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Transmission-reflection

The emissivity, S, is the ratio of the radiant emittance of a body to that of a blackbody at the same temperature. Kirchhoff s law requires that a = e for aH bodies at thermal equHibrium. For a blackbody, a = e = 1. Near room temperature, most clean metals have emissivities below 0.1, and most nonmetals have emissivities above 0.9. This description is of the spectraHy integrated (or total) absorptivity, reflectivity, transmissivity, and emissivity. These terms can also be defined as spectral properties, functions of wavelength or wavenumber, and the relations hold for the spectral properties as weH (71,74—76). [Pg.202]

Fig. 30. IR reflection transmission spectra for InAs films formed on a smooth, annealed Au surface and on a roughened Au surface. The substrate was formed by taking a well annealed, smooth Au on glass substrate and vapor depositing more Au on one half, at room temperature, so that a series of 40 bumps were formed over one half of the surface. The two deposits were thus formed in the same electrodeposition run. Adapted from ref. [282],... Fig. 30. IR reflection transmission spectra for InAs films formed on a smooth, annealed Au surface and on a roughened Au surface. The substrate was formed by taking a well annealed, smooth Au on glass substrate and vapor depositing more Au on one half, at room temperature, so that a series of 40 bumps were formed over one half of the surface. The two deposits were thus formed in the same electrodeposition run. Adapted from ref. [282],...
The samples used to construct the models should be similar to the production samples also, their spectra should be recorded in the same mode (reflectance, transmission or transflectance) as those for the samples to be subsequently predicted, and include all potential sources of variability. Although such sources are relatively limited - pharmaceutical samples usually have a well-defined qualitative and quantitative composition from raw material to end product, and production processes are solidly established and reproducible - their... [Pg.472]

Figure 2.10 Analogy between scattering by a particle and reflection-transmission by a slab. Figure 2.10 Analogy between scattering by a particle and reflection-transmission by a slab.
The Vitatron TLD-100 thin-layer densitometer (Vitatron, Dieren, The Netherlands) is a single-beam instrument (Fig.3.11) which has been designed for reflectance, transmission... [Pg.52]

The Zeiss PMQ 3 chromatogram analyzer is probably the most versatile thin-film scanner available (Fig.3.13). The system can be used for reflectance, transmission, simultaneous reflectance and transmission and fluorescence quenching. It has two direct fluorescence modes, one with filter emission and surface illumination at a direction of 90° to the surface of the plate, and the other with 45° illumination and monochromatic emission. The instrument can be used for scanning thin-layer chromatograms, paper... [Pg.54]

Optical microscopy (OM) Reflection Transmission Phase contrast Polarized light... [Pg.378]

Wurtzite-structure ZnO thin films grown by a variety of deposition techniques, as well as commercially available single crystal bulk samples are discussed. Furthermore, data for ZnO thin films intermixed with numerous elements are reviewed. Most of the results are obtained by SE, which is a precise and reliable tool for measurements of the DFs. The SE results are supplemented by Raman scattering and electrical Hall-effect measurement data, as well as data reported in the literature by similar or alternative techniques (reflection, transmission, and luminescence excitation spectroscopy). [Pg.81]

In practice we usually think about the response of a material to oscillatory fields— absorption, reflection, transmission, refraction, etc. We learn to connect the frequencies at which electromagnetic waves are absorbed with the natural motions of the material. If necessary, we can use oscillatory-field responses to know what the material would do in nonoscillatory fields. [Pg.242]

We now consider a simple extension of the presentations in Secs. 8-10 and 8-11 to analyze a medium where reflection, transmission, and absorption modes are all important. As in Sec. 8-10, we shall analyze a system consisting of two parallel diffuse planes with a medium in between which may absorb, transmit, and reflect radiation. For generality we assume that the surface of the transmitting medium may have both a specular and a diffuse component of reflection. The system is shown in Fig. 8-58. [Pg.436]

Five different optical phenomena are used for producing linear polarization dichroism, birefringence, reflection, reflection-transmission by metal gratings (grids), and scattering. [Pg.89]

Currently, quantum mechanics provides the most complete theoretical understanding of spectroscopy and the information that spectroscopic analysis yields. Quantum theory predicts a discrete set of energy levels for particles, and, therefore, the reflection, transmission and absorption characteristics of a sample can be compared to the characteristics of known materials over a spectrum of wavelengths, thus providing a means of identification of a sample. Since spectroscopy could, conceivably, cover a vast number of methods of analysis, the particular kinds of information that can be acquired through the use of spectroscopic analysis is best illustrated by way of several examples. Astronomical spectroscopy... [Pg.216]

The predicted in-plane isotropization of the polariton dispersion in an anisotro -pic crystalline organic microcavity can be observed in the spectra of reflection, transmission and photoluminescence. [Pg.278]

Materials and lighting are design tools. There are three types of physically definable material properties - optical properties, physical form, and temporal properties. Optical properties include tight distribution occurring over the surface and within the depth of the material as well as reflectance, transmission,... [Pg.15]


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See also in sourсe #XX -- [ Pg.261 , Pg.265 , Pg.274 , Pg.281 ]




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Absorption. Reflection. Transmission

Attenuated total reflection transmission

Complex reflection and transmission coefficient

Fourier transform infrared-reflectance transmission

Fourier transform infrared-reflectance transmission measurement

Fourier transform infrared-reflectance transmission microscopy

Fresnel reflection and transmission

Fresnel reflection-transmission

Fresnel reflection-transmission techniques

Laue cameras, back-reflection transmission

Layered Polymers-Transmission and Reflection

Light reflection/transmission

Light reflection/transmission instrumentation

Reflection and Transmission at a Plane Boundary

Reflection and Transmission at an Interface

Reflection and Transmission by a Slab

Reflection and Transmission of Electromagnetic Waves

Reflection and transmission

Reflection and transmission amplitudes

Reflection and transmission properties

Reflection, Absorption, and Transmission

Reflection-absorption spectroscopy compared with transmission

Reflection/transmission spectra

The theory of IR reflection and transmission

Transmission and Reflection Measurements

Transmission-reflectance accessory, study

Transmission-reflection studies

Tunneling, Transmission, and Reflection

Visual colorimetry by transmission or reflection

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