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Production of Atoms

Production of F Pj atoms can also be achieved by microwave dissociation of fluorides such as SFs and CF4. These sources are satisfactory for spectroscopic studies such as the e.p.r. spectroscopy of F and F or for the formation of excited BrF and IF from the recombination of Br + F or I + F in the presence of singlet oxygen. However, they are in some degree suspect for stematic quantitative kinetic studies. The nature and reactivity of the discharge products other than F Pj are very incompletely known. [Pg.241]

In principle, a cleaner source of F P, atoms than any of the preceding ones is the rapid reaction of N S atoms with NF2 radicals produced by thermolysis of N2F4. This reaction occurs either directly to give F atoms [Pg.241]

It is a curious (but useful) observation that a flow of CO radicals, formed by Cl + OCO or Cl + O3, acts as an excellent agent for inhibiting wall recombination of Cl atoms. [Pg.242]

Alternative techniques for producing Cl Pj atoms have been described. The reaction of excess O atoms with OCIO has been used to produce known concentrations of Cl Pj atoms for the calibration of C-atom resonance fluorescence intensity as a function of the concentration of C atom. The following reaction stoicheiometry was used  [Pg.242]

The reaction Cl + OCIO - 2C10 also occurs, but this does not affect the Cl atom stoicheiometry. Another approach is to use the slow reaction between O Pj atoms and an excess of molecular Cl2  [Pg.242]


Production of atomic hydrogen as a species this may penetrate metal to produce blistering or embrittlement. [Pg.55]

Instead of employing the high temperature of a flame to bring about the production of atoms from the sample, it is possible in some cases to make use of either (a) non-flame methods involving the use of electrically heated graphite tubes or rods, or (b) vapour techniques. Procedures (a) and (b) both find applications in atomic absorption spectroscopy and in atomic fluorescence spectroscopy. [Pg.787]

Similarly, cocondensation of Cu and C2H4 or Cu and C2H4 Ar at 10-12 K under conditions that favor the production of atomic Cu leads to formation of Cu(C2H4) (n = 1-3). When this product is annealed at 30-45 K, binuclear derivatives form ... [Pg.496]

Bond strengths are essentially controlled by valence ionization potentials. In the well established extended Hiickel theory (EHT) products of atomic orbital overlap integrals and valence ionization potentials are used to construct the non-diagonal matrix elements which then appear in the energy eigenvalues. The data in Table 1 fit our second basic rule perfectly. [Pg.82]

We have divided the discussion into three principal areas. The first two sections deal with the production of atomic hydrogen species in gaseous and liquid environments the third is really a collage of experimental observations and unintentional introduction techniques that are generally of less interest from the viewpoint of a manufacturing technologist. [Pg.33]

The production of atoms is a common critical requirement of all these techniques and there are various devices that can be used to generate the atoms in analytically useful spectroscopic states. The following schema summarizes the processes that occur during atomization ... [Pg.239]

Because the interactions measured in Mossbauer experiments are products of atomic and nuclear factors, experiments on iodine isotopes have yielded values of the change of nuclear radius between the ground state and the excited state, AR/R, quadrupole moment values Q, and magnetic moment values, fi, as well as electric field gradients and internal magnetic fields. [Pg.127]

In addition to the physical interactions described above, the tip may also be used to alter the local chemical conditions within the tunnel junction. For example, catalytic rehydrogenation of carbonaceous fragments on Pt(lll) by tip-directed production of atomized hydrogen in vacuum at the Pt-Ir tip has been described [524]. Similar modification schemes may also be envisioned based on limiting the transport of reactants and products into or away from the partly occluded tunnel junction. As noted earlier, such effects may be important in the study of electrodeposition and etching process [126-131]. Nonetheless, much remains to be understood about the detailed physics and chemistry of the immersed tunnel junction. [Pg.291]

The deformation functions, however, must also describe density accumulation in the bond regions, which in the one-center formalism is represented by the atom-centered terms. They must be more diffuse, with a different radial dependence. Since the electron density is a sum over the products of atomic orbitals, an argument can be made for using a radial dependence derived from the atomic orbital functions. The radial dependence is based on that of hydrogenic orbitals, which are valid for the one-electron atom. They have Slater-type radial functions, equal to exponentials multiplied by r1 times a polynomial of degree n — l — 1 in the radial coordinate r. As an example, the 2s and 2p hydrogenic orbitals are given by... [Pg.64]

The coefficients n, have to obey the condition n, f, imposed by Poisson s electrostatic equation, as pointed out by Stewart (1977). The radial dependence of the multipole density deformation functions may be related to the products of atomic orbitals in the quantum-mechanical electron density formalism of Eq. (3.7). The ss, sp, and pp type orbital products lead, according to the rules of multiplication of spherical harmonic functions (appendix E), to monopolar, dipolar, and quadrupolar functions, as illustrated in Fig. 3.6. The 2s and 2p hydrogenic orbitals contain, as highest power of r, an exponential multiplied by the first power of r, as in Eq. (3.33). This suggests n, = 2 for all three types of product functions of first-row atoms (Hansen and Coppens 1978). [Pg.65]

Section treats the spatial, angular momentum, and spin symmetries of the many-electron wavefunctions that are formed as antisymmetrized products of atomic or molecular orbitals. Proper coupling of angular momenta (orbital and spin) is covered here, and atomic and molecular term symbols are treated. The need to include Configuration Interaction to achieve qualitatively correct descriptions of certain species electronic structures is treated here. The role of the resultant Configuration Correlation Diagrams in the Woodward-Hoffmann theory of chemical reactivity is also developed. [Pg.3]

The first line describes production of atoms X from a fixed reservoir A at a constant rate aQ. The macroscopic equations are... [Pg.263]

The production of atomic hydrogen by the Hg(3P,) sensitized reaction has been known for many years and the reaction has been used as a clean source of H atoms. Two processes have been postulated without direct evidence of the primary products... [Pg.156]

Models for the electronic structure of polynuclear systems were also developed. Except for metals, where a free electron model of the valence electrons was used, all methods were based on a description of the electronic structure in terms of atomic orbitals. Direct numerical solutions of the Hartree-Fock equations were not feasible and the Thomas-Fermi density model gave ridiculous results. Instead, two different models were introduced. The valence bond formulation (5) followed closely the concepts of chemical bonds between atoms which predated quantum theory (and even the discovery of the electron). In this formulation certain reasonable "configurations" were constructed by drawing bonds between unpaired electrons on different atoms. A mathematical function formed from a sum of products of atomic orbitals was used to represent each configuration. The energy and electronic structure was then... [Pg.27]

For the transition state, of course, one of the 3 N — 6 vibrations is really a translation for the moment we single it out and write for its frequency ratio vj.nlvf.r>. When Equation A2.11 is substituted into Equation A2.10, the products of atomic masses will cancel, leaving Equation A2.12 ... [Pg.122]

Absorption of electromagnetic radiation by monatomic gases leads either to production of atoms in excited states or, if the wavelength is short enough, to ionization. Absorption lines have widths which depend on the following factors1 (a) the temperature, i.e. there will be a Doppler effect which will broaden the line if the absorbing atoms are in motion (b) an intrinsic factor dependent on the nature of the electronic state and on the extent of perturbations by other states ... [Pg.2]

Out of a number of experiments in recent years on the impact, of electrons with hydrogen molecules, there come certain results which at first sight appear discordant. On the one hand the experiments on ionization show that an electron, when it ionizes a hydrogen molecule, does so without causing dissociation. That is, the production of atomic ions as the primary result of impact of moderate. speed electrons with hydrogen molecules is a process which occurs rarely if at all. On the other hand,... [Pg.1]


See other pages where Production of Atoms is mentioned: [Pg.84]    [Pg.332]    [Pg.627]    [Pg.271]    [Pg.84]    [Pg.82]    [Pg.78]    [Pg.51]    [Pg.1]    [Pg.11]    [Pg.179]    [Pg.9]    [Pg.49]    [Pg.501]    [Pg.9]    [Pg.720]    [Pg.76]    [Pg.4]    [Pg.11]    [Pg.57]    [Pg.501]    [Pg.367]    [Pg.2]    [Pg.2]    [Pg.19]    [Pg.11]   


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Production of excited states in atoms

Production of the Atomic Vapor

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