5.1. INTRODUCTION Interest in thin-film formation processes dates at least to the 1920s. During research at the Cavendish Laboratories in England on evaporated thin films, the concept of formation of nuclei that grew and coalesced to form the film was advan[r]
There were obtained SRGs with a pitch of 250 nm and 1 µm, depending on the irradiation set-up. The modulation depth was between 10 nm and 800 nm, depending on the incident fluence/intensity and the number of subsequent incident pulses. The surface relief modulation time is of the order[r]
450 4. Block and crystal structure of films 4.1 BPI films Block structure of films can be visualized by means of polarizing microscope in reflection mode because BPI as well as other amino acid ferroelectrics belongs to low symmetry class and are characterized by strong[r]
IX properties of the light and its applicability in integrated optical components as well as sub- system for optical communications. The chapter fifteenth by G. Telipan, et al. describes the physical properties of linear polymer and organic molecules. The physical properties[r]
separately measured ionic and electronic conductivities in LbL assembled conducting polymer films by de-doping the conducting polymer to minimize the contribution from electronic conductivity. 54 However, EIS modeling of LbL films to measure ionic and[r]
In both linear and concentric SRGs, three main steps for preparing a sample are required; Azo-polymer thin film coating on fiber end facet, and optical interference pattern generation and exposure to the inscribing laser beam. It is noteworthy that these one-step and direct exposure metho[r]
the z-axis in the back focal region of an external lens and measures the far-field on-axis ( i.e ., closed aperture) transmittance and the whole ( i.e ., open aperture) transmittance as a function of the scan distance z . We have performed the Z-scan experiment by using a He- Ne l[r]
The proposed structure of these co-sputtered films was shown as Figure 2 .After co-sputtering process, the amorphous as-deposited NTO thin films were annealed in vacuum atmosphere.. It i[r]
In order to achieve small and uniform grains and modify magnetic properties of CoCrPt films for high areal density magnetic recording, the effects of NiP seedlayer on the microstructure [r]
Nevertheless, prior to proceeding to this characterization, it is important to check the epitaxial relationship between the bottom electrode and PZT films. Indeed, it must be kept in mind that the framework of this study is the fundamental understanding of the impact of crystal structure[r]
TRANG 4 TABLE OF CONTENTS ACKNOWLEDGEMENTS ii TABLE OF CONTENTS iv SUMMARY vii LIST OF TABLES ix LIST OF FIGURES x CHAPTER 1: INTRODUCTION 1 1.1 Magnetic thin films 3 1.1.1 Continuous ma[r]
Magnetic properties of Co-ferrite films with a thickness of 40 nm deposited on glass with a ZnO underlayer at different substrate temperatures [Coercivity _Hc, the remanence ratio Mr/Ms,[r]
Polycrystalline Silicon Thin Film Transistors (poly-Si TFTs) have been played as important driving elements for Flat panel display (FPD). In this work, we studied crystallinities of laser-crystallized poly-Si thin films using Multi-Line Beam (MLB) –CLC and investigated the dependence of poly-Si thin[r]
TRANG 5 ii TABLE OF CONTENTS ACKNOWLEDGEMENT I TABLE OF CONTENTS II SUMMARY VI LIST OF FIGURES VIII LIST OF ABBREVIATIONS XII LIST OF SYMBOLS XIII CHAPTER 1: INTRODUCTION 1 1.1 Anti-ferr[r]
This article reviews the development in our laboratory of magnetic lattices comprising periodic arrays of magnetic microtraps created by patterned magnetic films to trap periodic arrays of ultracold atoms.
For the magnetic Tb(Fe0 55CoU45)ri, (known as TerfecoHan) film, the field-dependence of the longitudinal Hall effect is carried out at various angles a between the applied[r]
a Absorption spectra C6PcH2 in chloroform solution empty-rectangles and solid thin films filled-circles and absorption spectra of C6PcH2:PC70BM BHJ thin film with various amounts of DIO [r]
We report on an environmentally friendly and versatile chemical solution deposition route to K0.5Na0.5NbO3 (KNN) thin films. The excess amounts of K and Na in KNN precursor solutions was found to be strong influence on perovskite KNN single-phase thin films. It was revealed from Raman spectroscopic[r]
5. Conclusion The VO 2 material fabricated using the PLD technique results in crystalline thin films performing sharp, high amplitude SMT phase transition and with very good electrical properties. The electrical and temperature-activated VO 2 -based sw[r]
concentration. The best hydrothermal annealing temperature for the formation of TiO 2 nanorod thin films is 150 o C. At temperatures lower than 120 ° C, did not see the formation of TiO 2 nanorod thin films on substrate. At a temperature of 18[r]