Introduction
This paper will focus on how the annealing of lead zirconium titanate thin films affects its various properties, including its microstructure and electrical properties. This includes examining factors such as the annealing methods, environment, temperature, hold time and heating rate. Lead zirconium titanate is important because improvements in its production will allow for major improvements the next generation of electronic sensors and storage systems.
Background
Piezoelectric materials are a class of materials that exhibit gaining or changing polarization when a stress is applied to the material. Polarization is the separation of charges when a material is exposed to an electric field. This ability to polarize allows
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Figure 1: Perovskite Structure of PZT (Structure of PZT)
PZT is mostly used in thin film formations and is known for its high dielectric constant, meaning that PZT can store a large amount of electric charge in an electric field. This dielectric constant depends on the film’s composition, with the highest value measured around the morphotropic phase boundary. The morphotropic phase boundary is where a ferroelectric material transitions from its tetragonal and rhombohedral phases, which for PZT is around an atomic ratio of 1.00 Pb:0.52 Zr:0.48 Ti (Chen et al., 1992). PZT is made via a number of processes where a film of the desired composition is deposited on a substrate and annealed to crystallize. The film deposition can take place in different ways, including sol-gel spin coating, molecular beam epitaxy, chemical vapor deposition, pulsed laser deposition and sputtering (Chang, 1999). While these factors have an impact on the final properties of the PZT, the final annealing determines the majority of the properties.
The annealing of lead zirconate titanate is similar to annealing any other material where heating the material improves the crystallinity of the material and removes defects. For PZT this is especially important since the amorphous phase must transform into another phase before finally transforming into the desired perovskite phase. This intermediate phase is the pyrochlore phase, which
Ceramics Engineering-- the industry that Materials Technology Corporation, or "MTC" is a part of-- is a multi-billion dollar a year industry. Because ceramics can be manufactured to have unique combinations of strength, weight, thermal and magnetic conductivity, and deformability, they have countless uses in industries such as aerospace, biomedical, automotive, and electrical. With an unlimited number of such combinations, it is possible to create a material that exactly suits a given situation.
The doping iron increases the capacity of batteries, but this diminishes with extensive cycling. The detrimental effect of iron can be avoided by annealing. Ruthenium is another transition metal which can be used as a dopant which enhances the stability of the crystal structure. It also increases conductivity and improve performance of the battery. Chromium is another transition metal that can be used as a dopant. It reduces the ordering of lithium ions in LiMn2O4 spinel and this stabilizes the spinel structure. It also increases capacity retention during cycling. Zinc is used as a dopant in cathode materials as it has a stabilizing effect on the crystal structure. Addition of Zinc oxide also prevents reaction between the electrode and electrolyte. Titanium along with cobalt also acts as a stabilizer and also reduces dissolution of electrodes. Zirconium reduces reactivity levels between the electrode and the electrolyte and performs the same function as titanium by stabilizing the crystal structure. Aluminium is one of the most commonly used dopants in cathode materials. It performs the function of increasing capacity of the electrodes. The addition of aluminium improves electrode kinetics, structural modifications and microstructural effects. Some of the other dopants include Magnesium and Lathanum which increases the lattice parameter and improves the stability of the crystal structure and also
Where α is an empirical parameter (0 ≤α≤1) and f is the frequency in Hz. This formula considered the deviation from the ideal RC-behavior due to surface inhomogeneties, roughness effects, and different compositions of surface layers 40, 41. The first time constant at low frequency range was claimed to the presence of an inhomogeneous passive film 42. A constant phase element (CPE) was used instead of a pure capacitance due to these inhomogenities, which were found at the oxide/electrolyte interface and under the oxide film. CEE can be introduced in terms of impedance from the following equation:
We calculated the specific heat of metal one to be 0.39 J/g℃ which correlates to the exact specific heat capacity of element 30 Zinc. For metal two, we calculated the specific heat capacity to be 0.38 J/g℃ which was close to the actual specific heat of element 23 Iron. The specific heat capacity of Iron was 0.45 J/g℃. Our inaccuracy could be a result of not reading the thermometer as accurately as we could have. To improve yield in the future, we could make sure we record more accurate temperatures.
With the strain rate constant it can be seen that different temperatures do not affect the stress-strain curve of the nanocomposite. As in the section 2.3.1 we define a parameter for the temperature sensitivity as:
When two objects made of different materials rub together, electrons can be transferred from one object to the other.
The use of energetic materials has been increasing as the years go on. Azo-Tetrazolate belongs to high nitrogen content high-density energy materials (HNC, HEDMs). The norm for (HNC, HDEMs) is that they have good thermal stability, impact and shock insensitivity, good performance and the possibility for the formation of less smoke or soot. This seems nearly impossible, as having good thermal stability and impact insensitivity usually results in low explosive performance. The need for a good mix of all three qualities has resulted in growing interest in high-energy density materials, high nitrogen content (HEDMs, HNC). Azo-Tetrazolate and its derivatives are the most recent developments in this field. They come in the form of salts with high nitrogen content and high (positive) heats of formation. These salts have exhibited both good insensitivity to friction, shock, and electrostatic discharge while having a good performance value. The nonmetallic salts of 5,5′-azotetrazolate include Guanidinium Azo-Tetrazolate (GAT), Aminoguanidinium Azo-Tetrazolate (AGAT), Diaminoguanidinium Azo-Tetrazolate (DAGAT), Triaminoguanidinium Azo-Tetrazolate (TAGAT), and Ammonium Azo-Tetrazolate
In this paper, I discuss the characteristics and different applications of piezoelectric material and how matching is an important to observe the behavior of
5a shows X-ray photoelectron spectroscopy in determining the electronic state of Fe present in BaFe12O19 ceramic. Due to their different binding energy, the presence of Ba, Fe and O is quite evident. The C 1s peak (284.5 eV) which appears at 289.1 eV in our sample, was used as the reference for charge correction. The deconvolution of Fe spectrum done using origin software considering Gaussian function is shown in Fig. 5b. The peaks occurred at 710.7 eV and at 712.6 eV of the main 2p3/2 peak, are in accordance with the Fe2+ and Fe3+ oxidation state. The presence of Fe3+ is also confirmed by the satellite peak at 718.7 eV and 2p1/2 peak at 725.6 eV
They have good mechanical strength, and are hard, chemically inert and immune to humidity, which lead to the application of piezoelectric ceramics for the generation of voltage, electromechanical actuation, frequency control and the generation and detection of acoustic and ultrasonic energy [1, 3]. Piezoelectric ceramics are used in generators, sensors, actuators, and transducers, etc. [4]. They are also used in daily life such as some piezoelectric cigarette lighters, most battery operated smoke detector alarms, many gas grill igniters [5]. There have been a variety of research due to the wide applications of piezoelectric ceramics and the prospect for future development and improvement. Therefore, this paper will briefly introduce the history, applications and future development of piezoelectric ceramic
This manufactured piezoelectric are usually made of barium titanate, lead zirconate and lead metaniobate. Moreover, manufactured piezoelectric can be made in any size or shape desired. However, manufactured piezoelectric loses sensitivity above a critical temperature better “known as the Curie point” [1]. The Curie point can be between 120 oC and 600 oC, which depend on the material of the piezoelectric.
(-- removed HTML --) In spite of much attention that has been given to heterostructures involving polar materials, only recently, the charge transfer at the interface of nonpolar/nonpolar oxides due to ferroelectric polarization discontinuity has been in focus. The driving force behind this charge transfer is the large electrostatic energy penalty for a buildup of charge at the interface caused by discontinuous polarization across the interface of PbTiO (-- removed HTML --) 3 (-- removed HTML --) /SrTiO (-- removed HTML --) 3 (-- removed HTML --) , for example, Ref. (-- removed HTML --) 5 (-- removed HTML --) . Chen (-- removed HTML --) et al. (-- removed HTML --) and Nazir (-- removed HTML --) et al. (-- removed HTML --) have found that a lattice-mismatch induced compressive strain leads to a strong polarization and the newly formed interfacial metallic states can depend
Polymer derived ceramics (PDC) were first introduced over thirty years ago, and are a fundamental material in high demand today. Over the years, these materials have been heavily studied to better understand how to manufacture them and determine their desired properties. Such materials include coatings, ceramic fivers, and ceramics containing properties that allow them to have high stability at high temperatures. Desired properties of PDC typically include high resistance to decomposition, phase separation, crystallization, high chemical durability, semi-conductivity, and creep. [4]
BC Au electrode OTFTs based on the process sequence of pentacene/OTS/AP plasma treatment/Au electrode (patterned)/APS/SiO2 was fabricated. The electrical characteristics of OTFTs with plasma treatment showed relatively high performances of devices with a low-contact resistance (Fig. 7). The current crowding effect seen in the output characteristics of the reference device can be responsible for the low performance of the device. [43,44]. In contrast, the fabricated device with 12 kV AP plasma treatment reveals the highest performance including a mobility, an on/off current ratio (Ion/Ioff), Vt, and low subthreshold slope (S) of 0.23 cm2 V-1 S-1, 9.8 × 105, −1.63 V, and of 0.16 mV dec-1 (Table 2).
We have now discussed the two extremes in electronic materials; a conductor, and an insulator we will now move to a material that lies in between these two, a semiconductor. The