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Interaction of Light with Matter

A further spatial derivative of the first Maxwell equation and the appropriate substitution yields [Pg.132]

In terms of just one of the fields, e.g., the electric field, we have [Pg.132]

With //., and a independent of E, the solution of this second order partial differential equation is composed of transverse harmonic waves [Pg.132]

The complete description of the individual components of the propagating field amplitudes with their appropriate projection onto the interface of the two media is given by the Fresnel equations. [Pg.132]

The attenuation of the amplitudes along the propagation path in our wave description enters through the imaginary part —i 2 of the complex dielectric function i = eq — i 2. The latter translates into a complex refractive index h = n — ik. Both result from the electrical conductivity term a. The corresponding attenuation of the Poynting vector in our system, which we assume to respond in a linear way to field perturbations, accordingly shows [Pg.132]

At this point, it is necessary to ask how light from the sources examined in the previous section might behave when it strikes an object, whether that object be the atmosphere, a liquid, solid or gaseous substance, or any other material substance one can think of. We can call any of these substances or objects the light modifier since light is indeed changed upon interaction. Some of the more [Pg.20]


A1.6 Interaction of light with matter a coherent perspective... [Pg.218]

An excellent and readable discnssion of all aspects of the interaction of light with matter, from blackbody radiation to lasers and nonlinear optics. [Pg.281]

Spectroscopy, or the study of the interaction of light with matter, has become one of the major tools of the natural and physical sciences during this century. As the wavelength of the radiation is varied across the electromagnetic spectrum, characteristic properties of atoms, molecules, liquids and solids are probed. In the... [Pg.1232]

To understand the production of laser light, it is necessary to consider the interaction of light with matter. Quanta of light (photons) of wavelength X have energy E given by Equation 18.1, in which h is Planck s constant (6.63 x 10 J-sec) and c is the velocity of light (3 x 10 m-sec-h-... [Pg.123]

The physical basis of spectroscopy is the interaction of light with matter. The main types of interaction of electromagnetic radiation with matter are absorption, reflection, excitation-emission (fluorescence, phosphorescence, luminescence), scattering, diffraction, and photochemical reaction (absorbance and bond breaking). Radiation damage may occur. Traditionally, spectroscopy is the measurement of light intensity... [Pg.299]

Fluorescence and phosphorescence are particular cases of luminescence (Table 1.1). The mode of excitation is absorption of a photon, which brings the absorbing species into an electronic excited state. The emission of photons accompanying deexcitation is then called photoluminescence (fluorescence, phosphorescence or delayed fluorescence), which is one of the possible physical effects resulting from interaction of light with matter, as shown in Figure 1.1. [Pg.4]

The reduction of obtainable light-pulse durations down to subpicosecond pulses (halfwidth about 10 sec) allows fast transient phenomena which were not accessible before to be studied in the interaction of light with matter. One example is the extension of spin echoe-techniques, well known in nuclear-magnetic-resonance spectroscopy, to the photon echoes in the optical region. [Pg.84]

II. Interaction of Light with Matter and History of PDT III. Mechanisms of Photodynamic Production 121... [Pg.119]

The interaction of light with matter gives rise to many varied and fascinating phenomena. Molecular photochemistry at the most basic level deals with interactions of molecules and photons to generate different electronic configurations, which may show substantially different chemical reactivity than ground-state species (1). Photochemical reactions may involve many electronic states, each of different character, which may be coupled strongly... [Pg.351]

It is possible to obtain A and / fromEq. (7.118).55 However, the extraction of the refractive index of the film and its thickness involves Fresnel s equation for the interaction of light with matter, and this mathematical manipulation was impractically laborious before the introduction of computers in the 1960s. [Pg.434]

Spectroscopy is concerned with the interaction of light with matter. This monograph deals with collision-induced absorption of radiation in gases, especially in the infrared region of the spectrum. Contrary to the more familiar molecular spectroscopy which has been treated in a number of well-known volumes, this monograph focuses on the supermolecular spectra observable in dense gases it is the first monograph on the subject. [Pg.1]

Show by substitution in the formula given in the text ( Interaction of Light with Matter ) that ao, the radius of the first Bohr orbit for hydrogen, is 5.29 x 10-11 m. [Pg.126]

Absorption and emission of light Interaction of light with matter Particles and waves... [Pg.401]

The use of optical methods to study the dynamics and structure of complex polymeric and colloidal liquids subject to external fields has a long history. The choice of an optical technique is normally motivated by the microstructural information it provides, its sensitivity, and dynamic range. A successful application of an optical measurement, however, will depend on many factors. First, the type of interaction of light with matter must be correctly chosen so that the desired microstructural information of a sample can be extracted. Once selected, the arrangement of optical elements required to perform the required measurement must be designed. This involves not only the selection of the elements themselves, but also their alignment. Finally, a proper interpretation of the observables will depend on one s ability to connect the measurement to the sample s microstructure. [Pg.276]

FIGURE 1 Fundamental phenomena resulting from the interaction of light with matter. [Pg.135]

The interaction of light with matter is the perturbation of the charged electrons and nuclei by the electric field E associated with the radiation. This results in the production of a polarization P in the sample that can be expressed as... [Pg.407]

The interaction of light with matter has fascinated people since ancient times. The color of an object is the result of this interaction. In modem terms, this interaction is described as spectroscopy. In this chapter, how the optical properties of a material are the result of its chemical composition and stmcture are examined. Several examples of technologically relevant applications are then presented of the manipulation of the optical properties to achieve a desired performance. [Pg.377]


See other pages where Interaction of Light with Matter is mentioned: [Pg.956]    [Pg.1179]    [Pg.407]    [Pg.245]    [Pg.286]    [Pg.465]    [Pg.44]    [Pg.521]    [Pg.423]    [Pg.380]    [Pg.259]    [Pg.121]    [Pg.195]    [Pg.12]    [Pg.344]    [Pg.31]    [Pg.22]    [Pg.11]    [Pg.18]    [Pg.334]    [Pg.113]    [Pg.77]    [Pg.1]    [Pg.2]    [Pg.4]    [Pg.6]    [Pg.8]    [Pg.10]    [Pg.131]    [Pg.7]    [Pg.32]   


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