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Atomic Spectroscopy Explained

Light is emitted as electron falls back to lower energy level. [Pg.318]

Electron absorbs energy and is excited to rmstable energy level. [Pg.318]

For example, suppose that an electron in a hydrogen atom relaxes from an orbital in the n = 3 level to an orbital in the n = 2 level. Then AE, the energy difference corresponding to the transition from n = 3 to n = 2, is determined as follows  [Pg.319]

The energy carries a negative sign because the atom emits the energy as it relaxes from n = 3 to n = 2. Since energy must be conserved, the exact amount of energy emitted by the atom is carried away by the photon  [Pg.319]

This energy then determines the frequency and wavelength of the photon. Since the wavelength of the photon is related to its energy as E = he/, we calculate the wavelength of the photon as  [Pg.319]


We are now ready to build a quantum mechanical model of a hydrogen atom. Our task is to combine our knowledge that an electron has wavelike properties and is described by a wavefunction with the nuclear model of the atom, and explain the ladder of energy levels suggested by spectroscopy. [Pg.145]

The observation of atomic spectra stimulated physicists in the early 19th century to develop the theory of quantum mechanics. This theory sets out to explain all physical phenomena at an atomic scale and atomic spectroscopy is an important validation. Quantum mechanics is flawed, however, notably in the description of gravity, but it is the best theory at present (although super string theory promises well) for the description of the structure of nuclei, atoms and molecules. [Pg.41]

The term exp(-2k2c ) in (6-9) accounts for the disorder of the solid. Static disorder arises if atoms of the same coordination shell have slightly different distances to the central atom. Amorphous solids, for instance, possess large static disorder. Dynamic disorder, on the other hand, is caused by lattice vibrations of the atoms, as explained in Appendix 1. Dynamic disorder becomes much less important at lower temperatures, and it is therefore an important advantage to measure spectra at cryogenic temperatures, especially if a sample consists of highly dispersed particles. The same argument holds in X-ray and electron diffraction, as well as in Mossbauer spectroscopy. [Pg.170]

In analytical atomic spectroscopy, how are atomic populations usually formed from solutions In your answer, include an outline of the conventional apparatus and basic processes involved, and explain how the atomic or ionic population may be maximized. [Pg.158]

When applied to hydrogen, Bohr s theory worked well when atoms with more electrons were considered, the theory failed. Complications such as elliptical rather than circular orbits were introduced in an attempt to fit the data to Bohr s theory. The developing experimental science of atomic spectroscopy provided extensive data for testing of the Bohr theory and its modifications and forced the theorists to work hard to explain the spectroscopists observations. In spite of their efforts, the Bohr theory eventually proved unsatisfactory the energy levels shown in Figure 2-2 are valid only for the hydrogen atom. An important characteristic of the electron, its wave nature, still needed to be considered. [Pg.19]

In previous work we have shown how this embedding of the icosahedron in can be used to resolve the product multiplicity in the icosahedral H (g + 2h) Jahn-Teller problem [10,20]. In the context of atomic spectroscopy, Judd and Lo have made use of the connection to explain some puzzling degeneracies in the... [Pg.42]

A huge effort is made by theoreticians to explain the discrepancies between the experimental values and the theoretical values, based upon the fundamental relation of atomic spectroscopy. This rather complicated process to calculate corrections that can be applied to experimental results to duplicate the experimental value of Roo is briefly summarized in Sect. 4. However, it is shown below that the origin of the problem is found in the fact that the fundamental relation of atomic spectroscopy is almost but not quite adequate to agree with the experimental facts. No amount of corrections can salvage an incorrect equation. [Pg.58]

In its more recent phase of development, the multidisciplinary nature of metal-vapor cryochemistry is becoming evident with, for example, chemical physicists attempting to explain subtle, spectroscopic phenomena associated with matrix-entrapped, metal atomic species (75-77). A clear display of renewed physics interest in the field may be seen from a glance at the proceedings of the International Conference of Matrix Isolation Spectroscopy (Ber. Bunsenges. Phys. Chem., January, 1978). In addition, matrix reactions are providing unique, syn-... [Pg.80]

Techniques other than UV-visible spectroscopy have been used in matrix-isolation studies of Ag see, for example, some early ESR studies by Kasai and McLeod 56). The fluorescence spectra of Ag atoms isolated in noble-gas matrices have been recorded (76,147), and found to show large Stokes shifts when optically excited via a Si j — atomic transition which is threefold split in the matrix by spin-orbit and vibronic interactions. The large Stokes shifts may be explained in terms of an excited state silver atom-matrix cage complex in this... [Pg.95]


See other pages where Atomic Spectroscopy Explained is mentioned: [Pg.318]    [Pg.318]    [Pg.564]    [Pg.264]    [Pg.564]    [Pg.28]    [Pg.32]    [Pg.24]    [Pg.669]    [Pg.220]    [Pg.130]    [Pg.11]    [Pg.54]    [Pg.191]    [Pg.82]    [Pg.353]    [Pg.120]    [Pg.1]    [Pg.440]    [Pg.444]    [Pg.300]    [Pg.833]    [Pg.781]    [Pg.16]    [Pg.28]    [Pg.8]    [Pg.139]    [Pg.169]    [Pg.245]    [Pg.255]    [Pg.221]    [Pg.788]    [Pg.169]    [Pg.77]    [Pg.81]    [Pg.337]    [Pg.91]    [Pg.57]    [Pg.265]    [Pg.70]   


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Atomic spectroscopy

Explained

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