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Radio frequency and microwave

A large number of CVD diamond deposition technologies have emerged these can be broadly classified as thermal methods (e.g., hot filament methods) and plasma methods (direct current, radio frequency, and microwave) [79]. Film deposition rates range from less than 0.1 pm-h to 1 mm-h depending upon the method used. The following are essential features of all methods. [Pg.16]

Similar to the principles of optics, materials interact with radio frequency and microwave radiation in three ways they reflect radiation impinging upon them, they transmit radiation, and finally absorb some of the energy which is being transmitted through them. [Pg.213]

There are basically two forms of dielectric heating radio-frequency and microwave. Radio-frequency heating uses a frequency (13 to 100 MHz) to generate heat in polar materials. The electrodes are generally designed into the platens of a press, and they are... [Pg.276]

We shall calculate the matrix elements of the effective Hamiltonian within the basis of these six primitive states in due course. These states do not, however, have definite parities. Since parity is conserved (except in the presence of an applied electric field), we construct a basis set of six functions, three of each parity type, so that for a given J level we are left with the diagonalisation of 3 x 3 matrices, rather than 6x6. More importantly, we are aiming to understand the electric dipole radio frequency and microwave spectra, and know that transitions must occur between states of opposite parity. [Pg.512]

Furthermore it remains to be pointed out that many molecules of potential astrophysical interest have been sought in interstellar clouds but have not been found. Some of the notable negative results include cyclic molecules and NO, H2C20 and others. However, at the present time it seems premature to draw definite conclusions since the detection limits are barely below the expected line intensities. We may note that CH4 which is expected to exist in interstellar space (Section IV) has no allowed pure rotational spectrum. However, Dorney and Watson (1972) have shown that a centrifugally induced dipole moment exists which produces a complicated forbidden rotational spectrum in the radio frequency and microwave regions. The particular transitions are very weak and have not yet been observed in the laboratory. [Pg.40]

Both CO2-HF and CO2-HCI complexes were first examined in the gas phase by Klemperer and co-workers, using the molecular beam electric resonance technique, with the radio-frequency and microwave spectra of CO2-HF and CO2-HCI indicating nearly linear, hydrogen-bonded structures [35, 36], Accurate determinations of rotational constants allowed the separations between the centers-of-mass of each sub-unit to be obtained, and assuming that neither CO2 nor HX underwent intramolecular change, the O—H bond lengths could be estimated for each complex. A comparison of CO2-HF and CO2-HCI showed the O—H separation in the former to be 10% less than in the latter. Equilibrium structures for CO2-HF and CO2HCI are shown in Fig. 10, and Table 1 lists structural parameters for all known CO2-HX complexes. [Pg.268]

Field Effects Drying—Drying with Infrared, Radio-Frequency, and Microwave Methods... [Pg.1426]

Following the war, other new and important methods for radio frequency and microwave spectroscopy were introduced. In 1946 Purcell, Torrey and Poimd [12] and Bloch, Hansen and Packard [13] at radio frequencies developed the nuclear magnetic resonance absorption and induction methods that later came to be known as NMR and provided the basis NMR chemical analysis and for magnetic resonance imaging (MRI). [Pg.12]

Radio Frequency and Microwave Radiation Light Energy Radiation Light Source Photoinitiators... [Pg.839]

If the source is monochromatic or nearly so, or if the source is monochromatic and tunable, then very high resolution is possible, providing the frequency stability of the source is good. Tunable sources have been available for some time in the radio-frequency and microwave regions of the spectrum, but it is only recently that tunable lasers have become available in the infrared and visible regions. [Pg.151]

In GC-AED, the GC eluent stream is directly introduced into the plasma of an atomic emission spectrometer. The helium GC gas readily mixes with the hehum or argon plasma that is normally used. This plasma is maintained in the plasma state at high energy through the use of several types of energy. Both AC and DC arcs have been used, as well as radio frequency and microwave radiation. Micro-wave plasmas are most common in commercial GC-AED instruments. Often volumes of reagent gases or a make-up gas are added to ensure optimum atomization of the molecules by the plasma. [Pg.1016]


See other pages where Radio frequency and microwave is mentioned: [Pg.140]    [Pg.237]    [Pg.190]    [Pg.187]    [Pg.35]    [Pg.411]    [Pg.403]    [Pg.172]    [Pg.190]    [Pg.1323]    [Pg.1426]    [Pg.105]    [Pg.3]    [Pg.5]    [Pg.12]    [Pg.13]    [Pg.14]    [Pg.15]    [Pg.845]    [Pg.1322]    [Pg.1425]    [Pg.271]    [Pg.105]    [Pg.14]    [Pg.763]    [Pg.770]    [Pg.789]    [Pg.510]    [Pg.335]   


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And microwaves

Radio, radios

Radio-frequency

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