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Synthesis and Studies of Dendritic Poly(Ether Imine) Boronates and Cholesteryl-Functionalized Mesogens SYNOPSIS Dendrimers are hyperbranched synthetic macromolecules having branches-upon-branches structures, high molecular weights, globular shapes and monodispersities. Dendrimers possess a large number of modifiable functional groups at their peripheries. Initial efforts were largely concerned with the synthesis, design and development of new dendrimers. Exploring the chemical, biological and material applicability of these macromolecules are relevant to current interests, as a result of the unique structural features of dendrimers. Incorporation of transition metals and organic moieties at the peripheries of the dendrimers was studied to determine their efficacies in catalysis. Evolution of dendritic effects was observed in few instances, that were non-linear in nature. On the other hand, dendritic peripheries were also utilized to study mesogenic properties in liquid crystals. Chapter 1 of the Thesis gives an overview of the types of dendrimers, its structural features and their application in catalysis and as liquid crystalline materials. Chapter 2 describes the synthesis of a new type of poly(ethyl ether imine) dendrimer, having nitrogen as a branching unit, ethylene moiety as the spacer and an oxygen as the connecting linker. Synthesis, characterization, and studies of the photophysical properties of these dendrimers are described in this chapter. The molecular structure of second generation dendrimer is shown in Figure 1. Synthesis of this dendrimer was initiated using 2,2'-oxy-bis(ethan-1¬amine) as the core. The reaction sequence of two alternate nucleophilic substitutions and two alternate reductions, involving ethyl bromoacetate and bromoacetonitrile as monomers was employed in the synthesis of the dendrimer. The formation of dendrimers having ether linkage and tertiary amines as branching unit was established by spectroscopies and mass spectrometry. A number of functional groups, such as, acid, alcohol, amine, ester and nitrile are present at the peripheries of each generation the dendrimers that open up the possibilities for further studies. Carboxylic acid terminated poly(ethyl ether imine) dendrimers are substituted iminodiacetic acids, belonging to the class of polyaminocarboxylic acid. Methyl iminodiacetic acid boronates with NB coordination have emerged as an excellent substitute for unstable boronic acids. Upon increasing the steric bulk on the nitrogen moiety, the hydrolytic stability of the boronates to a base-catalyzed hydrolysis is increased. Combining the structure of carboxylic acid terminated dendrimer and the stability of the dendritic boronates, such dendritic iminodiacetic acids were reacted with arylboronic acids to prepare bis-and tetrakis-boronates (Figure 2). Kinetic hydrolytic studies of boronates were conducted to assess the stabilities of the newly synthesized dendritic boronates. From the studies it was observed that the tetrakis-boronate was ~20 times more stable in comparison with dimeric and monomeric boronates (Figure 3). Subsequent to synthesis and hydrolytic stability studies, C-C bond-forming Suzuki-Miyaura cross-coupling reactions were conducted. A comparison of the reactivities among monomeric, dimeric and tetrameric arylboronates in C-C bond-forming reactions showed a higher reactivity of monomeric and dimeric boronates, than the tetrameric aryl boronate to construct ter-and tetra-aryl in one-pot iterative manner (Figure 4). Chapter 3 of this Thesis describes the synthesis and characterization of dendritic boronates and studies of their hydrolytic stability in Suzuki-Miyaura cross¬coupling reactions to construct ter-and tetraaryls. Figure 4. Synthesis of (a) ter-(6) and (b) tetra-aryls (7) by following one-pot iterative cross-coupling reactions. Step-wise iterative synthesis of dendrimer allows a uniform branching throughout the structure. The first and second generation poly(ether imine) dendrimer series, having hydroxyl groups at their peripheries were chosen for further modification. A versatile mesogenic group, namely, cholesterol was covalently attached at the peripheries of the dendrimers with succinic moiety as linker, so as to install 4 and 8 cholesteryl moieties at the peripheries of the dendrimers (Figure 5), that were characterized by H, C NMR spectroscopies and elemental analysis, so as to confirm their structural homogeneities. Figure 5. Molecular structures of the first and second generation dendritic mesogens. Subsequent to synthesis and characterization, liquid crystalline properties of all the dendritic mesogens was assessed through differential scanning calorimetry (DSC), polarizing optical microscopy (POM) and X-ray diffraction (XRD) studies. In POM study, broken fan or leaf like texture revealed the lamellar arrangement, whereas homeotropic appearance of texture on surfactant (cetyltrimethylammonium bromide) coated substrate indicated the lamellar nature of G1-Et-(OCS)4, G1-Pr-(OCS)4 and G2-Pr-(OCS)8 (Figure 6). From DSC studies, the change in enthalpy was found to increase with increase in generation and change in enthalpy per mesogenic unit was found to be ~ -1 1-2 kJ mol, which indicated the mesophase arrangement to be lamellar. Decrease in the length of spacer dendritic backbone and increase in the generation increased the isotropization temperature of the dendritic liquid crystals. Variable temperature XRD studies were undertaken to characterize the mesophase property. Two sharp peaks in small angle region and a diffused halo in wide angle region in XRD pattern of the material suggested the smectic A (SmA) liquid crystalline arrangement of G1-Et-(OCS)4, G1-Pr-(OCS)4 and G2-Pr-(OCS)8 (Figure 7). Figure 6. POM textures of (a) G1-Et-(OCS)4 at 136 oC; (b) G2-Et-(OCS)8 at 129 oC; (c) G1-Pr-(OCS)4 at 92 oC; (d) G2-Pr-(OCS)8 at 118 oC and (e) transition temperatures for dendromesogens (DSC second heating cycle, heating-cooling rate = 10 oC min-1). Figure 7. Small angle XRD profiles of: (a) G1-Pr-(OCS)4 and (b) G2-Et-(OCS)8 at 60 o C (black), 150 oC (red) and 180 oC (green), (Insets: Lorentzean fit of wide angle peak). The second generation ethyl-linker dendrimer G2-Et-(OCS)8 exhibited a layered structure with a superimposed in-plane modulation (SmÃ), the length of which corresponded to a rectangular column width. Chapter 4 describes the synthesis, characterization and studies of mesophase property and fluorescence property of cholesterol functionalized homologous pairs of the PETIM dendritic liquid crystals. Peripheral functionalization of the dendrimers provides an easy access to dendritic liquid crystalline materials. The covalent functionalization was extended further with the dendrimers for both the series, so as to have 2, 4, 8 and 16 cholesteryl groups at the peripheries of 0, 1, 2 and 3 generation dendrimers, respectively, having succinic amide and phthalic ester functionalities for 1, 2 and 3 generation dendrimers with 4, 8 and 16 cholesteryl groups. Molecular structures of third generation dendrimers are shown in Figure 8. Figure 8. Molecular structures of third generation G3-Pr-(NHCS)16 and G3-Pr-(OCP)16. Subsequent to synthesis and characterization, mesophase property was studied through POM, DSC and XRD techniques. In POM study, a birefringent texture was observed in heating and cooling cycles. Leaflet, broken fan or bâtonnet like texture suggested the layered arrangement of the molecules (Figure 9). In DSC studiues, it was observed that the amide-linked dendrimers showed higher glass transition and isotropization temperatures than that of ester-linked dendrimers within the same generation irrespective of the back-bone of the dendrimer. Succinic moiety linked dendrimers showed lower glass transition temperature than that of phthalic moiety linked dendrimers and consequently, larger mesophase range. The change in enthalpy for isotropization was found to increase with increase in generation, whereas change in -1 enthalpy per mesogenic unit was 1-2 kJ mol, indicative of a layered arrangement in the mesophase. Figure 9. POM textures (20x) of (a) G3-Pr-(NHCS)16 at 90 oC; (b) G3-Pr-(OCS)16 at 90 ooo C; (c) PG1-(NHCS)4 at 134 C; (d) G3-Pr-(OCP)16 at 98 C and (e) transition temperatures for dendromesogens (second cycle, heating-cooling rate = 10 oC min-1). Appearance of two sharp peaks in small angle region and a wide halo in wide angle region in XRD pattern supported lamellar mesophase property of the material (Figure 10). On decreasing the temperature, increase in the layer thickness also suggested the smectic A arrangement of the molecules except third generation phthalate derivative G3-Pr-(OCP)16, which showed rectangular columnar mesophase. For all the dendromesogens, the layer thickness increased with the increase in generation. Upon protonation, the first generation dendrimer showed a change in mesophase from simple smectic A to modulated smectic A with decrease in layer thickness. The change in liquid crystal property of the dendromesogens from lamellar to columnar mesophase by changing the linker of the mesogen is unknown so far in the dendrimer liquid crystals. Chapter 5 gives details of synthesis, characterization and mesophase property study of ester-and amide-linked dendritic liquid crystals. Overall, the Thesis establishes a synthetic methodology for the synthesis of a new homologous series of poly(ether imine) dendrimers with ethyl spacer; synthesis of dendritic boronates and their studies in cross-coupling reactions through in-situ slow release of boronic acid; hydrolytic stability study showed higher stability of dendritic boronates which was used in one-pot iterative cross-coupling reactions to construct ter-and tetra-aryls. decrease in linker length in dendrimer backbone modified the thermal, as well as, mesophase behavior of the dendritic liquid crystals; change in the linker functionality from ester to amide changed the thermal behavior of dendritic liquid crystals; a switching of mesophase property from lamellar to columnar was observed by changing the rigidity of the linker from succinate to phthalate without changing the linker length. The results of the above chapters are in different stages of publications: 1 Dendritic iminodiacetic acids and their boronates in Suzuki-Miyaura cross¬coupling reactions. Sharma, A.; Kumar, P.; Pal, R.; Jayaraman, N. Revised Manuscript submitted. 2 In-plane modulated smectic à vs smectic A lamellar structures in homologous pairs of dendritic liquid crystals. Kumar, P.; Rao, D. S. S.; Prasad, S. K.; Jayaraman, N. Revised Manuscript submitted. 3 Effect of protonation on dendritic liquid crystals of poly(ether imine) dendrimers: structure property relationship studies. Kumar, P.; Rao, D. S. S.; Prasad, S. K.; Jayaraman, N. Manuscript submitted. 4 Smectic to rectangular columnar switch from succinic to phthalic linker alteration in poly(ether imine) dendritic liquid crystals. Kumar, P.; Rao, D. S. S.; Prasad, S. K.; Jayaraman, N. Manuscript in preparation.

In many studies of the side-chain liquid crystalline polymers (SCLCPs) bearing azobenzene mesogens as pendant groups, obtaining the orientation of azobenzene mesogens at a macroscopic scale as well as its control is important, because it impacts many properties related to the cooperative motion characteristic of liquid crystals and the trans-cis photoisomerization of the azobenzene molecules. Various means can be used to align the mesogens in the polymers, including rubbed surface, mechanical stretching or shearing, and electric or magnetic field. In the case of azobenzene-containing SCLCPs, another method consists in using linearly polarized light (LPL) to induce orientation of azobenzene mesogens perpendicular to the polarization direction of the excitation light, and such photoinduced orientation has been the subject of numerous studies. In the first study realized in this thesis (Chapter 1), we carried out the first systematic investigation on the interplay of the mechanically and optically induced orientation of azobenzene mesogens as well as the effect of thermal annealing in a SCLCP and a diblock copolymer comprising two SCLCPs bearing azobenzene and biphenyl mesogens, respectively. Using a supporting-film approach previously developed by our group, a given polymer film can be first stretched in either the nematic or smectic phase to yield orientation of azobenzene mesogens either parallel or perpendicular to the strain direction, then exposed to unpolarized UV light to erase the mechanically induced orientation upon the trans–cis isomerization, followed by linearly polarized visible light for photoinduced reorientation as a result of the cis–trans backisomerization, and finally heated to different LC phases for thermal annealing. Using infrared dichroism to monitor the change in orientation degree, the results of this study have unveiled complex and different orientational behavior and coupling effects for the homopolymer of poly{6-[4-(4-methoxyphenylazo)phenoxy]hexyl methacrylate} (PAzMA) and the diblock copolymer of PAzMA-block- poly{6-[4-(4-cyanophenyl) phenoxy]hexyl methacrylate} (PAzMA-PBiPh). Most notably for the homopolymer, the stretching-induced orientation exerts no memory effect on the photoinduced reorientation, the direction of which is determined by the polarization of the visible light regardless of the mechanically induced orientation direction in the stretched film. Moreover, subsequent thermal annealing in the nematic phase leads to parallel orientation independently of the initial mechanically or photoinduced orientation direction. By contrast, the diblock copolymer displays a strong orientation memory effect. Regardless of the condition used, either for photoinduced reorientation or thermal annealing in the liquid crystalline phase, only the initial stretching-induced perpendicular orientation of azobenzene mesogens can be recovered. The reported findings provide new insight into the different orientation mechanisms, and help understand the important issue of orientation induction and control in azobenzene-containing SCLCPs. The second study presented in this thesis (Chapter 2) deals with supramolecular side-chain liquid crystalline polymers (S-SCLCPs), in which side-group mesogens are linked to the chain backbone through non-covalent interactions such as hydrogen bonding. Little is known about the mechanically induced orientation of mesogens in S-SCLCPs. In contrast to covalent SCLCPs, free-standing, solution-cast thin films of a S-SCLCP, built up with 4-(4’-heptylphenyl) azophenol (7PAP) H-bonded to poly(4-vinyl pyridine) (P4VP), display excellent stretchability. Taking advantage of this finding, we investigated the stretching-induced orientation and the viscoelastic behavior of this S-SCLCP, and the results revealed major differences between supramolecular and covalent SCLCPs. For covalent SCLCPs, the strong coupling between chain backbone and side-group mesogens means that the two constituents can mutually influence each other; the lack of chain entanglements is a manifestation of this coupling effect, which accounts for the difficulty in obtaining freestanding and mechanically stretchable films. Upon elongation of a covalent SCLCP film cast on a supporting film, the mechanical force acts on the coupled polymer backbone and mesogenic side groups, and the latter orients cooperatively and efficiently (high orientation degree), which, in turn, imposes an anisotropic conformation of the chain backbone (low orientation degree). In the case of the S-SCLCP of P4VP-7PAP, the coupling between the side-group mesogens and the chain backbone is much weakened owing to the dynamic dissociation/association of the H-bonds linking the two constituents. The consequence of this decoupling is readily observable from the viscoelastic behavior. The average molecular weight between entanglements is basically unchanged in both the smectic and isotropic phase, and is similar to non-liquid crystalline samples. As a result, the S-SCLCP can easily form freestanding and stretchable films. Furthermore, the stretching induced orientation behavior of P4VP-7PAP is totally different. Stretching in the smectic phase results in a very low degree of orientation of the side-group mesogens even at a large strain (500%), while the orientation of the main chain backbone develops steadily with increasing the strain, much the same way as amorphous polymers. The results imply that upon stretching, the mechanical force is mostly coupled to the polymer backbone and leads to its orientation, while the main chain orientation exerts little effect on orienting the H-bonded mesogenic side groups. This surprising finding is explained by the likelihood that during stretching in the smectic phase (at relatively higher temperatures) the dynamic dissociation of the H-bonds allow the side-group mesogens to be decoupled from the chain backbone and relax quickly. In the third project (Chapter 3), we investigated the shape memory properties of a S-SCLCP prepared by tethering two azobenzene mesogens, namely, 7PAP and 4-(4'-ethoxyphenyl) azophenol (2OPAP), to P4VP through H-bonding. The results revealed that, despite the dynamic nature of the linking H-bonds, the supramolecular SCLCP behaves similarly to covalent SCLCP by exhibiting a two-stage thermally triggered shape recovery process governed by both the glass transition and the LC-isotropic phase transition. The ability for the supramolecular SCLCP to store part of the strain energy above T[subscript g] in the LC phase enables the triple-shape memory property. Moreover, thanks to the azobenzene mesogens used, which can undergo trans-cis photoisomerization, exposure the supramolecular SCLCP to UV light can also trigger the shape recovery process, thus enabling the remote activation and the spatiotemporal control of the shape memory. By measuring the generated contractile force and its removal upon turning on and off the UV light, respectively, on an elongated film under constant strain, it seems that the optically triggered shape recovery stems from a combination of a photothermal effect and an effect of photoplasticization or of an order-disorder phase transition resulting from the trans-cis photoisomerization of azobenzene mesogens.

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Grace à leurs propriétés d’auto-réparation et d’auto-organisation, les matériaux pi-conjugués liquide-cristallins (LCs) présentent un grand intérêt pour l’élaboration de matériaux semi-conducteurs à hautes performances. Ils peuvent être utilisés pour différents types d’applications en électronique organique telles que les cellules solaires (OPV), les diodes électroluminescentes (OLED) et les transistors à effet de champs (OFET). Dans ce travail, nous avons conçu et préparé une nouvelle famille de LCs combinant des entités pi-conjuguées de type calamitique et discotique au sein d’une architecture moléculaire unique. Plus particulièrement, nous avons imaginé trois différentes architectures telles que des dyades et triades linéaires et des triades ramifiées, incluant des dérivés discotiques de pérylène ou de triphénylène et des dérivés calamitiques de terthiophène, de benzothienobenzothiophène ou encore de pyromellitique. L’objectif était d’étudier leurs comportements liquide-cristallins et leurs propriétés d’auto-organisation et de transport de charges.Les résultats obtenus ont montré que ces matériaux donnent des auto-assemblages complexes formant des arrangements multi-lamellaires de bicouches, dans lesquelles les entités calamitiques et discotiques présentent une organisation dans le plan. De plus, en choisissant judicieusement les entités pi-conjuguées calamitiques et discotiques (type-p ou type-n), nous avons démontré que ce type de matériaux auto-organisés peut présenter des propriétés de transport de charge ambipolaire en formant des chemins distincts pour chaque type de charge (trou et électron) par nano-ségrégation de ces entités de type p et de type n. / Due to their self-healing ability and their self-organization property, pi-conjugated liquid crystals (LCs) are materials of great interest to prepare high performance semiconducting materials. They can be used in different types of organic electronic applications such as solar cells (OPV), Organic Light-Emitting Diodes (OLED) and Organic Field-Effect Transistors (OFET). In this work, we were interested in designing and preparing a novel family of LCs combining π-conjugated discotic and calamitic moieties in a unique molecular architecture. More particularly, we designed three different molecular architectures based on a linear dyad, triad and a branched triad, which include discotic triphenylene or perylene and calamitic terthiophene, benzothienobenzothiophene or pyromellitic moieties. The objective was to study their liquid crystalline behaviors and their self-organization and charge transport properties.Based on our results, we demonstrated that these materials can form complex self-assemblies in the bulk such as multi-lamellar arrangements presenting bilayered lamellar phases with in-layer organization of both calamitic and discotic species. In addition, based on the appropriate choice of the disk- and rod-like π-conjugated cores (p-type or n-type), we showed that this kind of self-organized materials could exhibit ambipolar charge transport properties, presenting a spontaneous nanosegregation of p-type and n-type entities in bulk, and leading to well-defined distinct conductive channels for each type of charge carriers (hole and electron).

The work presented in this thesis has two parts. The first part deals with methodological developments in the area of solid-state NMR, relevant to the study of partially ordered systems. Liquid crystals are best examples of such partially ordered systems and they are easily oriented by the magnetic field used for the NMR study. They provide spectra rich in information useful for the study of structure and dynamic s of the oriented molecule. Dipolar couplings and anisotropic chemical shifts are relatively easy to obtain for these systems. However, the methodologies used for extracting the required information are constantly undergoing change, with newer ideas being used for optimal use of the technique and increasing the sensitivity of the methodology. In this thesis, existing methods used for obtaining dipolar couplings from oriented liquid crystalline samples are examined in detail and conditions for optimal use of the methods are investigated. Different approaches for enhancing the sensitivity of the techniques are also proposed. Estimation of chemical shift anisotropy of carbons for a molecule that is used as a building block for several mesogens has been obtained and its utility for estimating the order parameters of the system have been examined. The second part of the thesis deals with the application of solid state NMR methods to the study of a number of novel liquid crystalline systems and for the estimation of dynamics, order and orientation of the mesogenic molecules in the magnetic field. Chapter-2 deals with a detailed and systematic study to improve the sensitivity of cross-polarization based separated local field (SLF) NMR spectroscopy techniques such as PISEMA(Polarization Inversion Spin Exchange at the Magic Angle) and PDLF(Pro-ton Detected Local Field). The chapter has been further divided into three sections. Section-A describes the optimization procedure for cross-polarization period for reducing zero-frequency peaks in SLF experiments. Polarization Inversion(PI) is one of the important components of PISEMA and plays a crucial role in enhancing the dipolar cross-peaks and suppressing the axial-peaks. Shortening this period has the advantage of less r.f. power input into the system, thus less susceptibility to sample heating. Therefore it is crucial to arrive at the optimum condition for which maximum sensitivity and resolution are obtained. A detailed experimental investigation of the role of the initial po1arization period has been carried out for two different samples of static oriented liquid crystalline material at two different temperatures and a contact time of 2ms has been found to be optimal for such samples. Insection-B of this chapter, the initial preparation period of the experiment is considered as a possible means of increasing the sensitivity of the experiment. Thus the use of cross-polarization via the dipolar bath by the use of a diabatic demagnetization in the rotating frame(ADRF-CP) has been proposed to be incorporated into PISEMA. To understand the CP dynamics, magnetization in double-and zero-quantum reservoirs of an ensemble of spin-1/2 nuclei and their role in determining the sensitivity the experiments have been theoretically examined. Experimentally, a modification incorporating ADRF-CP is shown to result in enhancement of signal-to-noise by as much as 90% in the case of rigid single crystals of a model peptide and up to 50% in non-rigid, partially ordered liquid crystalline systems. In section-C another useful SLF technique known as PDLF spectroscopy has also been examined. In this case a sweep of one of the r.f. amplitudes(RAMP-CP),rather than ADRF is found to work well. The reason for the different behaviours has been discussed. Chapter-3 highlights two experimental approaches used to extract the chemical shift anisotropy(CSA) tensor information from rotating solids. Section-A is devoted to the measurement of the CSA values of thiophene by using MAS side band analysis, by extracting the principal values from the intensities of just a few spinning side bands. Experiments have been performed on thiophene-2 carboxylic acid and thiophene-3 carboxylic acid samples and the carbon CSA values have been obtained. In section-B, CSA values of carbons of the core unit of the liquid crystal4- hexyloxybenzoic acid (HBA) have been obtained by using the recoupling pulse sequence SUPER(Separation of Undistorted Powder patterns by Effortless Recoupling).HBA belongs to an important class of thermotropic liquid crystals which are structurally simple and often used as starting materials for many novel mesogens. As this molecule could serve as an ideal model compound, high resolution13C NMR studies of HBA in solution, solid and liquid crystalline phases have been also undertaken. The CSA values obtained from the 2D SUPER experiment showed good agreement to those computed by DFT calculations. The CSA values were used for obtaining the order parameter of the system at different temperatures. These matched well the order parameter obtained from the 13C-1 H dipolar couplings in the nematic phase determined by SLF spectroscopy at various temperatures. A knowledge of the CSA of the carbons is thus very useful, as they can be used for gaining knowledge about the system from the chemical shifts obtained from a simple 1D spectrum. In chapter-4, 1-and 2-dimensional13CNMR techniques have been utilized to obtain extensive information about some novel mesogenic molecules. Four molecules of different structure and topology have been taken up for study. These molecules have the following features. Mesogen-1 has a terminal hydroxyl group. Such systems with further modification can result in mesogenic monomers for side chain liquid crystalline polymers. Mesogen-2 has a dimethyl amino group at one end and has three phenyl groups connected by appropriate linking units that form the core. In the third case, mesogen-3, the terminal hydroxyl group of mesogen-1 is replaced with a hydrogen such that13C-1 H dipolar couplings provide directly information on molecular ordering and orientation. In the fourth case, mesogen-4, the core is built with four phenyl rings. Here the fourth ring is linked to other three rings via a flexible chain unit. In each of these cases the 2DSLFNMR experiments have been carried out where13C-1 H dipolar couplings as well as13C chemical shifts were used for obtaining the order parameters of various segments of the molecule. The data provide useful insight into the phase behaviour, ordering and orientation of the molecules. Chapter-5 discusses the applications of the natural abundance 13CNMR techniques to thiophene based mesogens, that have the potential for use in molecular electronics material. Typically, these molecules consist of phenyl rings appropriately connected by linking units with thiophene. Different core units as well as different linking units to thiophene have been considered. The six mesogens thus obtained have been investigated in detail using 1D and 2D NMR methods.13C-1 H dipolar couplings have been used to obtain ordering information, that show interesting correlation to the molecular orientation and dynamics.