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Evaporation, thermal

Thermal evaporation in vacuum allows for deposition and purification of small molecule organic semiconductors. The material is placed into a vacuum and heated. Once the vapor pressure of the heated material exceeds the background pressure of the material in the chamber, the material evaporates and condenses on cooler surfaces that it lands on. High molecular weight organic semiconductors cannot be deposited this way they are too heavy to evaporate and decompose instead. [Pg.30]

Thermal evaporation of metals and semiconductor materials is t3rpically performed under high or ultra high vacuum conditions. This is done for three main reasons. First, the evacuation of the chamber reduces the partial pressure of oxygen or other gases which may react with, become embedded in, or [Pg.30]

Gases can be seen as collections of particles that collide elastically with each other and have a total kinetic energy that depends on the temperature of the gas. The mean free path for a gas can be shown to be proportional to the pressure and is given by  [Pg.31]

In air and at room temperature, a typical mean free path is 65nm. Evaporated materials at atmospheric pressure, therefore, scatter many times before [Pg.31]

Once heating of the source begins there are additional sources of background gas including desorption of gases from the source, crucible (if one is used), filaments, and other surfaces in the vacuum chamber through radiative or conductive heating volatile materials incorporated in the source material and thermal decomposition products. [Pg.32]

Most of the synthesis methods for nanoparticles have the disadvantages of impurities, expensive raw materials, special conditions, tedious procedures, long reaction times, and not being environmentally friendly. The drawbacks limit the commercial use of nanoparticles however, the simple synthesis and inexpensive method of thermal evaporation overcomes some of the shortcomings of previous methods. Pan et al. [88] prepared silicon-based nanostructures with different colors, morphologies, and microstructures over a wide temperature range of 890-1,320°C by thermal evaporation of Si02 powder at 1,350°C for 5 h. [Pg.7]


Thermal Evaporation. Thermal evaporatioa is doae ia a high vacuum to minimise chemical side reactioas of the evaporated active metal. [Pg.137]

Zinc Costing of Ca.pa.citors, In the zinc coating of paper strip for capacitors, the paper strip is fed from air through locks into a vacuum environment. There, it is coated by thermally evaporated zinc. The rate of evaporation is so high that contamination of the zinc vapor is excluded. The paper is fed at the maximum rate permitted by its own strength. [Pg.367]

Thermal outbreathing or venting requirements, including thermal evaporation for a fluid (the code refers to oil) with a flash point of 100°F or below, use at least the figures of Column 4 in Table 7-14. [Pg.468]

Thermal outbreathing or venting requirements, including thermal evaporation for a fluid (the code... [Pg.468]

In Section 13.2, we introduce the materials used in OLEDs. The most obvious classification of the organic materials used in OLEDs is small molecule versus polymer. This distinction relates more to the processing methods used than to the basic principles of operation of the final device. Small molecule materials are typically coated by thermal evaporation in vacuum, whereas polymers are usually spin-coated from solution. Vacuum evaporation lends itself to easy coaling of successive layers. With solution processing, one must consider the compatibility of each layer with the solvents used for coating subsequent layers. Increasingly, multilayered polymer devices arc being described in the literature and, naturally, hybrid devices with layers of both polymer and small molecule have been made. [Pg.219]

There are many organic compounds with useful electronic and/or optical properties and with sufficiently high volatility to be evaporable at a temperature well below that at which decomposition occurs. Since thermal evaporation lends itself to facile multilayering, organic compounds may be selected for use in one or more function electron injection, electron transport, hole injection, hole transport, andI or emission. A complete list of materials that have been used in OLEDs is too vast to be included here. Rather, we list those that have been most extensively studied. [Pg.221]

In our recent work, we have used Pd deposited on t hkl) in order to characterize thin metal films [Arenz et al., 2002] and to test their catalytic activity (Fig. 8.16). We have employed both methodologies thermal evaporation in UHV and electrochemical deposition. For the Pd/Pt(l 11) system, in situ SXS measurements have been used to show that after the formation of 1 ML of pseudomorphic Pd film, three-dimensional pseudomorphic crystalline islands of pure Pd begin to aggregate. [Pg.264]

The transparent top contact is deposited last of all, which imposes restrictions on the process temperature. Thermally evaporated ITO and ZnO deposited by metal-organic CVD (MOCVD) are most suitable. At a typical thickness of 70 nm the ITO serves as a good antireflection coating as well. Due to the somewhat high sheet resistance, a metal (Ag) grid is necessary to reduce the series resistance [11]. [Pg.172]

Supported model catalysts are frequently prepared by thermally evaporating metal atoms onto a planar oxide surface in UHV. The morphology and growth of supported metal clusters depend on a number of factors such as substrate morphology, the deposition rate, and the surface temperature. For a controlled synthesis of supported model catalysts, it is necessary to monitor the growth kinetics of supported metal... [Pg.85]

Fouad, O.A., Ismail, A.A., Zaki, Z.I. and Mohamed, R.M. (2006) Zinc oxide thin films prepared by thermal evaporation deposition and its photocatalytic activity. Applied Catalysis B Environmental, 62, 144-149. [Pg.243]

In molecular beam epitaxy (MBE), the constituent elements of the desired film in the form of molecular beams are deposited epitaxially onto a heated crystalline substrate. These molecular beams are typically from thermally evaporated elemental sources (e.g., evaporation of elemental As produces molecules of As2, As3, and As4). A refinement of this is atomic layer epitaxy (ALE) (also known as atomic layer deposition, ALD) in which the substrate is exposed alternately to two... [Pg.702]

A1(PBI)3] (c.f. the Bell analogue mentioned above and in Figure 1(c)) is also a stable complex which can be thermally evaporated and also emits in the blue region of the spectrum.187... [Pg.706]

Figure 4.8. Current voltage curves for selected A1PO capacitor structures. A high-quality thermally oxidized Si02 dielectric in an identical structure is included for reference. Top contacts are 0.011-cm2 A1 dots thermally evaporated via shadow mask. Bottom contact is made via conductive substrate p++ Si in the case of 600 °C A1PO and Si02 capacitors, and sputtered Ta metal for 300 °C A1PO devices. Figure 4.8. Current voltage curves for selected A1PO capacitor structures. A high-quality thermally oxidized Si02 dielectric in an identical structure is included for reference. Top contacts are 0.011-cm2 A1 dots thermally evaporated via shadow mask. Bottom contact is made via conductive substrate p++ Si in the case of 600 °C A1PO and Si02 capacitors, and sputtered Ta metal for 300 °C A1PO devices.
Schottky Diode Growth. The electrical properties of the films deposited using SSP 1 (Fig. 6.13) were evaluated by current versus voltage (I-V) measurements recorded for the thin films using thermally evaporated aluminum contacts (10mm2), to make Schottky barrier diodes (see Fig. 6.14). [Pg.172]


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Thermal evaporator

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