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And vibration-rotation bands

C. G. Joslin, C. G. Gray, and S. Goldman, Chem. Phys. Lett., 227, 405 (1994). Infrared Rotation and Vibration-Rotation Bands of Endohedral Fullerene Complexes. Helium in C60-Derived Nanotubes. [Pg.298]

The ideas fundamental to an understanding of infrared spectroscopy were introduced in this chapter. The electromagnetic spectrum was considered in terms of various atomic and molecular processes and classical and quantum ideas were introduced. The vibrations of molecules and how they produce infrared spectra were then examined. The various factors that are responsible for the position and intensity of infrared modes were described. Factors such as combination and overtone bands, Fermi resonance, coupling and vibration-rotation bands can lead to changes in infrared spectra. An appreciation of these issues is important when... [Pg.12]

Infrared absorption properties of 2-aminothiazole were reported with those of 52 other thiazoles (113). N-Deuterated 2-aminothiazole and 2-amino-4-methylthiazo e were submitted to intensive infrared investigations. All the assignments were performed using gas-phase studies of the shape of the vibration-rotation bands, dichroism, isotopic substitution, and separation of frequencies related to H-bonded and free species (115). With its ten atoms, this compound has 24 fundamental vibrations 18 for the skeleton and 6 for NHo. For the skeleton (Cj symmetry) 13 in-plane vibrations of A symmetry (2v(- h, 26c-h- Irc-N- and 7o)r .cieu.J and... [Pg.23]

The distinction between in-plane A symmetry) and out-of-plane (A" symmetry) vibrations resulted from the study of the polarization of the diffusion lines and of the rotational fine structure of the vibration-rotation bands in the infrared spectrum of thiazole vapor. [Pg.54]

The out-of-plane vibrations of thiazole correspond to C-type vibration-rotation bands and the in-plane vibrations to A, B, or (A + B) hybrid-type bands (Fig, 1-9). The Raman diffusion lines of weak intensity were assigned to A"-type oscillations and the more intense and polarized lines to A vibration modes (Fig. I-IO and Table 1-23). [Pg.54]

Suites 1 to VIII contain infrared frequencies corresponding to vibration-rotation bands of A, B, or (A-l-B) hybrid types and can thus be assigned to vibrations of A symmetry the corresponding Raman lines are generally polarized. [Pg.66]

The frequencies classified in suites IX and X belong to depolarized Raman lines and correspond to vibrations-rotation bands of the C type. They can be assigned to oscillations of A" symmetry. [Pg.66]

More usual is the kind of vibration-rotation band shown in Figure 6.8. This spectmm was obtained with an interferometer having a resolution of 0.5 cm and shows the v= 1-0... [Pg.148]

Assignments. - Electric modulation of vibrational rotational bands of polar molecules included a study of phosphine.120 Ringbending (puckering) transition frequencies have been measured for the phospholene (42) for the ground and excited states.121 The PD deformation band for the sulphide (43) has been assigned.122... [Pg.405]

Herman, R., and Wallis, R. F. (1955), Influence of Vibration-Rotation Interaction on Line Intensities in Vibration-Rotation Bands of Diatomic Molecules, 7. Chem. Phys. 23, 637. [Pg.227]

It is well established that the average lengths of CH bonds are consistently 0.003 to 0.004 A longer than the corresponding CD bonds in the ground vibrational state (see Fig. 12.1, its caption, and Section 12.2.3). It remains only to establish the dipole moment derivative, (9p/9r), at the equilibrium bond length. That is available from theoretical calculation or spectroscopic measurement (via precise measurements of IR intensities of vibration-rotation bands). Calculations based on Equation 12.7 yield predicted dipole moment IE s in reasonable agreement with experiment. [Pg.395]

Figure 10.6—Vibrational-rotational bands of carbon monoxide (P = 1000 Pa). The various lines illustrate the principle of the selection rules (see Fig. 10.7). In this case, AV = +1 and AJ = 1. Branch R can be seen on the left-hand side of the spectrum while branch P is on the right. The distance between the rotational bands allows the moment of inertia I of the molecule to be calculated. I is not constant due to the anharmonicity factor. Figure 10.6—Vibrational-rotational bands of carbon monoxide (P = 1000 Pa). The various lines illustrate the principle of the selection rules (see Fig. 10.7). In this case, AV = +1 and AJ = 1. Branch R can be seen on the left-hand side of the spectrum while branch P is on the right. The distance between the rotational bands allows the moment of inertia I of the molecule to be calculated. I is not constant due to the anharmonicity factor.
Figure 10.7—Representation of the rotational and vibrational energy levels and conversion into the vibrational rotational spectrum (at bottom). The fundamental vibration corresponds to V = +1 and J ll-The vibrational rotational band corresponds to all the allowed quantum leaps. If the scale of the diagram is in cm-1 the arrows correspond to the wavenumbers of absorption. The R branch corresponds to A J = +1 and the P branch to A J = -1. They are located on each side of the Q band, which is absent in the spectrum (AJ = 0 corresponds, here, to a forbidden transition). Figure 10.7—Representation of the rotational and vibrational energy levels and conversion into the vibrational rotational spectrum (at bottom). The fundamental vibration corresponds to V = +1 and J ll-The vibrational rotational band corresponds to all the allowed quantum leaps. If the scale of the diagram is in cm-1 the arrows correspond to the wavenumbers of absorption. The R branch corresponds to A J = +1 and the P branch to A J = -1. They are located on each side of the Q band, which is absent in the spectrum (AJ = 0 corresponds, here, to a forbidden transition).
R. Krech, G. Caledonia, S. Schertzer, K. Ritter, T. W. Wilkerson, L. Cotnoir, R. Taylor, and G. Birnbaum. Laboratory observation of collision induced emission in the fundamental vibration rotation band of H2. Phys. Rev. Lett., 49 1913, 1982. [Pg.416]

Fig. 43) Rotational fine structure of a vibration-rotation band of a diatomic molecule. Note the decreasing spacing with increasing / in the R branch, and the increasing spacing with increasing / in the P branch. Fig. 43) Rotational fine structure of a vibration-rotation band of a diatomic molecule. Note the decreasing spacing with increasing / in the R branch, and the increasing spacing with increasing / in the P branch.
Analysis of the rotational fine structure of IR bands yields the moments of inertia 7°, 7°, and 7 . From these, the molecular structure can be fitted. (It may be necessary to assign spectra of isotopically substituted species in order to have sufficient data for a structural determination.) Such structures are subject to the usual errors due to zero-point vibrations. Values of moments of inertia determined from IR work are less accurate than those obtained from microwave work. However, the pure-rotation spectra of many polyatomic molecules cannot be observed because the molecules have no permanent electric dipole moment in contrast, all polyatomic molecules have IR-active vibration-rotation bands, from which the rotational constants and structure can be determined. For example, the structure of the nonpolar molecule ethylene, CH2=CH2, was determined from IR study of the normal species and of CD2=CD2 to be8... [Pg.387]

The shape of the vibration-rotation bands in infrared absorption and Raman scattering experiments on diatomic molecules dissolved in a host fluid have been used to determine2,15 the autocorrelation functions unit vector pointing along the molecular axis and P2(x) is the Legendre polynomial of index 2. These correlation functions measure the rate of rotational reorientation of the molecule in the host fluid. The observed temperature- and density-dependence of these functions yields a great deal of information about reorientation in solids, liquids, and gases. These correlation functions have been successfully evaluated on the basis of molecular models.15... [Pg.6]

Most atmospheric visible and DV absorption and emission involves energy transitions of the outer electron shell of the atoms and molecules involved. The infrared spectrum of radiation from these atmospheric constituents is dominated by energy mechanisms associated with the vibration of molecules. The mid-infrared region is rich with molecular fundamental vibration-rotation bands. Many of the overtones of these bands occur in the near infrared. Pure rotation spectra are more often seen in the far infrared. Most polyatomic species found in the atmosphere exhibit strong vibration-rotation bands in the 1 - 25 yin region of the spectrum, which is the region of interest in this paper. The richness of the region for gas analysis... [Pg.217]


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Rotating band

Rotation bands

Rotation-vibration

Rotational vibrations

Rotational-vibrational

Vibrating rotator

Vibrational bands

Vibrational, rotational, and

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