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Evaporated materials

The advantages of this technique are that they are applicable to probes in ultra high vacuum, where any impurities are excluded, and also to samples at atmospheric pressure. The diameter of the evaporated cavity can be varied between 10 jam and 1 mm, and the quantity of the evaporated material may be less than 10" g. Solids in any desired form, crystalline or powered, are accessible to analysis. [Pg.57]

Photoelectron spectroscopy has been used to study equilibria in the gas phase. Thus, the taut-omerism of triazoline-5-thione is studied by variable temperature photoelectron spectroscopy <83CJC1197). PhotoeleCtron spectra of 1,2-dimethyltriazoline-5-thione (67a) calibrated with the Pi/2 and Ps/2 lines of argon and xenon are recorded with a resolution of 30 meV. The spectra of freshly evaporated material obtained with a Pj probe indicate the presence of the unchanged thione even at 160 °C. A spectrum recorded with a P2 probe after heating the evaporated sample to 160 °C exhibits an additional minor band at 9.40 eV which is most likely due to 2-methyl-4-methylthiotriazole (67b). [Pg.22]

One of the most serious shortcomings of the HV pulse atom-probe is the inability to pulse field evaporate materials of very low electrical conductivity such as a high purity silicon. This is due to the difficulty of transmitting ns HV pulses across the tip. This limitation is overcome by the use of laser pulses which can be focused right to the tip apex. Thus the material applicability of the atom-probe is greatly expanded by the use of laser pulses for the pulsed-field evaporation. [Pg.141]

All evaporating material is intercepted by the hemisphere, because the molecular beam exists only at angles less than 90° from the center line. Therefore, the mass flow from the source must equal the flux of the molecular beam leaving the control volume across the surface of the hemisphere. Under these conditions, the mass flow from the source is given by... [Pg.190]

Using an electron beam which is guided onto the material by an electromagnetic field. Using electron beam evaporation materials with high melting points which are difficult to evaporate can also be deposited. [Pg.153]

E-beam Evaporation Modern machines increasingly use electron-beam evaporators. In this process an e-beam is focused on the evaporation material which, as a result of the energy input from the beam, is heated and evaporates (Fig. 8.2). [Pg.184]

E-beam evaporators have the benefit of higher evaporation temperatures than resistance evaporators and it is also possible to evaporate materials, for example Ni, B, and Co, which alloy or react chemically when using resistance evaporators [3], A disadvantage of e-beam evaporators is that substantially more complex instrumentation is required for process control. [Pg.185]

Vacuum Contamination of the A1 layer by residual gas components (mainly water vapor) affects the barrier substantially good vacuum (<5 x 104 mbar) in the evaporation chamber is therefore required for barrier applications. Contamination from the evaporation material and the evaporators must also be avoided as much as possible. [Pg.196]

Bigger clusters have been formed, for instance, by the expansion of laser evaporated material in a gas still under vacuum. For metal-carbon cluster systems (including M C + of Ti, Zr and V), their formation and the origin of delayed atomic ions were studied in a laser vaporization source coupled to a time-of-flight mass spectrometer. The mass spectrum of metal-carbon cluster ions (TiC2 and Zr C j+ cluster ions) obtained by using a titanium-zirconium (50 50) mixed alloy rod produced in a laser vaporization source (Nd YAG, X = 532 nm) and subsequently ionized by a XeCl excimer laser (308 nm) is shown in Figure 9.61. For cluster formation, methane ( 15% seeded in helium) is pulsed over the rod and the produced clusters are supersonically expanded in the vacuum. The mass spectrum shows the production of many zirconium-carbon clusters. Under these conditions only the titanium monomer, titanium dioxide and titanium dicarbide ions are formed. [Pg.448]

The effect of volatility in fractionating elements is due to the ratio of the saturation vapor pressures, but as shown by Equation (6), the relative masses of the gas species and possible differences in the evaporation coefficients also affect the degree of chemical fractionation produced by evaporation. When Equation (6) is used in connection with isotope fractionation, it is generally assumed that isotopes of the same element have the same evaporation coefficient and that the ratio of the saturation vapor pressures is equal to the isotopic ratio at the surface of the evaporating material (i.e., no equilibrium fractionation). This results in the following equation for the relative flux of the isotopes ... [Pg.412]

In variance to these expectations, after depositing Ir on Cu( 100) at a sample temperature of 200 K, the corresponding ISS measurements display immediately an apparent lack of evaporated material at the surface (Fig. 9). The... [Pg.378]

Drying is the process by which volatile materials, usually water, are evaporated from a material to yield a sohd product. Drying is a heat-ancf mass-transfer process. Heat is necessary to evaporate water. The latent heat of vaporization of water is about 2500 J/g, which means that the drying process requires a significant amount of energy. Simultaneously, the evaporating material must leave the drying material by diffusion and/or convection. [Pg.1347]

Compressed and extruded products from biomass residues represent a high level of material preparation and processing. Wet residues must be mixed with dry residues or excess moisture evaporated. Materials must be ground to a minimum size. Mixing, conveying and feeding materials to a press or extruder must be carefully organized. [Pg.187]

Kondakov et al. have reported the analysis by high performance liquid chromatography of degradation products of a phosphorescent OLED based on evaporable materials [221]. This work has inspired confidence in using... [Pg.178]

The high purity of the caustic soda obtained by the membrane process eliminates the need for a caustic soda evaporator in cases where it is to be supplied to customers such as pulp mills which utilize a dilute caustic soda. This is in marked contrast to the diaphragm process which inevitably requires evaporation to separate sodium chloride. For the general trade, in which caustic soda at 50% concentration is required, a conventional multiple effect evaporator is generally utilized to concentrate the catholyte. Caustic soda from the membrane process contains a very slight amount of sodium chloride which does not cause corrosion of the evaporator materials or precipitation of sodium chloride, and thus allows easier and more stable evaporator operation than in the diaphragm process. [Pg.393]


See other pages where Evaporated materials is mentioned: [Pg.179]    [Pg.184]    [Pg.348]    [Pg.516]    [Pg.129]    [Pg.180]    [Pg.101]    [Pg.115]    [Pg.575]    [Pg.208]    [Pg.516]    [Pg.45]    [Pg.304]    [Pg.448]    [Pg.588]    [Pg.179]    [Pg.184]    [Pg.348]    [Pg.192]    [Pg.193]    [Pg.108]    [Pg.162]    [Pg.45]    [Pg.304]    [Pg.264]    [Pg.158]    [Pg.412]    [Pg.419]    [Pg.723]    [Pg.666]    [Pg.389]    [Pg.183]    [Pg.116]    [Pg.14]    [Pg.194]   
See also in sourсe #XX -- [ Pg.337 ]




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