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Principles of Vibrational Spectroscopy

Infrared spectroscopy is based on the phenomenon of infrared absorption by molecular vibrations. When a molecule is irradiated by electromagnetic waves within the infrared frequency range, one particular frequency may match the vibrational frequency of the molecule Consequently, the molecular vibration will be excited by waves with the frequency vph = vvif,. The excitation means that the energy of molecular vibration will increase, normally by Av = +1, as shown in Equation 9.7. In the meantime, the electromagnetic radiations with the specific frequency vph will be absorbed by the molecule because the photon energy is transferred to excite molecular vibrations. The fundamental transition from u = 0 to v = 1 dominates the infrared absorption, although other transitions may be possible. [Pg.257]


Because principles of vibrational spectroscopy have been covered extensively in a number of texts [8,9,28-32], only a few basic points are summarized here. [Pg.100]

In this section, we introduce the working principle of vibrational spectroscopy. It will be compared with a parent technique called Inelastic Electron Tunneling Spectroscopy, which was developed in the 60 s. Although the working principle is similar in each of them, the specific nature of electron-vibration interaction differs. We shall conclude this section by reviewing the most important achievements of single-molecule vibrational spectroscopy. [Pg.211]

All this requires some understanding about the principles of vibrational spectroscopy, force constants, the use of symmetry, and knowledge of the frequencies (and intensities) of a wide range of functional groups. Fortunately this has all been done superbly by Nakamoto, and every coordination chemist who makes any use of vibrational spectroscopy should have easy access to these publications. In this chapter we have no intention of repeating this work. Rather, we intend... [Pg.91]

Califano, S., Vibrational States, John Wiley Sous, Chichester (1976). Chamberlain, John, The Principles of Interferometric Spectroscopy, John Wiley Sons, Chichester (1979). [Pg.201]

The underlying principle of infrared spectroscopy is based upon the molecular vibrations which is further composed of the stretching and the bending vibrations of a molecule. [Pg.315]

T.L. Threlfall and J.M. Chalmers, Vibrational spectroscopy of solid-state forms - introduction, principles and overview, in Applications of Vibrational Spectroscopy in Pharmaceutical Research and Development, D.E. Pivonka, J.M. Chalmers, and RR. Griffiths (Eds), Wiley-Interscience, New York, 2007. [Pg.240]

The measurement of vibrational optical activity requires the optimization of signal quality, since the experimental intensities are between three and six orders of magnitude smaller than the parent IR absorption or Raman scattering intensities. To date all successful measurements have employed the principles of modulation spectroscopy so as to overcome short-term instabilities and noise and thereby to measure VOA intensities accurately. In this approach, the polarization of the incident radiation is modulated between left and tight circular states and the difference intensity, averaged over many modulation cycles, is retained. In spite of this common basis, there are major differences in measurement technique and instrumentation between VCD and ROA consequently, the basic experimental methodology of these two techniques will be described separately. [Pg.119]

Figure 9. Principle of NeNePo spectroscopy. The probe pulse detaches the photoelectron from the negative ion, introducing a vibrational wavepacket into the ground state of the neutral particle. Its propagation is interrogated by the probe pulse, which ionizes it to a positive ion. Figure 9. Principle of NeNePo spectroscopy. The probe pulse detaches the photoelectron from the negative ion, introducing a vibrational wavepacket into the ground state of the neutral particle. Its propagation is interrogated by the probe pulse, which ionizes it to a positive ion.
The first chapter of this volume, by Sheppard and de la Cruz, addresses the application of vibrational spectroscopy for the characterization of adsorbed hydrocarbons. This chapter is a successor to the 1958 Advances in Catalysis chapter about infrared spectra of adsorbed species, authored by the pioneers Eischens and Pliskin. Vibrational spectroscopy continues to provide some of the most incisive techniques available for determination of adsorbate structures. The present chapter is concerned with introductory principles and spectra of adsorbed alkenes a sequel is scheduled to appear in a subsequent volume of Advances in Catalysis. [Pg.446]

This book intends to supply the basic information necessary to apply the methods of vibrational spectroscopy, to design experimental procedures, to perform and evaluate experiments. It does not intend to provide a market survey of the instruments which are available at present, because such information would very soon be outdated. However, the general principles of the instruments and their accessories, which remain valid, are discussed. Details concerning sample preparation and the recording of the spectra, which is the subject of introductory courses, are assumed to be known. Special procedures which are described in monographs, such as Fourier transformation or chemometric methods, are also not exhaustively described. This book has been written for graduate students as well as for experienced scientists who intend to update their knowledge. [Pg.794]

Infra-red (IR) spectroscopy functions to probe vibrational transitions (2000-50 000 nm 5000-200 cm i.e. wave number - typical IR spectroscopy units) in the singlet ground electronic state of molecules. The absorption principles of IR spectroscopy are identical to those of UV-visible and CD spectroscopy. Hence the Beer-Lambert law (Equation (4.3)) applies. Moreover, absorption band intensities are determined by the transition dipole moment and there are extensive perturbation and coupling effects. Overall though, values of molar extinction coefficients for vibrational transitions, are up to 10 times lower in magnitude... [Pg.189]

Fig. 1. The principle of pumjvprobe spectroscopy by means of transient two-photon ionization A first fs-laser pulse electronically excites the particle into an ensemble of vibrational states creating a wave packet. Its temporal evolution is probed by a second probe pulse, which ionizes the excited particle as a function of the time-dependent Franck Condon-window (a) shows the principle for a bound-bound transition, where the oscillative behaviour of the wave packet will appear (b) shows it for a bound-free transition exhibiting the exponential decay of the fragmentizing particle, and (c) shows the process across a predissociated state, where the oscillating particle progressively leads into a fragmentation channel. Fig. 1. The principle of pumjvprobe spectroscopy by means of transient two-photon ionization A first fs-laser pulse electronically excites the particle into an ensemble of vibrational states creating a wave packet. Its temporal evolution is probed by a second probe pulse, which ionizes the excited particle as a function of the time-dependent Franck Condon-window (a) shows the principle for a bound-bound transition, where the oscillative behaviour of the wave packet will appear (b) shows it for a bound-free transition exhibiting the exponential decay of the fragmentizing particle, and (c) shows the process across a predissociated state, where the oscillating particle progressively leads into a fragmentation channel.
Our primary interest is in determining the structure of polymers so we need to understand the molecular basis of vibrational spectroscopy as a structural tool (a.4). The vibrational energy levels can be calculated from first principles by using a technique called normal coordinate analysis (a.5), and as a result some of the factors influencing spectra have been discovered. [Pg.6]

To observe particular rotational isomeric states, the method must be much more rapid than the rate of conformational isomerization. Optical methods such as absorption spectroscopy or light-scattering spectroscopy provide a short-time probe of the molecular conformation. If the electronic states of the molecule are strongly coupled to the backbone conformation, the ultraviolet or visible spectrum of the molecule can be used to study the conformational composition. The vibrational states of macromolecules are often coupled to the backbone conformation. The frequencies of molecular vibrations can be determined by infrared absorption spectroscopy and Raman scattering spectroscopy. The basic principles of vibrational spectres-... [Pg.29]

Infrared (IR) and Raman are both well established as methods of vibrational spectroscopy. Both have been used for decades as tools for the identification and characterization of polymeric materials in fact, the requirement for a method of analysis synthetic polymers was the basis for the original development of analytical infrared instrumentation during World War II. It is assumed that the reader has a general understanding of analytical chemistry, and a basic understanding of the principles of spectroscopy. A general overview of vibrational spectroscopy is provided in Sec. 5 for those unfamiliar with the infrared and Raman techniques. [Pg.207]

The basic principles of reflectance spectroscopy is firs emphasizing what is particular to each method (vibrational fingerprints... [Pg.549]

In this paper, the basic principles of reflectance spectroscopy will be first discussed, emphasizing what is particular to each method electronic spectra for UV-visible Reflectance Spectroscopy (UVERS), vibrational fingerprints for Electrochemically Modulated Infrared Reflectance Spectroscopy (EMIRS). After a short presentation of the experimental set-up for each technique, various examples, taken mainly from our laboratory, will be given. [Pg.550]


See other pages where Principles of Vibrational Spectroscopy is mentioned: [Pg.95]    [Pg.223]    [Pg.107]    [Pg.257]    [Pg.2]    [Pg.27]    [Pg.28]    [Pg.30]    [Pg.32]    [Pg.470]    [Pg.7]    [Pg.9]    [Pg.69]    [Pg.16]    [Pg.255]    [Pg.256]    [Pg.95]    [Pg.223]    [Pg.107]    [Pg.257]    [Pg.2]    [Pg.27]    [Pg.28]    [Pg.30]    [Pg.32]    [Pg.470]    [Pg.7]    [Pg.9]    [Pg.69]    [Pg.16]    [Pg.255]    [Pg.256]    [Pg.118]    [Pg.47]    [Pg.21]    [Pg.6374]    [Pg.117]    [Pg.172]    [Pg.6373]    [Pg.102]    [Pg.320]    [Pg.314]    [Pg.229]    [Pg.3]    [Pg.463]   


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