modes of the carboxylate groups in the hybrid ionic dendrimer PPI16CzB1 appeared, whereas the signal at 1728 cm−1 corresponding to the ester remains, (Fig. S1†).
Changes in the region for N–H bonds can also be observed: two bands, corresponding to the N–H bonds of the PPI dendrimer core, disappear and are replaced by a broad band between 3600 and 3200 cm−1, corresponding to the protonated amines (NH3+) of PPI and the N–H bonds of the carbamate groups.
The signals corresponding to the protons of the acid groups are very broad and are barely visible in the 1H spectrum. As a consequence, these signals cannot be taken into account to discuss the formation of the salts. The highest chemical shifts in the dendron part are related to the nuclei nearest to the focal point. Thus, the signals for the protons of the diastereotopic methylene (Hs,s′, see Fig. S2†) and the methyl group β to the carboxylic acid group (Hu) move to higher field in the carboxylate but the signal due to the proton of the carbamate group (–OCONH–) is shifted downfield. Protonation of the primary amine groups on the dendrimer surface is confirmed by the downfield shift of the HB signal α to the terminal amino group (∼0.3 ppm).
13C NMR is more sensitive to this effect than 1H NMR and there are two main pieces of evidence in this respect. Firstly, when the amine is protonated, the signal for the carbon α to NH2 (CB) moves from 40.2/40.6 ppm to 38.6 ppm (data confirmed by an HSQC experiment) and the shifts of the carbon signals belonging to the dendron (Cs,s′) move from 65.48 ppm and 65.78 ppm to 66.84 ppm and 67.24 ppm, respectively. Moreover, the 13C signal of the carboxylic acid group (Cz) is shifted to lower field by between +1 and +4 ppm, the signal for the methylic carbon (Cu) β to the carboxyl group is shifted to lower field from 17.60 ppm to 18.77 ppm and the 13C signal of the carbamate group (Cr′) is also deshielded (from 155.89 ppm to 156.81 ppm) (see Fig. S2†).
The strength of the ionic interaction in solution was assessed by diffusion NMR (DOSY). These studies were carried out on a dendron (CzB1), on PPI dendrimers and on three of zwitterionic dendrimers corresponding to generations 3, 4 and 5 of the PPI dendrimer. Once the diffusion coefficients had been obtained relative to an internal standard18 (TMS) it was observed that the ionic dendrimers behave as single molecules in solution, with only a single diffusion coefficient observed (Fig. 1).
This finding confirms that the ionic bond is strong enough to keep the two parts of the ionic dendrimer linked in solution. In previous studies on different ionic dendrimers7c,19 our group found that in solution the bond strength was not sufficiently high to keep the two parts together in the ionic dendrimer. There are examples where DOSY studies have been used to estimate the extent of ion-pairing interactions in salts, mainly in transition metal complexes20 and a few on dendrimers with cations of medicinal interest.21 The latter study confirms the interaction between ionic molecules but these did not diffuse with the same coefficient. In our case, the coefficients are an average between those of the dendron and free PPI, except for the generation 5 complexes which have a much lower coefficient. The relative positions of the anion and the cation were studied by NOESY experiments. It can be seen from Fig. S4† that the protons of the terminal branches dock closely with diastereotopic protons of the carboxylic acid dendron and with the methyl protons (cross-peaks are indicated in Fig. S4†). An NOE effect between functional groups and PPI was not observed.
The signals for the aromatic protons of the dendron become more shielded on increasing the PPI generation, a trend that suggests a more compact arrangement of the dendron around the dendrimer and thus a stronger bond for PPI64CzB1, which would explain its different diffusion behavior.
The downfield shift of the carboxylic carbon (Cz) signal in 13C CPMAS experiments performed on CzB1 and PPI64CzB1 provides evidence for the formation of the carboxylate anion (Fig. S5†).
Ionic hybrid dendrimer | Transition temperaturea (°C) | Ionic hybrid dendrimer | Transition temperaturea (°C) |
---|---|---|---|
a Transition data obtained by DSC corresponding to the second heating process performed at 10 °C min−1. b Optical data. c C = crystalline phase, N: nematic mesophase, SmA = smectic A mesophase, Colh = hexagonal columnar mesophase, Colr = rectangular columnar mesophase, Ng, SmAg, Colrg, Colhg: glassy phases, I = isotropic liquid. | |||
CzA1 | C 52 I | CzA2 | Ng 25 N 66 I |
PPI4CzA1 | Ng 5 N 64 I | PPI4CzA2 | Ng 4 N 55 I |
PPI8CzA1 | Ng 6 N 47 I | PPI8CzA2 | Ng 32 N 81 I |
PPI16CzA1 | Ng 8 N 72 I | PPI16CzA2 | Ng 6 N 65 I |
PPI32CzA1 | Ng 29 N 69 I | PPI32CzA2 | Colrg 5 Colr 66 I |
PPI64CzA1 | Colrg 10 Colr 62 I | PPI64CzA2 | Colhg 0 Colh 61 I |
CzB1 | C 46 I | CzB2 | C 69 I |
PPI4CzB1 | SmAg 50 SmA 95b I | PPI4CzB2 | SmAg 75 SmA 110 I |
PPI8CzB1 | SmAg 42 SmA 92 I | PPI8CzB2 | SmAg 72 SmA 115 I |
PPI16CzB1 | SmAg-11 SmA 100 | PPI16CzB2 | SmAg 42 SmA 89 I |
PPI32CzB1 | SmAg 35 SmA 124b | PPI32CzB2 | SmAg 33 SmA 90 I |
PPI64CzB1 | Colrg 37 Colr 117 I | PPI64CzB2 | Colhg 35 Colh 92 I |
Dendrimers derived from dendrons CzBm show a smectic A mesophase for PPI generations G = 1–4 and columnar phases for G = 5. The smectic A and columnar nature of the mesophases was confirmed by X-ray diffraction. Changes in the texture or DSC peaks were not observed upon cooling the samples, indicating that the mesophase freezes into a glassy state that retains the liquid crystal structure. This situation was confirmed by X-ray diffraction of this glassy state. The POM textures in the SmA phase and DSC scans of two ionic hybrid dendrimers (PPI4CzB1 and PPI32CzB1) are shown in Fig. 2 as examples. DSC scan for ionic hybrid dendrimers PPI16CzA1, PPI16B1 are shown in Fig. S6.†
For the nematic mesophases the absence of Bragg reflections helped to confirm the absence of periodic positional order. The X-ray patterns contain a diffuse maximum in the low-angle region, which is characteristic of the local correlations along the long axis of the molecules, and a broad, diffuse halo in the high-angle region, which is typical of the conformational disorder of the aliphatic chains and is related to the local lateral interferences (Fig. 3a).
Fig. 3 Room-temperature X-ray patterns of (a) dendrimer PPI8CzA1 in the N mesophase, (b) dendrimer PPI16CzB1 in the SmA mesophase. |
The lamellar positional order inherent in the smectic mesophases produced Bragg spots that were characteristic of the layer spacing. Consequently, in addition to the high-angle broad halo related to the conformational disorder and to the short-range correlations in the layer plane, the X-ray patterns of the smectic mesophases in this series contain one or more sharp reflections in the low-angle region, corresponding to the arrangement of the molecules in regularly spaced parallel layers. The presence of several low-angle maxima in the reciprocal spacing ratio 1:2:3 etc. is related to the successive reflection orders. However, the presence of a single maximum provided sufficient evidence to assign a smectic mesophase (Fig. 3b). The deduced spacings for all of the smectic mesophases are listed in Table 2.
Ionic hybrid dendrimer | Mesophasea | Temperatureb (°C) | Parameters (Å) | Φ (Å) (calculate) | S d (Å2) (calculate) |
---|---|---|---|---|---|
a SmA = smectic A mesophase. b rt = room temperature. | |||||
PPI4CzB1 | SmA | 50 | d = 42.5 | 13.8 | 75.1 |
PPI8CzB1 | SmA | 42 | d = 42.5 | 19.7 | 76.4 |
PPI16CzB1 | SmA | rt | d = 46.6 | 27 | 71.3 |
PPI32CzB1 | SmA | rt | d = 45.4 | 38.7 | 73.5 |
PPI4CzB2 | SmA | rt | d = 44.8 | 19.1 | 143.8 |
PPI8CzB2 | SmA | rt | d = 47.4 | 26.4 | 137.2 |
PPI16CzB2 | SmA | rt | d = 43.8 | 39.2 | 151.2 |
PPI32CzB2 | SmA | rt | d = 45.2 | 54.7 | 146.9 |
The data obtained are consistent with the adoption by the molecules of a cylinder-shaped conformation. In this cylinder, in a similar way to the model described for other smectic liquid crystalline dendrimers,6a,6c,7c the central region is occupied by the PPI core, with the ionic pairs pointing upwards and downwards, and the dendrons are statistically distributed at both ends (Fig. 4, top left). In fact, this model is valid for both the nematic and the smectic mesophases. However, in the nematic mesophase there is only orientational order and there is no positional periodicity, whereas in the smectic mesophase there is a regular arrangement in layers in addition to the orientational order (Fig. 4, bottom left).
Fig. 4 Proposed arrangement of the dendrimers in the nematic, smectic A and columnar mesophases. d: layer thickness, Φ: cylinder diameter; values are gathered in Table 1. |
In an effort to gain an insight into the molecular arrangement and the packing in the mesophase, calculations can be carried out on the assumption that the density of the organic molecules is close to 1 g cm−3. Assuming that the functionalization of the terminal amino groups of PPI is complete, it is possible to estimate the diameter Φ in Å of the cylindrical molecules and, from this value, the cross-section Sd in Å2 of each dendron considered perpendicular to the cylinder axis (see ESI† and Fig. 4, top left).
The structural parameters, the diameter of the cylindrical molecule (Φ) and the cross-section of each dendron (Sd) in the smectic (SmA) mesophase are listed in Table 2. These data show that the cylinder height (d, layer spacing) does not change appreciably on varying the generation of the dendrimer or of the dendron. This trend is in reasonable agreement with the results found for other smectic liquid crystalline dendrimers and is due to the predominant spreading of the dendritic branches of PPI in the plane perpendicular to the cylinder axis, a situation that arises in order to accommodate all the dendrons. Furthermore, it is observed that the surface required by the second-generation dendrons (145 Å2 on average) is approximately twice the surface required by the first-generation dendrons (74 Å2 on average), which is consistent with the proposed cylindrical arrangement. Moreover, as mentioned below, the occurrence of columnar mesomorphism for a lower generation of PPI in the case of the second-generation dendron can be accounted for by its higher space requirements, which force the dendrimers to change their conformation from cylindrical to disc-like for a lower generation.
The evolution from smectic to columnar mesomorphism is related to this conformational change. Indeed, in the case of dendron CzB1 it can be observed that the molecule diameter Φ increases with the PPI generation (Table 2) until a situation is reached where the molecule adopts the shape of a flattened cylinder, the diameter of which is almost equal to its height (PPI32CzB1). For a higher PPI generation a situation is reached in which the cylinder cross-section does not have enough space to accommodate the increasingly large number of dendrons. At this point, a dramatic conformational change takes place and the dendrons arrange themselves around the PPI core because the steric hindrance encountered in the cylindrical arrangement is relieved if the dendrons shift to a radial orientation, thus yielding a disc shape (Fig. 4, top right).
When this disc-like arrangement is achieved, the molecules stack in columns and these columns pack in a two-dimensional lattice with rectangular symmetry for PPI64CzA1, PPI64CzB1 and PPI32CzA2 (Fig. 4, bottom right). Columnar mesophases yield X-ray diffraction patterns that contain a set of sharp maxima in the low-angle region, which are characteristic of the two-dimensional packing of columns, and a broad, diffuse halo at high angles, which is typical of the conformational disorder of the aliphatic chains and is consistent with the absence of a regular stacking distance along the column axis. The measured spacing and the deduced structural parameters are given in Table 3. The rectangular symmetry of the columnar packing for these three compounds is deduced from the presence of two low-angle sharp maxima that can be assigned, respectively, to the (1 1) and (0 2) reflections of the two-dimensional rectangular lattice, from which the lattice constants a and b are obtained.
Ionic hybrid dendrimer | Mesophase | T (°C) | Parameters (Å) | d obs (Å) | d calc (Å) | h d b (Å) | h k |
---|---|---|---|---|---|---|---|
a Data obtained at 37 °C in the heating process. b Disc thickness (hd = 10 × M/(6.023 × a × (b/2)) for the Colr phase and hd = 10 × M/(6.023 × (√3/2) × a2) for the Colh phase). rt: room temperature. Colr: rectangular columnar mesophase, Colh: hexagonal columnar mesophase. | |||||||
PPI64CzA1 | Colr | rt | a = 69.3 | 42.3 | 42.3 | 51.3 | 11 |
b = 53.4 | 26.7 | 26.7 | 02 | ||||
PPI64CzB1 | Colr | 37a | a = 73 | 45.4 | 45.4 | 49.8 | 11 |
b = 58 | 28.8 | 29 | 02 | ||||
PPI32CzA2 | Colr | rt | a = 62.8 | 39.4 | 38.9 | 59.2 | 11 |
b = 50.6 | 25.3 | 25.1 | 02 | ||||
PPI64CzA2 | Colh | rt | a = 55.6 | 48.1 | 48.1 | 70.3 | 10 |
27.9 | 27.8 | 11 | |||||
PPI64CzB2 | Colh | rt | a = 55.9 | 48.8 | 48.4 | 88.1 | 10 |
27.6 | 27.9 | 11 |
When the highest PPI generation is ionically bonded to second-generation dendrons (compounds PPI64CzA2 and PPI64CzB2), the mutual balance between the distinct regions of the molecule produces a different spatial arrangement and a hexagonal symmetry is generated (Fig. 4, bottom right). The hexagonal symmetry is deduced from the presence of two low-angle sharp maxima in the reciprocal spacing ratio 1:√3, which are assigned, respectively, to the (1 0) and (1 1) reflections of the two-dimensional hexagonal lattice, from which the lattice constant a is obtained. As for the rectangular columnar mesophases in this series, only a broad, diffuse halo is observed in the high-angle region. As for the smectic mesophases, simple calculations can be carried out for the columnar mesophases in order to gain an insight into the packing in the liquid crystal phase. These calculations enable values for hd to be estimated (Table 3; see ESI†). This parameter is the mean disc thickness or, expressed otherwise, the height of column required to accommodate one molecule. Comparison of the hd values with the lattice constants gathered in Table 3 indicates that these molecules in the columnar mesophases have a considerable thickness compared to their cross-section and, therefore, their shape is more appropriately described as cylindrical than disc-like. Another significant conclusion drawn from the hd values gathered in Table 3 is related to their evolution upon changing the PPI generation. On considering dendron CzA2, the only one that is present in the two hybrid dendrimers collected in Table 3 (PPI32CzA2 and PPI64CzA2), the difference in hd on increasing the PPI generation from 4 to 5 is 11 Å. This is consistent with the data reported in the literature for similar situations and is accounted for by a preferential elongation of the PPI branches in the direction of the column axis.22
In the UV region all of the hybrid dendrimers present absorption bands at 265 nm, 295 nm and 332 nm, which are assigned to carbazole-centered transitions, π–π* transitions and n–π* transitions, respectively. The emission spectra (excitation at 295 nm) all exhibit two bands at 352 nm and 369 nm along with a shoulder at 388 nm.
The absorption spectra of dendron CzA1 and the corresponding ionic hybrid dendrimers are shown in Fig. 5. As can be observed, the molar absorbance of the peaks increases in a linear manner with the number of carbazole rings in the dendrimer (related to the generation of the dendrimer PPI, series A).
Fig. 5 Normalized UV-vis absorption spectra in CH2Cl2 solution of dendron CzA1 and the dendrimers PPInCzA1. |
Comparison of the molar absorbance value for each dendrimer at 265 nm with the value obtained for the dendron confirms the situation outlined above. The relevant data are collected in Tables S6 and S7.† On the other hand, it was observed that dendrimers PPInCzB1 show a slight deviation from linearity in this behavior. Quantum yields for the PPInCzB1 family were measured with quinine sulfate monohydrate as a standard (Φ = 0.546 in 1 N H2SO4). The values lie in the range 0.09–0.10 and the lowest quantum yield was observed for the first generation hybrid ionic dendrimer (n = 4) PPI4B1 (data are gathered in Table S8†).
The emission of the dendrimers was studied and it was found that the peak maxima are similar in both series derived from dendrons A and B [around 352, 369, 388 (sh) in solution and 355, 372, 389 (sh) in film].
The bands in the emission spectra in mesophase appear broader than the corresponding emission bands in the in solution (Fig. 6). This difference is more noticeable for dendrimers of family A, probably due to the greater ability of the dendrimers of series PPInCzAm to engage in π–π interactions between the aromatic rings of the promesogenic unit and the carbazole groups when compared to those of series B. This effect gives rise to a more marked red-shift for the compounds derived from CzAm dendrons. The absorption spectra of dendrons and ionic hybrid dendrimers PPInCzA1 and PPInCzB1 are shown in ESI (Fig. S7†).
Fig. 6 Emission spectra in CH2Cl2 solution and in the mesophase film of (a) PPI32CzA1, (b) PPI32CzB1, (c) PPI4CzA2, (d) PPI4CzB2. |
The potential was cycled between 0 and 2 V at a scan rate of 100 mV−1 against an Ag/AgCl reference electrode with a platinum auxiliary electrode and a graphite working electrode. In the first cycle of the CV scan the anodic peaks of the dendrimer are more intense than the cathodic peaks. This marked asymmetry in the redox couple indicates that these species undergo irreversible oxidation.
The dendrimers were studied in five cycles and representative CV curves are shown in Fig. 7 and S8.†
Cyclic voltammetry traces obtained using ITO as the working electrode and with the potential cycled between 0 and 2 V were also studied in order to assess whether electropolymerizaton of the samples occurred (Fig. 7).
It can be observed that the intensity of the oxidation peak increases in successive cycles but the intensity of the reduction peak increases to a lesser extent. In addition, the formation of an electrodeposited film of the ionic hybrid dendrimers takes place on the ITO working electrode. This effect was not observed with the dendrons.
All of the dendrimers are mesogenic and the mesophase type depends on the generation of dendrimer and the dendron type. Dendrimers derived from CzAm dendrons show nematic and columnar mesomorphism, whereas dendrimers derived from CzBm dendrons exhibit smectic A and columnar mesophases.
All of the systems are luminescent at room temperature in solution and in films, and the intensity of the emission and absorption depends on the number of carbazole units in the dendrimer.
All compounds have electrochemical properties due to presence of carbazole rings, but it was observed that the oxidation behaviour does not depend on the dendrimer generation.
Footnote |
† Electronic supplementary information (ESI) available: Text giving more details about the employed techniques including reaction schemes and structures, optical studies, synthesis and characterization of the materials, and DSC data, figures showing the compound structure, NMR and IR spectra, and DSC curves, and optical data. See DOI: 10.1039/c5ra12237f |
This journal is © The Royal Society of Chemistry 2015 |