Statistical physics in soft matter systems, physical properties of bio-inspired systems and the mechanical manipulations of nano-systems have been studied using optical tweezers to form the basis of this doctoral Thesis. The first two chapters are on a general introduction about optical tweezers and detailed description of the setup used along with its calibrations. The next three chapters describe studies of statistical properties in soft matter systems, namely, out-of-equilibrium microrheology in a worm-like micellar system, irreversibility to reversibility crossover in the non-equilibrium trajectories of an optically trapped particle with the verification of fluctuation theorems even for non-ergodic descriptions of the system and high velocity Brownian vortexes at the liquid-air interface. The mechanical manipulation of the nano-systems, i.e. optically driven nano-rotors and the trapping, as well as transportation of palladium decorated single wall carbon nanotubes using optical tweezers have been discussed in the next two chapters. In the next chapter, the study of physical property of a bio-inspired system -the cell membrane deformability of human erythrocytes with increasing calcium ion concentration has been described. This Thesis is an endeavor to understand different mesoscopic systems using optical trapping and manipulation. Chapter 1 gives an introduction on optical tweezers. The working principle of optical trapping and manipulation are discussed along with their applicability in different fields of physics. Chapter 2 discusses the experimental setup in detail. The setup used for the experiments is a dual optical trap around an inverted microscope. The formation of the traps, the technique to steer the trapping beams and to place the traps at the desired positions in 3D without affecting the symmetry or stiffness are described. Instantaneous position tracking of the trapped particle is a very crucial part of optical trapping experiments. A tracking beam is used for this purpose and the trapped bead is imaged on a quadrant photo diode which provides the current signals that corresponds to the particle’s position in the focal plane. Then the calibration of the setup using various calibration methods are explained. Calibration of the setup includes the calibration of the position sensing devices, e.g. the quadrant photo diode and the CCD camera attached to the microscope, calibration of the electronic devices, e.g. the stage nano-positioner, nano-tilt mirror mount etc., and finally calibration of the trap stiffnesses (in both X and Y ) at varying laser powers. Precautions taken during the experiments to minimize the artifacts are also mentioned. In Chapter 3, a nonlinear microrheology experiment to probe directional viscoelasticity of a sheared worm-like micellar system has been described. Many wormlike micellar systems exhibit appreciable shear thinning due to shear induced alignment. As the micelles get aligned, introducing directionality in the system, the viscoelastic properties no longer remain isotropic. An optical tweezers based technique enables us to probe the out-of-equilibrium rheological properties of CTAT (cetyltrimethylammonium tosylate, cationic surfactant) system simultaneously along two orthogonal directions -parallel to the applied shear, as well as perpendicular to it. A trapped bead is dragged through the medium (1 wt% CTAT) and the position fluctuations of the bead, along the direction of motion (X) and perpendicular to it (Y ), are recorded in both ‘drive on’ and ‘drive off’ states. While the displacement of the bead along X -in response to the active drag force -carry signature of conventional shear thinning, its spontaneous position fluctuations along Y , following the fluctuation dissipation theorem, provide the loss modulus (G∗∗ along Y ) which manifests a dramatic orthogonal shear thickening, an effect hitherto unobserved. Chapter 4 describes an irreversibility to reversibility crossover in the transient response of a particle in optical trap; and the verification of the fluctuation theorem for a non-ergodic description of this system. The transient position fluctuations of a colloidal bead is studied as it approaches equilibrium after being released from varying heights (by using an additional very strong optical trap) in the potential energy landscape created by a weak optical trap. The time evolution of the system shows dramatic changes as the release point energy is decreased. Starting from a small-time-reversible to long-time-irreversible transition for a higher energy release, a time independent completely reversible state could be reached just by lowering the initial potential energy a bit. For an even lower energy release, the system shows an anomalous irreversibility. In this state, it progressively extracts useful work from the thermal fluctuations and surprisingly goes to a higher energy phase point. Highlighting the competition between the micro-reversibility and the irreversible dissipative loss in determining the long-time system behavior, this study exhibits the prominent emergence of a completely reversible state even at long time, in between the two irreversible states of opposite kind. The Transient Fluctuation Theorem (TFT) and the Integrated Transient Fluctuation Theorem (ITFT) which are defined to be valid only for ergodic systems, have been verified even for non-ergodic descriptions (separately for different release points) of this system. Chapter 5 illustrates the study of high velocity Brownian vortex at the liquid-air interface. A general kind of Brownian vortexes are constituted by applying an external non-conservative force field to a colloidal particle bound by a conservative optical trapping force at a liquid-air interface. As the liquid medium is translated at a constant velocity with the bead trapped at the interface, the drag force near the surface provide enough rotational component to bias the particle’s thermal fluctuations in a circulatory motion. The frequency of that circular motion increases linearly with the stage velocity, while an increment in the trapping laser power shows the opposite effect. The properties of these Brownian vortexes have been studied extensively to demonstrate how the thermal fluctuations and the advection of the bead play their role in the vortex motions, with an inference that the angular velocity of the circulatory motions offer a comparative measure of the interface fluctuations. In Chapter 6 the optical manipulation of asymmetric nanorods that constitutes optically driven nanorotors are described. The light force, irrespective of its polarization, is used to run a simple nanorotor. While the gradient force of a single beam optical trap holds an asymmetric nanorod, the scattering force is utilized to generate a non-zero torque on the nanorod making it rotate about the optic axis. The inherent textural irregularities or morphological asymmetries of the nanorods give birth to chirality which is responsible for generation of the torque under the radiation pressure. A farther study on nanorotors that are more transparent to infra-red (trapping beam) confirms that the scattering force is indeed the origin of the torque. A model is proposed to explain the rotational motion of the nanorods and estimate the speed of rotation. If the nanorods are not fairly transparent to the laser beam, even a small surface irregularity with non-zero chirality is sufficient to produce enough torque for moderate rotational speed. Different sized rotors can be used to set the speed of rotation over a wide range, with fine tuning possible through the variation of the laser power. Chapter 7 discuses optical trapping and transportation of palladium decorated single wall carbon nanotubes (Pd-SWNT). Individual carbon nanotubes being substantially smaller than the wavelength of light are not much responsive to optical manipulation. Decorating those single-walled carbon nanotubes with palladium particles changes that scenario dramatically, making the optical trapping and manipulation much easier. Palladium decorated nanotubes (Pd/SWNTs) have higher effective dielectric constant and are trapped at much lower laser power level with greater ease. In addition to that, an asymmetric line trap makes it possible to transport the Pd decorated SWNTs to a desired distant location in the sample cell. In the asymmetric line trap the Pd/SWNTs are first get attracted by the gradient force and then the scattering force push them away towards the other end of the line trap. In Chapter 8, how the rotational motion of crenated erythrocytes in an optical trap can be used to probe their membrane deformability is explained. When placed in a hypertonic buffer medium, discocytic human erythrocytes are subjected to crenation and take deformed shapes. The deformation of the cells brings in chirality and asymmetries in shape that make them rotate under the scattering force of a linearly polarized optical trap. A change in the deformability of the erythrocytes, due to any internal or environmental factor, is reflected in the rotational speed of the trapped crenated cells. Therefore the average rotational speed and the probability of rotation of the crenated erythrocytes in an optical trap can be considered as a direct signature of their membrane deformability. As an example, the relative increment in erythrocyte membrane rigidity with adsorption of Ca++ ions is examined quantitatively through this approach. The Thesis concludes with a summary of the main results and a brief discussion of the scope of future work in Chapter 9.

Over the last few decades, a vast research is going on, to study the optical properties of the nano particles i.e., metal and semiconductors thoroughly. Till date most of the optical studies are based on single particle measurement of a quantum dot (QD) or a chromophore under the influence of an external plasmonic field stimulus. In this the-sis, we tried to address the energy transfer at non local level on a layer of compact, monolayer QD assemblies over micro meter range. The energy transfer occurs in the presence of external field of metal particles or nanorods leads to the enhancement or quenching the emission from a layer of QDs. Chapter 1 is introduction to the basic theoretical aspects of excitons in semiconductor (QDs) and its optical properties under strong confinement regime. The discussion is followed with the optical properties of gold nanoparticles and rods, describing size and shape dependent variation of absorption properties, based on Mie and Mie-Gans theory. Theoretical background of collective effects in QD assemblies based on exciton-plasmonic interactions at single particle level as well as polarization based plasmo-nenhanced fluorescence has been subjected. Experimental techniques are explained in chapter 2 which contains the details of the synthesis of polymer capped nanoparticles with the respective characterization. A discussion on the synthesis methods for cadmium selenide QDs, gold nano particles and the rods with different polymer cap-ping legends and the related capping exchange methods. The thin film preparation of QD monolayers as well as hybrid nano assemblies using several techniques, i.e., Langmuir-Blodgett (LB), dip coat methods are provided. Further the details of surface morphology of the prepared thin films has been studied by different microscopic techniques i.e., atomic force microscopy (AFM), transmission electron microscopy (TEM) and scanning electron microscopy (SEM). The details of the PL emission measurements of these hybrid arrays using confocal, Raman and polarization based near field scanning optical microscope (NSOM) modes followed with the life time measurements. In third chapter, the substantial strong coupling and collective emission regime is engineered in the QD monolayer films embedded with tiny gold nano particles keeping the QD density same. Tuning the photoluminescence (PL) of semiconducting QD assemblies using small Au NPs in different ratio, different packing density and extent of spectral overlap between QD photoluminescence and the metal nanoparticle absorbance has been discussed. We provided possible experimental and theoretical evidence for the plasmon-mediated emergence of collective emission and enhanced quantum efficiency in these QD films with the consolidation of multiple emitters and multiple NPs. The quantum efficiency of these hybrid assemblies is further explored with different material as well as the size effect of metal nano particles. Chapter 4 comprises the experiment results of the self-assembled compact and partially aligned gold nano rod (GNR) arrays on QD monolayer films. We experimentally demonstrated the quantum efficiency of these QD hybrid assemblies is gaining max-imum when the longitudinal surface plasmon resonance (LSPR) absorption maxima of GNR arrays is resonant with the QD monolayer PL maxima and is always non-existent for the off resonant case. Further, we reported the variability in the size and morphology of these GNR domains leads to the maximum achieved enhancement as well as anisotropy value in comparison with isolated rods and the explored conditions to further enhance the efficiency in these QD hybrid assemblies.

This doctoral thesis deals with synthesis and characterisation of electroactive electrode materials for li-ion batteries and accumulators. The work is divided into two main parts. One deals with LiFePO4 based cathode composite electroactive material and in the second is described the synthesis and utilization of monoclinic TiO2(B) as an anode for li-ion cell. The main aim of the work is to relate the synthesis procedure and structural properties of both materials to its electrochemical preformance.

During recent decades metallic nanoparticles have been found very interesting due to their unique characteristics which make them suitable for different applications. In this research, for the very first time, we tried to perform selective surface photo activation chemistry on the targeted facets of nanoparticles while they are in suspension. This technique enabled us to form desired assemblies of nanoparticles. We focused on elongated shaped gold nanorod due to its unique surface plasmon resonance and probable biomedical applications. In this research we formed a dumbbell shape assembly of nanoparticles in suspension. A probable application for these assemblies can be in vivo imaging. Initially, we reproduced gold nanorods using existing techniques in prior papers and optimized them according to our research needs. A low rpm centrifugal separation technique was developed to efficiently separate synthesized gold nanorods from other shapes. Several characterization techniques were utilized to characterize nanoparticles at each step including UV-absorbance, zeta potential, and dynamic light scattering. Different generations of oligomers were synthesized to be used as gold nanorods coating, and each coating was tested and characterized using appropriate techniques. Our two-step coating replacement method using one of these photocleavable oligomers enabled us to achieve, for the very first time, selective UV photo activation of gold nanorod tips. The photo activated tips were then exposed to oppositely charged gold nanospheres to form dumbbell shape assemblies of gold nanorods and nanospheres. Furthermore, dumbbell shape assembly of nanoparticles was investigated and characterized. / Master of Science

Dichte Ensembles aus GaN-Nanodrähten können in der Molekularstrahlepitaxie mithilfe eines selbstinduzierten Prozesses sowohl auf kristallinen als auch amorphen Substraten gezüchtet werden. Aufgrund der Natur selbstgesteuerter Prozesse ist dabei die Kontrolle über viele wichtige Ensembleparameter jedoch eingeschränkt. Die Arbeit adressiert genau diese Einschränkungen bei der Kristallzucht selbstinduzierter GaN-Nanodrähte. Konkret sind das Limitierungen bezüglich der Nanodraht-Durchmesser, die Nanodraht-Anzahl-/Flächendichte, der Koaleszenzgrad sowie die maximal realisierbare Wachstumstemperatur. Für jede dieser Einschränkungen werden Lösungen präsentiert, um die jeweilige Limitierung zu umgehen oder zu verschieben. Als Resultat wurde eine neue Klasse von GaN Nanodrähten mit bisher unerreichten strukturellen und optischen Eigenschaften geschaffen. Mithilfe eines Zwei-Schritt-Ansatzes, bei dem die Wachstumstemperatur während der Nukleationsphase erhöht wurde, konnte eine verbesserte Kontrolle über die Flächendichte, den Durchmesser und den Koaleszenzgrad der GaN-Nanodraht-Ensembles erreicht werden. Darüber hinaus werden Ansätze präsentiert, um die außerordentlich lange Inkubationszeit bei hohen Wachstumstemperaturen zu minimieren und damit wesentlich höhere Wachstumstemperaturen zu ermöglichen (bis zu 905°C). Die resulierenden GaN-Nanodraht-Ensembles weisen schmale exzitonische Übergänge mit sub-meV Linienbreiten auf, vergleichbar zu denen freistehender GaN-Schichten. Abschließend wurden Nanodrähte mit Durchmessern deutlich unterhalb von 10 nm fabriziert. Mithilfe eines Zersetzungsschrittes im Ultrahochvakuum direkt im Anschluss an die Wachstumsphase wurden reguläre Nanodraht-Ensembles verdünnt. Die resultierenden ultradünnen Nanodrähte weisen dielektrisches Confinement auf. Wir zeigen eine ausgeprägte exzitonische Emission von puren GaN-Nanodrähten mit Durchmessern bis hinab zu 6 nm. / In molecular beam epitaxy, dense arrays of GaN nanowires form spontaneously on crystalline as well as amorphous substrates. Due to the nature of spontaneous formation, the control over important parameters is limited. This thesis addresses the major limitations of spontaneous nanowire formation, namely the nanowire diameter, number density, and coalescence degree but also the maximum achievable growth temperature, and presents approaches to overcome the same. Thereby, we have fabricated a new class of nanowires with unprecedented structural and optical properties. We find that a two-step growth approach, where the substrate temperature is increased during the nucleation stage, is an efficient method to gain control over the area coverage, average diameter, and coalescence degree of GaN nanowire ensembles. Furthermore, we present growth approaches to minimize the long incubation time that precedes nanowire nucleation at elevated temperatures and to thus facilitate significantly higher growth temperatures (up to 905°C). The GaN nanowire ensembles grown at so far unexplored substrate temperatures exhibit excitonic transitions with sub-meV linewidths comparable to those of state-of-the-art free-standing GaN layers grown by hydride vapor phase epitaxy. Finally, we fabricate nanowires with diameters well below 10 nm, the lower boundary given by the nucleation mechanism of spontaneously formed nanowires. Here, regular nanowire arrays are thinned in a post-growth decomposition step in ultra-high vacuum. In situ monitoring the progress of decomposition using quadrupole mass spectrometry enables a precise control over the diameter of the thinned nanowires. These ultrathin nanowires show dielectric confinement, which is potentially much stronger than quantum confinement. We demonstrate intense excitonic emission from bare GaN nanowires with diameters down to 6 nm.

Synopsis of thesis entitled “Electrochemical and Photoelectrochemical Investigations of Co, Mn and Ir-based Catalysts for Water Splitting” by Ahamed Irshad M (SR No: 02-01-02-10-11-11-1-08823) under the supervision of Prof. N. Munichandraiah, Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore (India), for the Ph.D. degree of the Institute under the Faculty of Science. Hydrogen is considered as the fuel for future owing to its high gravimetric energy density and eco-friendly use. In addition, H2 is an important feedstock in Haber process for ammonia synthesis and petroleum refining. Although, it is the most abundant element in the universe, elemental hydrogen is not available in large quantities on the planet. Consequently, H2 must be produced from its various chemical compounds available on earth. Currently, H2 is produced in large scale from methane by a process called steam-methane reforming (SMR). This process releases huge amount of CO2 into atmosphere as the by-product causing serious environmental issues. The development of alternate clean methods to generate H2 is a key challenge for the realization of hydrogen economy. Production of H2 gas by water splitting using electricity or sunlight is known. Low cost, high natural abundance and carbon neutrality make water as the best source of hydrogen. Thermodynamically, splitting of H2O needs 237 kJ mol-1 of energy, which corresponds to 1.23 V according to the equation, ΔG = -nFE. However, commercial electrolyzers usually operate between 1.8 to 2.1 V, due to the need of large overvoltage. The high overvoltage and subsequent energy losses are mainly associated with the sluggish kinetics of oxygen evolution reaction (OER) at the anode and hydrogen evolution reaction (HER) at the cathode. The overvoltage can be considerably reduced using suitable catalysts. Hence, the design and development of stable, robust and highly active catalysts for OER and HER are essential to make water splitting efficient and economical. Attempts in the direction of preparing several novel OER and HER catalysts, physicochemical characterizations and their electrochemical or photoelectrochemical activity are described in the thesis. A comprehensive review of the literature on various types of catalysts, thermodynamics, kinetics and mechanisms of catalysis are provided in the Chapter 1 of the thesis. Chapter 2 furnishes a brief description on various experimental techniques and procedures adopted at different stages of the present studies. Chapter 3 explains the results of the studies on kinetics of deposition and stability of Nocera’s Co-phosphate (Co-Pi) catalyst using electrochemical quartz crystal microbalance (EQCM). The in-situ mass measurements during CV experiments on Au electrode confirm the deposition of Co-Pi at potential above 0.87 V vs. Ag/AgCl, 3 M KCl (Fig.1a and b). The catalyst is found to deposit via a nucleus mediated process at a rate of 1.8 ng s-1 from 0.5 mM Co2+ in 0.1 M neural phosphate solution at 1.0 V. Further studies on the potential and electrolyte dependent stability of the Co-Pi suggest that the catalyst undergoes severe corrosion at high overpotential and in non-buffer electrolytes. Current/ Fig.1 (a) Cyclic voltammograms and (b) mass variations vs. potential of Au-coated quartz crystal in 0.1 M potassium phosphate buffer solution (pH 7.0) containing 0.5 mM Co(NO3)2 Chapter 4 deals with the electrochemical deposition of a novel OER catalyst, namely, Co-acetate (Co-Ac) from a neutral acetate electrolyte containing Co2+ ions. Use of acetate solution instead of phosphate avoids the solubility limitations and helps to get thick layer of the catalyst in a short time from concentrated Co2+ solutions. In addition, the Co-Ac is found to be catalytically superior to Co-Pi (Fig. 2a). It is also observed that the Co-Ac catalyst undergoes ion exchange with electrolyte species during electrolysis in phosphate buffer solution, which results in the formation of a hybrid Co-Ac-Pi catalyst (Fig. 2b). The presence of both acetate and phosphate ions in the catalyst and their synergistic catalytic effect enhance the OER activity. Fig.2. (a) Linear sweep voltammograms of Co-Ac in (i) phosphate and (ii) acetate electrolytes, and that of Co-Pi in (iii) acetate and (iv) phosphate electrolytes. (b) SEM image showing the formation of two layers of the catalysts after electrolysis in phosphate solution. In Chapter 5, high OER activity of an electrodeposited amorphous Ir-phosphate (Ir-Pi) is investigated. The catalyst is prepared by the anodic polarization of a carbon paper electrode in neutral phosphate solution containing Ir3+ ions (Fig. 3). The Ir-Pi film deposited on the electrode has Ir and P in an approximate ratio of 1:2 with Ir in an oxidation state higher than +4. Phosphate ions play a major role for both the electrochemical deposition process and its catalytic activity towards OER. The Ir-Pi catalyst is superior to similarly deposited IrO2 and Co-Pi catalysts both in terms of onset potential and current density at any potential in the OER region. Tafel measurements and pH dependence studies identify the formation of a high energy intermediate during oxygen evolution. Fig.3. (a) Cyclic voltammograms during the Ir-Pi deposition and (b) SEM image of Ir-Pi on C. Chapter 6 is on the preparation of a composite of Mn-phosphate (MnOx-Pi) and reduced graphene oxide (rGO) and its utilization as an OER catalyst. The composite is prepared by the simultaneous electrochemical reduction of KMnO4 and graphene oxide (GO) in a phosphate solution (pH 7.0). Various analytical techniques such as TEM, XPS, Raman spectroscopy, etc. confirm the formation of a composite (Fig. 4) and electrochemical studies indicate the favourable role of rGO towards OER. Under identical conditions, MnOx-Pi-rGO gives 6.2 mA cm-2 at 2.05 V vs. RHE whereas it is only 2.9 mA cm-2 for MnOx-Pi alone. However, the catalyst is not very stable during OER which is ascribed to slow oxidation of Mn3+ in the catalyst. Fig.4. (a) Raman spectrum and (b) TEM image of MnOx-Pi-rGO. In Chapter 7, an amorphous Ni-Co-S film is prepared by a potentiodynamic deposition method using thiourea as the sulphur source. The electrodeposit is used as a catalyst for the HER in neutral phosphate solution. The composition of the catalyst and the HER activity are tuned by varying the ratio of concentrations of Ni2+ and Co2+. The bimetallic Ni-Co-S catalyst exhibits better HER activity than both Ni-S and Co-S (Fig. 5a). Under optimized deposition conditions, Ni-Co-S requires just 150 mV for the onset of HER and 10 mA cm-2 is obtained for 280 mV overpotential. The Ni-Co-S shows two different Tafel slopes, indicating two different potential dependent HER mechanisms (Fig. 5b). Presence of two different catalytic sites which contribute selectively in different potential regions is proposed. Fig.5. (a) Linear sweep voltammograms of HER at 1 mV s-1 in 1 M phosphate solutions (pH 7.4) using (i) Ni-S, (ii) Co-S and (c) Ni-Co-S. (b) Tafel plot of Ni-Co-S showing two Tafel slopes. Photoelectrochemical OER using ZnO photoanode and Co-acetate (Co-Ac) cocatalyst is studied in Chapter 8 of the thesis. Randomly oriented crystalline ZnO nanorods are prepared by the electrochemical deposition of Zn(OH)2 followed by heat treatment at 350 ºC in air. Co-Ac is then photochemically deposited onto ZnO nanorods by UV illumination in the presence of neutral acetate buffer solution containing Co2+ ions. The hybrid Co-Ac-ZnO shows higher photoactivity in comparison with bare ZnO towards PEC water oxidation (Fig. 6). Co-Ac acts as a cocatalyst and reduces the charge carrier recombination at the electrode/electrolyte interface. Fig.6. (a) Linear sweep voltammograms of ZnO under (i) dark and (ii) light conditions, and that of Co-Ac-ZnO in (iii) dark and (iv) light in 0.1 M phosphate (pH 7.0) electrolyte. Chapter 9 deals with PEC water oxidation using α-Fe2O3 photoanode and Ir-phosphate (Ir-Pi) cocatalyst. α-Fe2O3 is prepared by direct heating of Fe film in air which in turn is deposited by the electrochemical reduction of Fe2+. Thickness of the film as well as calcination temperature is carefully optimized. In order to further enhance the OER kinetics, Ir-Pi is electrochemically deposited onto α-Fe2O3. Under optimized conditions, Ir-Pi deposited α-Fe2O3 shows around 3 times higher photocurrent than that of bare α-Fe2O3 at 1.23 V vs. RHE (Fig. 7). Ir-Pi acts as a cocatalyst for OER and reduces the photogenerated charge carrier recombination. Fig.7. Photocurrent variation of α-Fe2O3 electrode at 1.23 V vs. RHE for (i) front and (ii) back side illuminations, against Ir-Pi deposition time. The thesis ends with a short summary and future prospectus of studies described in the thesis. The research work presented in the thesis is carried out by the candidate as the part of Ph.D. program. Some of the results have already been published in the literature and some manuscripts are under preparation. A list of publications is included at the end of the thesis. It is anticipated that the studies reported in the thesis will constitute a worthwhile contribution.

The thesis entitled “Novel Cationic Gemini Lipids, Click Chemistry Based Adducts and Amphiphile-Capped Silver Nanostructures: Synthesis, Aggregation and Biological Properties” elucidates the design, synthesis, aggregation and gene transfection properties of novel gemini cationic lipids based on cholesterol and pseudoglyceryl backbone, and click chemistry based adducts. This thesis also elucidates the synthesis and aggregation properties of silver nanoparticles loaded cationic liposomes and silver nanorods stabilized by micellar solutions of gemini surfactants. The work has been divided into six chapters. Chapter 1: Introduction: Membrane Formation from Cholesterol-based Cationic Lipids and their use as Non-Viral Gene Delivery Agents This chapter describes the importance of cholesterol in biological membranes, the aggregation properties of cholesterol-based cationic lipids and their interactions with phospholipid membranes. This chapter also gives a comprehensive account of the research towards the development of novel cationic cholesterol-based monomeric and gemini lipids. It also reviews the utilization of cholesterol-based cationic monomeric and gemini lipids in gene transfection properties. Chapter 2A: Effect of Hydroxyl group on the Cationic Headgroups of Cholesterol-based Gemini Lipids on their Aggregation, DNA Binding Properties and Interaction with Phospholipid Membranes This chapter describes the syntheses and aggregation properties of two series of cholesterol-based monomeric and gemini cationic lipids with and without hydroxyl functionality (Figure 1). The gemini lipids of a given series differ in their spacer polymethylene -(CH2)n- chain lengths between the cationic headgroups. Figure 1. Molecular structures of non-hydroxylated and hydroxylated cationic cholesterol-based gemini lipids and their monomeric counterparts. All monomeric and gemini lipids were found to generate stable suspensions in aqueous media. Electron microscopic studies showed that all the lipids form vesicular aggregates in aqueous media. The structures seen under TEM for the non-hydroxylated series of monomeric (C-M) and gemini lipids are of variable sizes, they appeared like separated vesicular aggregates. For the hydroxylated series of lipids, however, both the monomeric lipid aggregates (CH-M) and aggregates of their gemini counterparts were found to be ‘connected’ with each other to form elongated chain of aggregates of different length scales. XRD studies with the cast films of lipids revealed that the monomeric lipids of either series have higher bilayer width than the corresponding gemini lipids. Incorporation of the -(CH2)n- spacer units at the head group level joining the two monomeric units lowered the bilayer thicknesses of both series of the lipid aggregates. Thus the monomeric lipids (C-M and CH-M) appear to form nearly regular bilayer type arrangements whereas gemini lipids form interdigited and tilted bilayer arrangements in their aggregates. Calorimetry studies of the coaggregates showed that ~10 mol-% of most of the cholesterol gemini lipids is enough to abolish the phase transition of DPPC membranes whereas more than 10 mol-% is required in case of their monomeric counterparts. Further these thermotropic properties depend upon the length of the spacer of the gemini lipid included in the mixture. We have observed greater quenching of the thermal phase transition of DPPC membranes with 10 mol-% of C-M as compared to CH-M doped liposomes. At 10 mol-% of all the cationic lipid doped DPPC covesicles, only CG-3 doped liposomes showed an observable transition temperature. Maximum broadening of the DPPC transition peak was observed in the case of the gemini lipids, CHG-6 and CHG-12. DNA binding and release studies show that the interactions between gemini lipids and DNA depend upon the nature of the head group as well as the length of the spacer between the cationic head groups. For the non-hydroxylated cholesterol-based cationic lipid series, the monomeric liposomes of C-M facilitates the dissociation of EB from the EB-DNA complex to an extent of 93% at a maximum lipid:DNA ratio of 3.0 whereas the liposomes of CG-4 and CG-12 showed the lowest extent of maximum EB exclusion (~74%) from the EB-DNA complex at lipid:DNA ratio of 3.0. For hydroxylated cholesterol-based cationic lipid series, the monomeric liposomes of CH-M facilitate the dissociation of EB from the intercalated EB-DNA complex to an extent of 81 % whereas the liposomes of CHG-3 showed the minimum binding to DNA. Thus the two monomeric liposomes C-M and CH-M were the more efficient formulations that allow dissociation of DNA from the corresponding lipoplexes. These findings have important being in their gene transfection activity compared their respective gemini lipid counterparts. Chapter 2B: Novel Cholesterol-based Cationic Gemini Lipids possessing Hydroxyethyl group on the Headgroup: Transfection Efficacy and Cell Toxicity Properties This chapter describes the transfection efficacy and cell toxicity properties of five cholesterol based gemini cationic lipids possessing hydroxyethyl functionality on each head group, which differ in the length of the polymethylene spacer [-(CH2)n-] chain (Figure 2). These gemini lipids are important to gene delivery processes as they possess pre-optimized molecular features, e.g., cholesterol backbone, ether linkage and a variable spacer chain between both the headgroups of the gemini lipids. Cationic liposomes were prepared from each of these lipids individually and as a mixture of individual cationic gemini lipid and 1,2-dioleoylphosphatidylethanolamine (DOPE). The gemini lipid with a hydroxyethylated headgroup and a -(CH2)5- spacer, CHG-5 showed the highest transfection activity at N/P (lipid/DNA) ratio of 0.5 and lipid:DOPE molar ratio of 2. Upon comparison of the relevant parameters, e.g., % transfected cells, the amount of DNA transfected to each cell and % cell viability all together against LipofectAMINE 2000, one of the most potent commercially available transfecting agents, the optimized lipid formulation based on CHG-5/DOPE was found to be comparable. In terms of its ability to induce gene-transfer in presence of serum and shelf-life CHG-5/DOPE liposome was found to be better than its commercial counterpart. Recording of confocal images confirmed that in presence of 10% serum using 1.2 µg DNA per well and lipid:DOPE ratio of 1:4 and N/P charge ratio of 0.75, CHG-5 is better than LipofectAMINE 2000. These properties render them to be reagents of practical value for various gene delivery applications. Figure 2. Molecular structures of cholesterol-based cationic monomeric lipid and gemini lipids possessing hydroxyethyl group on the headgroup synthesized. Chapter 3: Bilayer Membrane and Stable Monolayer Forming Properties of Cationic Pseudoglyceryl Gemini Lipids having Polymethylene Spacers and Oxyethylene Linkages This chapter describes the synthesis of five new cationic pseudoglyceryl gemini lipid versions of their monomeric counterpart (Figure 3). Each cationic lipid aggregate in aqueous media was found to form vesicular structures as evidenced from the negatively stained TEM experiments and DLS measurements. XRD experiments with their cast films of aqueous dispersions revealed that introduction of the polymethylene -(CH2)n-spacer chain joining the two monomers decreased the bilayer widths of the gemini lipid aggregates. The inter-lipidic packing and the hydration of the lipid vesicles were examined using fluorescence anisotropy and generalized polarization measurements using membrane-soluble probes, DPH and Paldan respectively. Fluorescence anisotropy measurements showed that the aggregates of lipid 2c with -(CH2)5- spacer chain were highly packed and ordered in the vesicular aggregates than that of the other cationic lipid aggregates in the series. Paldan hydration studies showed that incorporation of the polymethylene -(CH2)n- spacer chains joining two monomeric units lowered the hydration of the gemini lipid aggregates in the solid gel state. Each of these cationic lipid aggregates showed sharp transition temperatures (Tm) as observed from differential scanning calorimetric studies. DSC studies further revealed that the incorporation of oxyethylene group at the linker region of cationic pseudoglyceryl gemini lipid 2a with (CH2)3- spacer chain length lowered the thermotropic phase transition temperature (Tm) of the aggregates in aqueous media when compared with the corresponding gemini analogue without oxyethylene linkages. Langmuir film balance studies showed that each cationic gemini lipid and their monomeric counterpart were able to form stable monolayers at the air-water interphase. We observed that the mean molecular area (collapse area) of each of the cationic lipid obtained from the Langmuir monolayer studies increased with increase in the spacer chain lengths. Figure 3. Molecular structures of the cationic pseudoglyceryl gemini lipids and their monomeric counterpart. Chapter 4: Vesicle and Stable Monolayer Formation from Simple ‘Click’ Chemistry Adducts in Water This chapter describes successful use of Cu(I) catalyzed “Click Chemistry” for the syntheses of a series of hitherto unknown amphiphilic adducts (M1, M2, D1 and T1) which on dispersal in water afforded vesicular aggregates as evidenced from dye entrapment, TEM, SEM, AFM and DLS studies (Figure 4). Figure 4. Molecular structures of triazole based adducts. XRD experiments with their cast films of aqueous suspensions indicate the formation of a tilted bilayer arrangement for the aggregates of M1 whereas regular bilayer structures are predominant for the aggregates derived from M2, D1 and T1. Measurement of pKa values using UV-Vis spectroscopy showed that the aggregates of monomeric click adducts (M1 and M2) possess less pKa value than that of the aggregates of dimeric (D1) and tetrameric (T1) analogues and the values lie within the range of 2.8-3.2. The hydrodynamic diameter of the aggregates of each click adduct increased with decrease in the pH of the media. Thus, the protonation of the triazole groups in the aggregates of each click adduct increased the hydrodynamic diameter. Dye entrapment studies showed that each click chemistry based adduct formed closed vesicular aggregates with inner aqueous compartment in aqueous media. The temperature induced order-to-disorder transitions of the aggregates and the accompanying changes in hydration were examined using high sensitive DSC, fluorescence anisotropy and generalized polarization measurements using a membranesoluble probe, DPH and Paldan respectively. In the solid state, M1 remains as the most hydrated species whereas in the fluidized phase, D1 maintains as the most hydrated aggregate. Clearly simple variation in the adduct molecular architecture bring about significant changes in their packing in aggregates and also the hydration of the resulting vesicles. Langmuir monolayer studies confirmed that these click adducts do form stable monolayers as well on water subphase at the air-water interface. We also calculated the mean molecular areas from the Langmuir monolayer studies and as perhaps expected the adduct T1 has the highest head group area. Thus click chemistry based simple triazole adducts, which can be very easily prepared, are good candidates for further investigations involving syntheses of novel self-assembling structures. Chapter 5: Lipid Mediated Synthesis of Silver Nanoparticles, their Physical Characterizations and DNA Binding Abilities In this chapter, work on the Ag-NP (silver nanoparticle) loaded liposomes preparation using four cationic lipids (1-4) in which the Ag-NPs were entrapped within lipid bilayer has been described. A novel method was developed to synthesize the Ag-NPs where the lipid itself capped and stabilized the Ag-NPs. Consequently there was no need of inclusion of any other capping agents like citrate. Confocal microscopy confirmed that these Ag-nanoparticles are fluorescent in character. It was also demonstrated that silver nanoparticles are indeed entrapped in lipid bilayer with transmission electron microscopy (TEM). DLS experiments provided information about the hydrodynamic diameter of the lipid vesicles which increased with the increase in Ag concentrations. This could be due to the ‘loosening’ of the lipid packing in vesicles. Zeta potential measurements showed that the zeta potential value decreased with the increase in the concentration of Ag-NPs in the cationic lipid vesicles. XRD studies with the cast films of the lipid or Ag-NP loaded lipid suspensions revealed that when the Ag-NPs get entrapped into the bilayer of the multilamellar vesicles of the lipid in the aqueous media, the unit bilayer thickness of the aggregates increased. Paldan experiments showed that with the incorporation of Ag-NPs in the lipid vesicles, the hydration of the lipid vesicles increased to a significant extent but the phase transition temperatures remained practically unaltered for all the lipids. Fluorescence anisotropy experiments revealed that the hydrocarbon chain packing of the lipid vesicles ‘loosens’ with the incorporation of Ag-NPs. Ag-NP loaded liposomes showed enhanced DNA binding ability and also the presence of Ag-NPs in cationic liposomes induced the release of DNA from silver nanoparticle-loaded lipoplexes more effectively. Figure 5. Molecular structures of the cationic lipids mentioned in the present chapter. Chapter 6: Dependence of Spacer Chain Lengths in the Synthesis of Ag-Nanorods in Gemini Cationic Surfactant Micelles Figure 6. Chemical structures of cationic gemini surfactants. This chapter describes the synthesis of Ag-nanospecies by seed-mediated wet synthesis method using four gemini surfactants (16-2-16, 16-4-16, 16-5-16 and 16-1216) as the capping agents (Figure 6). For this, we first synthesized Ag-nanoseeds of diameter ~7 nm stabilized by trisodium citrate (as capping agent). Then the solution containing Ag-nanoseeds was used to synthesize Ag-nanorods of different aspect ratios. It was that with decreasing Ag-nanoseed concentration, the aspect ratios of Agnanorods stabilized by gemini surfactants (16-2-16 and 16-4-16) increased gradually as evidenced from TEM images. These Ag-nanoseeds and Ag-nanorods were further characterized using UV-Vis spectroscopy (to know the surface plasmon bands), transmission electron microscopy (TEM), energy-dispersive X-ray spectroscopy (EDAX) and X-ray diffraction (XRD). It was observed that when gemini surfactant 164-16 was used to stabilize Ag-nanorods, the λmax of the longitudinal band shifted more towards the red region (red-shift) as observed by UV-Vis spectroscopy when compared to that of gemini surfactant with shortest spacer, 16-2-16. Thus the gemini surfactants with shorter -(CH2)2- and -(CH2)4- spacer chains promoted the growth of Ag-nanorods in their micellar solutions whereas -(CH2)5- and -(CH2)12- spacer chains of gemini surfactants did not. So, the growth of Ag-nanorods in micellar solutions is found to be highly spacer-chain length specific. TEM micrographs revealed that the aspect ratios of Ag-nanorods stabilized by gemini surfactants 16-4-16 are larger than those compared to the Ag-nanorods stabilized by gemini surfactants 16-2-16 at a particular amount of Agnanoseed solution. TEM images of the samples containing micellar solutions of gemini surfactants 16-5-16 and 16-12-16 showed that the formation of only Ag-nanoparticles of larger sizes (compared to Ag-nanoseeds stabilized by trisodium citrate) and Agnanoprisms irrespective of the amount of Ag-nanoseed solution added. No Ag-nanorod formation in the micellar solutions of gemini surfactants 16-5-16 and 16-12-16 was observed. Gemini surfactants (16-2-16 and 16-4-16) formed bilayer arrangements to facilitate the growth and stabilization of Ag-nanorods in aqueous media where the inner layer is attached to the Ag-nanorod surface through the gemini surfactant ammonium headgroups. X-ray diffraction (XRD) studies showed that these Ag-nanorods stabilized by gemini surfactants 16-2-16 and 16-4-16 crystallized in the aqueous media via (111), (220) and (222) lattice faces. Thus this study demonstrated the way one can control structures and shapes of the silver nanoobjects using gemini surfactant micelles. (For structural formula pl refer the thesis)

Microplastics take hundreds to thousands of years to degrade in nature, and pose a threat to the environment. A photocatalytical degradation method have been developed to take advantage of solar light to degrade microplastics, however it takes several months to degrade microplastics with the process. The purpose of this study is to enhance the degradation rate of microplastics by synthesizing a material where photocatalysis is combined with Fenton reaction. A material with zinc oxide nanorods coated with tin oxide and decorated with iron particles (𝑍𝑛𝑂/𝑆𝑛𝑂2/𝐹𝑒0) was synthesized and used to degrade methylene blue, polystyrene and polypropylene. The result show that the degradation rate with a 𝑍𝑛𝑂/𝑆𝑛𝑂2/𝐹𝑒0 – sample is faster than with a 𝑍𝑛𝑂 – sample, and that it can be used to degrade polystyrene and polypropylene.Students’ view on researchers can affect the development of their interest and attitude towards science. Study visits to laboratories have been used to increase students’ interest and give them new experiences. The purpose of this study is to investigate what and how high school students learn during a study visit to a nanotechnology laboratory, and how the study visit affects high school students’ interest and motivation for research and learning. A study visit with 5 stations was organized, and students were given a questionnaire about what they learned during the study visit. Thematic analysis was used to analyze the students’ answers. The result shows that the study visit increased students’ interest in research, and the importance of designing stations so that they are connected to students’ previous knowledge and are within their proximal development zone. / Mikroplaster tar hundratals till tusentals år att bryta ner i naturen och utgör ett hot mot miljön. En fotokatalytisk nedbrytningsprocess har utvecklats där solljus utnyttjas för att bryta ner mikroplaster, dock tar det flera månader att bryta ner mikroplaster med den processen. Syftet med denna studie är att förbättra nedbrytningshastigheten av mikroplaster genom att syntetisera ett material där fotokatalys kombineras med Fenton-reaktion. Ett material med zinkoxid nanorör belagda med tennoxid och dekorerade med järnpartiklar (𝑍𝑛𝑂/𝑆𝑛𝑂2/𝐹𝑒0) syntetiserades och användes för att bryta ner metylenblått, polystyren och polypropen. Resultatet visar att nedbrytningshastigheten med 𝑍𝑛𝑂/𝑆𝑛𝑂2/𝐹𝑒0 – materialet är snabbare än med ett 𝑍𝑛𝑂 – material, och att 𝑍𝑛𝑂/𝑆𝑛𝑂2/𝐹𝑒0 – materialet kan användas för att bryta ned polystyren och polypropen.Elevers syn på forskning och forskare kan påverka utvecklingen av deras intresse och inställning till vetenskap. Studiebesök på laboratorier har använts för att öka elevernas intresse och ge dem nya erfarenheter. Syftet med denna studie är att undersöka vad och hur gymnasieelever lär sig under ett studiebesök i ett nanotekniklaboratorium och hur studiebesöket påverkar gymnasieelevernas intresse och motivation för forskning och lärande. Ett studiebesök med 5 stationer organiserades och eleverna fick ett frågeformulär om vad de lärde sig under studiebesöket. Tematisk analys användes för att analysera elevernas svar. Resultatet visar att studiebesöket ökade elevernas intresse för forskning och vikten av att utforma stationer så att de är kopplade till elevernas tidigare kunskaper och ligger inom deras proximala utvecklingszon.