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The Molecule and Spectra

The barrier to rotation of CH3 groups, V 5.0 kJ/mol, was first estimated from a correlation between barrier contributions of other groups and the minimum internuclear distance for various organic compounds (using d(Ge-C) = 1.98 A) [3]. Very low values based on H NMR relaxation measurements (2.7 kJ/mol) [34] and experimental and calculated entropies (3.1 kJ/ mol) [57] cannot be correct see also [90, p. 19]. Consistent values for solid Ge(CH3)4 have been obtained from far-infrared studies [52], neutron scattering [80,90,91], and proton Zeeman spin-lattice relaxation experiments [94] (barrier height V and torsional ground level Eq in [Pg.24]

Reported ionization energies from electron impact studies range from 9.2 to 9.6 eV except for an earlier unusual value (11.2 eV) in [40]  [Pg.25]

Ionization energies (in eV) from He(l) photoelectron spectra are listed below along with assignments based on a qualitative MO energy level scheme [65] and semiempirical calculations and extrapolations within the series of M(CH3)4 compounds for M = C to Pb [66]  [Pg.25]

The electron attachment energy of 3.7 eV has been obtained by electron transmission spectroscopy (temporary formation of a negative ion by interaction with an electron beam) for the series of M(CH3)4 compounds with M = C, Si, Ge, and Sn these energies decrease progressively [105]. [Pg.25]

The relaxation energies Er = —1.62 eV for Ge 3p3/2 and Er = —8.33 eV for C Is and atomic charges from an electronegativity equalization procedure have been used to calculate binding [Pg.25]


In an emission spectrum a fixed wavelength is used to excite the molecules, and the intensity of emitted radiation is monitored as a function of wavelength. Although a molecule has only a single excitation spectrum, it has two emission spectra, one for fluorescence and one for phosphorescence. The corresponding emission spectra for the hypothetical system in Figure 10.43 are shown in Figure 10.44. [Pg.427]

In this method, photons of an energy well in excess of the ionization potential are directed onto a molecule. The photoelectron spectrum which results allows assessment of the energies of filled orbitals in the molecule, and thus provides a characterization of a molecule. Comparisons between photoelectron spectra of related compounds give structural information, for example, on the tautomeric structure of a compound by comparison of its spectrum with those of models of each of the fixed forms. [Pg.30]

The main mass fragmentation of secobenzylisoquinoline alkaloids involves bond cleavage between the two benzylic carbonyls. This process is evidenced by the presence of peaks representing fragment ions at m/z 151, found in spectra of all these bases and attributed to the lower portion of the molecules, and ions at m/z 220,236, and 222, found in spectra of 159,160, and 161, respectively, formed from the upper part of the compounds. Similarly, as in the mass spectra of other secoisoquinoline alkaloids incorporating the amino-ethyl substituent, the [H2C=N(CH3)2]+ ion at mjz 58 is the base peak. [Pg.280]

Most of what we know about the structure of atoms and molecules has been obtained by studying the interaction of electromagnetic radiation with matter. Line spectra reveal the existence of shells of different energy where electrons are held in atoms. From the study of molecules by means of infrared spectroscopy we obtain information about vibrational and rotational states of molecules. The types of bonds present, the geometry of the molecule, and even bond lengths may be determined in specific cases. The spectroscopic technique known as photoelectron spectroscopy (PES) has been of enormous importance in determining how electrons are bound in molecules. This technique provides direct information on the energies of molecular orbitals in molecules. [Pg.83]

The excitation spectrum of a molecule is similar to its absorption spectrum, while the fluorescence and phosphorescence emission occur at longer wavelengths than the absorbed light. The intensity of the emitted light allows quantitative measurement since, for dilute solutions, the emitted intensity is proportional to concentration. The excitation and emission spectra are characteristic of the molecule and allow qualitative measurements to be made. The inherent advantages of the techniques, particularly fluorescence, are ... [Pg.28]

IR spectroscopy is useful for the identification of some of the functional groups in an organic molecule. The technique also provides a fingerprint of the molecule and its comparison with authentic specimen often confirms the structure of that molecule. The IR spectra of AHLs show characteristic absorption peaks at 1780,1710,1650 cm-1 arising from the lactone ring, 3-oxo (when present), and amide carbonyl, respectively [15,16]. [Pg.304]

The electron coupled interaction of nuclear magnetic moments with themselves and also with an external magnetic field is responsible for NMR spectroscopy. Since the focus of this study is calculation of NMR spectra within the non-relativistic framework, we will take a closer look at the Hamiltonian derived from equation (76) to describe NMR processes. In this regard, we retain all the terms, which depend on nuclear magnetic moments of nuclei in the molecule and the external magnetic field through its vector potential in addition to the usual non-relativistic Hamiltonian. The result is... [Pg.460]

It is important to note that even without hyperfine data, the powder spectra give valuable information about the carrier of the ESR spectrum. Both the molecular symmetry of the molecule and the effective distance between the unpaired electrons usually can be deduced from the spectra. [Pg.172]


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