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Chapter 9: Molecular Geometry and Hybridization of Atomic Orbitals
Chapter 9: Molecular Geometry and Hybridization of Atomic Orbitals

255
255

... to compute accurate heats of reaction and enthalpies of activation. The mass-weighted steepest descent reaction paths were calculated using the method of Gonzalez and Schlegel.24,25 Ab-initio classical trajectories were integrated using the Hessian based predictor-corrector method.26,27 The Hessian ...
Quantum transport through STM-lifted single PTCDA molecules
Quantum transport through STM-lifted single PTCDA molecules

... and charge transfer, because both proceed via the extended π -electron system of the perylene backbone. At the same time, it has been shown that the Ag–O bonds have only a secondary influence on the electronic properties of the adsorbed molecule [8]. To first order, we can thus conclude that the Ag– ...
Appendix D – Raman Spectra
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... The Raman spectra for the SWNT sample at a wavelength of 785 nm and 532 nm can be found in Appendix D. For both spectra, the RBM, D-peak, and G-peak could be observed, although a considerable amount of noise was present in the spectra. At a wavelength of 785 nm, there were two peaks visible in the R ...
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... lines of various elements which may be used with higher accuracy for plasma diagnostic purposes [7]. The study of emission radiation from atoms (or ions) in plasma constitutes an important area of plasma diagnostics. From the experimental point of view, plasma is sometime optically thick to its emis ...
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... The dream of Dr. Kano (嘉納 治五郎 ) , as well known in the judo world, was to develop the traditional Kodokan (講道館) structure, along Ueshiba’s (植芝盛平) rotational way; he wasn’t able to develop his research in a rotational field due to his dead, but he paved the way to permit a natural Judo evolution with ...
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... in a metallic state.17 For the displayed XE spectra, the spectrometer counts for the excitation energy range between 529.5 and 530.4 eV were collected. This range was chosen, since this is where the largest spectral changes are observed in XAS. We thus enhance the XE signal from excited atoms that s ...
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Rotational spectroscopy



Rotational spectroscopy is concerned with the measurement of the energies of transitions between quantized rotational states of molecules in the gas phase. The spectra of polar molecules can be measured in absorption or emission by microwave spectroscopy or by far infrared spectroscopy. The rotational spectra of non-polar molecules cannot be observed by those methods, but can be observed and measured by Raman spectroscopy. Rotational spectroscopy is sometimes referred to as pure rotational spectroscopy to distinguish it from rotational-vibrational spectroscopy where changes in rotational energy occur together with changes in vibrational energy, and also from ro-vibronic spectroscopy (or just vibronic spectroscopy) where rotational, vibrational and electronic energy changes occur simultaneously.For rotational spectroscopy, molecules are classified according to symmetry into spherical top, linear and symmetric top; analytical expressions can be derived for the rotational energy terms of these molecules. Analytical expressions can be derived for the fourth category, asymmetric top, for rotational levels up to J=3, but higher energy levels need to be determined using numerical methods. The rotational energies are derived theoretically by considering the molecules to be rigid rotors and then applying extra terms to account for centrifugal distortion, fine structure, hyperfine structure and Coriolis coupling. Fitting the spectra to the theoretical expressions gives numerical values of the angular moments of inertia from which very precise values of molecular bond lengths and angles can be derived in favorable cases. In the presence of an electrostatic field there is Stark splitting which allows molecular electric dipole moments to be determined.An important application of rotational spectroscopy is in exploration of the chemical composition of the interstellar medium using radio telescopes.
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