Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Vibrational oscillator

Vibrating, oscillating. Continuous Essentially continuous Full To 250 tons/h solids... [Pg.1742]

Schwung, m. vibration, oscillation, swing soaring, flight activity momentum, -bewe-gung, /. vibratory motion, -gewicht, n. pendulum. [Pg.404]

This energy increase can take different forms. It can be added as translational kinetic energy to speed up the movement to and fro of the molecules it can be added to the rotations of the molecules to get them to spin faster it can be added to increase the amplitude of the vibrational oscillations of the molecules and it can be added to excite electrons to higher energy states in the atoms or molecules. Other forms of internal energy are also possible, but the above are the most common. [Pg.498]

The classical scheme for dichroism measurements implies measuring absorbances (optical densities) for light electric vector parallel and perpendicular to the orientation of director of a planarly oriented nematic or smectic sample. This approach requires high quality polarizers and planarly oriented samples. The alternative technique [50, 53] utilizes a comparison of the absorbance in the isotropic phase (Dj) with that of a homeotropically oriented smectic phase (Dh). In this case, the apparent order parameter for each vibrational oscillator of interest S (related to a certain molecular fragment) may be calculated as S = l-(Dh/Di) (l/f), where / is the thermal correction factor. The angles of orientation of vibrational oscillators (0) with respect to the normal to the smectic layers may be determined according to the equation... [Pg.210]

Surface nitrosyl complexes of TMI have been thoroughly investigated by the computational spectroscopy [22,23,32,33,36,49], and their molecular structure has been ascertained by a remarkable agreement between the theory and experiment of both vibrational (oscillation frequencies and intensities) and magnetic (g and A tensors) parameters. The calculated pNO values for the examined mononitrosyls along with the experimental frequencies are listed in Table 2.6. Analogous collation of the IR data for dinitrosyl species is shown in Table 2.7. [Pg.45]

One of the basic assumptions of this theory is that the polymerisation rate can be computed from the transition rate from an initial electronic state E to a final one Ef of the crystal at a given polymerisation state. The energies of these states depend on the nuclear configuration and their changes around the equilibrium positions for the initial and final electronic states can be expressed (43) in terms of vibrational oscillators which at a given temperature are either classical 1ui)c[Pg.181]

Fig. 1.5. Revivals in I2 following vibrational excitation with Lochfrass. (a) Data from experiments similar to [16]. (b) Simulations of vibrational oscillations in the I2 ground electronic state... Fig. 1.5. Revivals in I2 following vibrational excitation with Lochfrass. (a) Data from experiments similar to [16]. (b) Simulations of vibrational oscillations in the I2 ground electronic state...
The comprehensive manner by which VOA intensities relate to the details of molecular stereochemistry can be appreciated by recognizing that the set of 3N-6 vibrational degrees of freedom is defined in the same space that specifies the parameters of molecular conformation. No other form of molecular spectroscopy is so closely related to molecular stereochemistry. It is literally trae that VOA spectra arise from stereospecific vibrational oscillations of a chiral molecule. A challenge facing VOA spectroscopy at the present is how to fully extract this stractural and conformational information from the spectra. [Pg.117]

The shapes of the absorption band associated with the intensities of vibrational transitions, are sensitive functions of the equilibrium bond length, about which approximately harmonic vibrational oscillations occur. Potential energy curves for a diatomic molecule (Figure 4.2), are commonly represented by Morse equation,... [Pg.92]

The tunneling spectrum of a doped junction can be seen in Fig. 4. In this case we have an Al-A10x-4-pyridine-carboxylic acid-Ag sample, with approximately monolayer coverage, run at 1.4 K. Fig. 4a shows the modulation ( first harmonic ) voltage Vw across the junction as a function of applied bias. Since the modulation current Iu is kept constant, Vu is proportional to the dynamic resistance of the sample. The second harmonic voltage V2U ( Fig. 4b ), proportional to d V/dl, shows the vibrational spectrum of the absorbed molecules. As we shall see below, a quantity which is more closely related to the density of vibrational oscillator strengths D(r) is d I/dV. We show in Fig.4c the quantity... [Pg.220]

Fig. 1.19. Quenching of the coherent vibrational oscillations of MDMO-PPV upon photoinduced charge transfer. The AT/T dynamics for pure MDMO-PPV (continuous line) and for MDMO-PPV/PCBM (1 3 wt. ratio) (dashed line), excited by a sub-10-fs pulse, was recorded at the probe wavelength of 610 nm. The inset shows the Fourier transform of the oscillatory component of the MDMO-PPV signal, the nonresonant Raman spectrum of MDMO-PPV (excitation 1064 nm) and the resonant Raman spectrum of an MDMO-PPV/PCBM sample (excitation 457 nm). For the resonant Raman spectrum of MDMO-PPV, it was necessary to quench the strong background luminescence by adding PCBM... Fig. 1.19. Quenching of the coherent vibrational oscillations of MDMO-PPV upon photoinduced charge transfer. The AT/T dynamics for pure MDMO-PPV (continuous line) and for MDMO-PPV/PCBM (1 3 wt. ratio) (dashed line), excited by a sub-10-fs pulse, was recorded at the probe wavelength of 610 nm. The inset shows the Fourier transform of the oscillatory component of the MDMO-PPV signal, the nonresonant Raman spectrum of MDMO-PPV (excitation 1064 nm) and the resonant Raman spectrum of an MDMO-PPV/PCBM sample (excitation 457 nm). For the resonant Raman spectrum of MDMO-PPV, it was necessary to quench the strong background luminescence by adding PCBM...
A variably delayed probe pulse can be used to monitor the time-dependent vibrational oscillations and decay through coherent scattering ( diffraction ), yielding data like that shown in the simulation in Fig. 3a. In this simulation, the excitation and probe regions are overlapped spatially, and the decay of signal is due to damping and dephasing of the phonon-polariton response. From data of this form, the polariton frequency co and... [Pg.526]

The use of heterodyne detection to monitor vibrational oscillations even after traveling wave propagation out of the excitation region has also been demonstrated in the case of acoustic modes in bulk and thin... [Pg.537]

The addition of mass provides the means of transduction for many chemical sensors, including surface acoustic wave (SAW) devices, quartz crystal microbalances (QCM), and microcantilevers. In all these devices, the mass addition either perturbs the vibration, oscillations, or deflection within the transducer. The mode of transduction in an optical interferometer can also be linked to mass addition the sensor s response is altered by refractive index changes in the material being monitored. It is possible that this change can be elicited solely from refractive index changes without the addition of mass, although in sensing a particular... [Pg.96]

When you heat a crystalline solid the kinetic energy and hence the amplitude of the oscillations of the molecules increases. The material expands. As it does so the attractive force between the molecules decreases (see Chapter 8, page 208). At the melting temperature this force of attraction is not enough to keep the molecules in place and the material melts. Now the motion becomes a complex coupling of vibrational oscillations and translational movement, as holes" open up as a result of random displacements of neighbors. Clearly, there has to be enough empty space" in the material as a whole for this to occur. [Pg.319]

The dephasing processes of low frequency modes have been observed by femtosecond optical Kerr and impulsive stimulated light scattering (ISS) experiments using pulses with durations that are short compared to the period of vibrational oscillation.2 For example, the third order response from CS2 has been extensively studied by femtosecond optical Kerr and... [Pg.389]

The coherent motion initiated by an excitation pulse can be monitored by variably delayed, ultrashort probe pulses. Since these pulses may also be shorter in duration than the vibrational period, individual cycles of vibrational oscillation can be time resolved and spectroscopy of vibrationally distorted species (and other unstable species) can be carried out. In the first part of this section, the mechanisms through which femtosecond pulses may initiate and probe coherent lattice and molecular vibrational motion are discussed and illustrated with selected experimental results. Next, experiments in the areas of liquid state molecular dynamics and chemical reaction dynamics are reviewed. These important areas can be addressed incisively by coherent spectroscopy on the time scale of individual molecular collisions or half-collisions. [Pg.13]

The standing-wave vibrational oscillations are most easily detected by coherent scattering of a variably delayed probe pulse phase matched for diffraction with scattering wave vector qo. The oscillations give rise to spatial modulation of the dielectric tensor ... [Pg.14]

Optical absorption of an ultrashort pulse can lead to coherent vibrational oscillations in electronic excited states if the shapes or minima of the ground... [Pg.20]

A quantum-mechanical treatment has been given for the coherent excitation and detection of excited-state molecular vibrations by optical absorption of ultrashort excitation and probe pulses [66]. Here we present a simplified classical-mechanical treatment that is sufficient to explain the central experimental observations. The excited-state vibrations are described as damped harmonic oscillations [i.e., by Eq. (11) with no driving term but with initial condition Q(0) < 0.] We consider the effects of coherent vibrational oscillations in Si on the optical density OD i at a single wavelength k within the Sq -> Si absorption spectrum. Due to absorption from Sq to Si and stimulated emission from Si and Sq,... [Pg.22]

Figure 11. Molecular vibrational oscillations of ethyl violet in ethylene glycol solution superimposed with electronic excited-state decay. (Reprinted with permission from ref. 35.)... Figure 11. Molecular vibrational oscillations of ethyl violet in ethylene glycol solution superimposed with electronic excited-state decay. (Reprinted with permission from ref. 35.)...

See other pages where Vibrational oscillator is mentioned: [Pg.309]    [Pg.59]    [Pg.444]    [Pg.404]    [Pg.813]    [Pg.120]    [Pg.326]    [Pg.946]    [Pg.267]    [Pg.92]    [Pg.133]    [Pg.431]    [Pg.1398]    [Pg.18]    [Pg.51]    [Pg.260]    [Pg.90]    [Pg.151]    [Pg.243]    [Pg.246]    [Pg.523]    [Pg.671]    [Pg.213]    [Pg.309]    [Pg.6371]    [Pg.676]    [Pg.208]    [Pg.119]    [Pg.4]   
See also in sourсe #XX -- [ Pg.298 ]




SEARCH



Harmonic oscillator vibration treatment

Harmonic oscillator vibrational eigenfunctions

Harmonic oscillator vibrational energy levels

Harmonic oscillator vibrational energy relaxation

Harmonic oscillator vibrational states

Harmonic oscillator/vibration

Harmonic-oscillator function, hydrogen bonds bond vibrations

Oscillation Model vibration part

The Quantized Harmonic Oscillator Vibrational Spectroscopy

Vibrational states, four harmonic oscillators

Vibrational-translational relaxation harmonic oscillators

© 2024 chempedia.info