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Visible and near-ultraviolet

Useful fransparenf materials for cell windows, lenses, and so on are Pyrex glass for fhe visible and fused quartz for fhe visible and near-ulfraviolef. [Pg.62]

A more recent, and superior, type of detector, which also benefits from the multiplex advantage, is the charge-coupled device (CCD). The CCD, as used for spectroscopy, has been developed from the CCD detector used in a camcorder. [Pg.63]

A CCD is a two-dimensional array of silicon photosensors, each photosensor usually being referred to as a pixel. When radiation falls on a pixel, photoelectrons are produced in numbers proportional to the intensity of the radiation. A typical wavelength range to which the CCD is sensitive is 400-1050 nm, but this may be extended down to below 1.5 nm with a phosphor that converts short-wavelength into visible radiation. [Pg.63]

Having found the electronic dielectric function. Equation 23.49 to be given by [Pg.468]

One can see that using 4tt o estimates the polarizability to within an order of magnitude, but is not accurate enough to make useful predictions of the optical properties of materials. [Pg.468]

Source Polarizability values were taken from Kittel, C., Introduction to Solid State Physics, 7th edn., John Wiley Sons, New York, 1966. [Pg.469]


Diffraction gratings may be made by a holographic process, but blaze characteristics cannot be controlled and their efficiency is low in the infrared. They are mostly used for low-order work in the visible and near-ultraviolet. [Pg.47]

Typical recording spectrophotometers for the near-infrared, mid-infrared, visible and near-ultraviolet regions... [Pg.68]

Figure 3.24 A typical double-beam recording visible and near-ultraviolet spectrophotometer... Figure 3.24 A typical double-beam recording visible and near-ultraviolet spectrophotometer...
For the visible and near-ultraviolet portions of the spectmm, tunable dye lasers have commonly been used as the light source, although they are being replaced in many appHcation by tunable soHd-state lasers, eg, titanium-doped sapphire. Optical parametric oscillators are also developing as useful spectroscopic sources. In the infrared, tunable laser semiconductor diodes have been employed. The tunable diode lasers which contain lead salts have been employed for remote monitoring of poUutant species. Needs for infrared spectroscopy provide an impetus for continued development of tunable infrared lasers (see Infrared technology and RAMAN spectroscopy). [Pg.17]

Spectrophotometry proper is mainly concerned with the following regions of the spectrum ultraviolet, 185-400 nm visible 400-760 nm and infrared, 0.76-15 /tm. Colorimetry is concerned with the visible region of the spectrum. In this chapter attention will be confined largely to the visible and near ultraviolet region of the spectrum. [Pg.647]

Both CI2 and CINO2 absorb visible and near ultraviolet radiation, so that they can readily photolyze even with the faint amount of sunlight... [Pg.29]

The most stable resin for many of our purposes has proven to be a copolymer of ethyl methacrylate and methyl acrylate. This comes as little surprise the Rohm and Haas Company has for years sold a durable resin based on these two monomers, Acryloid B-72 (6,28). We have also prepared polymers of similar physical properties based on methyl methacrylate and ethyl acrylate and have found that their behavior is practically the same - the methyl and ethyl groups apparently do not become seriously involved in crosslinking. As reported elsewhere( 23), rather than crosslink, Acryloid B-72 tends to chain break under visible and near-ultraviolet radiation, although at a very slow rate. Polyvinylacetate is another polymer used in the care of museum objects that tends more to chain break than crosslink under these conditions(23), but it is not our purpose to discuss its properties at this time. [Pg.193]

Al(HE), Ga(HE) as well as In(HE) porphyrin are typical porphyrins incorporated with a tervalent metal ion Characteristic Q and B bands in the visible and near-ultraviolet region, respectively, arise from the (7T,7T ) excitations in the porphyrin ring with only minor perturbation from the outershell electrons of the central metal ion. The Q band is of forbidden character, however, the Q band can borrow the intensity by vibronic couplings from the allowed B band (30). The intensity of the Q(1,0) band is much less sensitive to the peripheral substituents, the axial ligands and the central metal ions, while that of the Q(0,0) band without excitation in the skeletal vibrational modes is rather sensitive to various substituents. [Pg.108]

These simple molecular orbital pictures provide useful descriptions of the structures and spectroscopic properties of planar conjugated molecules such as benzene and naphthalene, and heterocychc species such as pyridine. Heats of combustion or hydrogenation reflect the resonance stabilization of the ground states of these systems. Spectroscopic properties in the visible and near-ultraviolet depend on the nature and distribution of low-lying excited electronic states. The success of the simple molecular orbital description in rationalizing these experimental data speaks for the importance of symmetry in determining the basic characteristics of the molecular energy levels. [Pg.103]

The most obvious characteristic of the spectra of low-spin five-coordinate complexes is the high intensity of the bands in the visible and near ultraviolet. For a long time this feature of the spectra raised doubts as to whether these low frequency bands should be considered as d—d transitions or charge-transfer transitions. [Pg.79]

Visible and near-ultraviolet absorption spectra for aqueous solutions of Co(NH3)63+ and Co(NH3)5Br2+ are shown in Figure 6. The spectrum of Co(NH3)83 + is typical of diamagnetic, octahedral d6 systems, consisting of two broad bands of low intensity centered near 500 mjx and near 350 m and a very intense band in the ultraviolet. In the Co(NH3)5Br2+ spectrum the high-intensity bands occur at sig-... [Pg.158]

Figure 1.2. An image produced by exciting hydrogen gas and separating the outgoing light with a prism, reprinted from [Her. Fig. 1. p. 5]. Specifically, this is the emission spectrum of the hydrogen atom in the visible and near ultraviolet region. The label marks the position of the limit of the series of wavelengths. Figure 1.2. An image produced by exciting hydrogen gas and separating the outgoing light with a prism, reprinted from [Her. Fig. 1. p. 5]. Specifically, this is the emission spectrum of the hydrogen atom in the visible and near ultraviolet region. The label marks the position of the limit of the series of wavelengths.
The ground state is X L+ D0(H—CN) = 5.20 0.05 eV (264). Hydrogen cyanide has no absorption in the visible and near ultraviolet regions. It starts to absorb weakly at about 1900 A. Herzberg and Innes (463) have found three band systems in the region 1350 to 1900 A, corresponding to the y, (I, and a systems. The upper states are all bent. [Pg.42]

Fig. Vl-18. The absorption coefficients of Cl 2() in the visible and near ultraviolet regions, k is given in units of mm 1 cm"1, base 10, room temperature. From Goodeve and Wallace (409), reprinted by permission of the Chemical Society. [Pg.68]

Sunlight in the near infrared, visible, and near ultraviolet regions possesses considerable energy utilization of this through photochemical reactions could make a considerable contribution to energy resources. Sinoe biosynthesis itself is relatively inefficient 111 conversion of solar energy, emphasis has been placed upon the fabrication of artificial photochemical systems. One of the more promising approaches has involved application of photoelectric chemical cells or catalysts of semiconductor materials. [Pg.1284]

The tetrahedral ions, POtHSOr and CIO - show no near ultraviolet absorption whereas the ions, XO4", of the fourth-row transition elements, which have the same number of valence electrons, show characteristic visible and near ultraviolet absorption, two strong maxima with the corresponding peaks displaced toward shorter wavelengths with decreasing atomic number of the central atom. This trend is also observed for the fifth- and sixth-row transition element compounds. A satisfactory theory must account for these differences and regularities. [Pg.261]

Table IV shows the calculated and observed energies of transition in the three ions considered here, and it is seen that the first absorption by ClO Table IV shows the calculated and observed energies of transition in the three ions considered here, and it is seen that the first absorption by ClO<T lies well into the ultraviolet and MnO<r and CrO show two maxima in the visible and near ultraviolet. The rather surprising quantitative agreement probably arises from the empirical nature of our calculations. This agreement can be improved by changes in the values of the Hu s and the /Vs, but these changes are limited severely by the requirement that the intensities of absorption be given correctly.
Mount, G.M., R.W. Sanders, A.L. Schmetekopf and S. Solomon (1987) Visible and near ultraviolet spectroscopy at McMurdo station Antarctica 1 Overview and daily variations of NO2 and 05 during austral spring 1986.Journal of Geophysical Research 92 8320-8340. [Pg.328]

Values of b0 from Visible and Near Ultraviolet ORD Spectra... [Pg.723]

Infrared, visible and near ultraviolet spectroscopy are particularly important when used in conjunction with polarising devices in determining the mean orientation of molecules or particular parts of molecules. [Pg.16]


See other pages where Visible and near-ultraviolet is mentioned: [Pg.1119]    [Pg.62]    [Pg.70]    [Pg.219]    [Pg.245]    [Pg.474]    [Pg.667]    [Pg.557]    [Pg.286]    [Pg.461]    [Pg.285]    [Pg.340]    [Pg.126]    [Pg.365]    [Pg.721]    [Pg.722]    [Pg.389]    [Pg.340]    [Pg.223]    [Pg.1]    [Pg.6]    [Pg.51]    [Pg.220]    [Pg.390]    [Pg.164]    [Pg.297]    [Pg.59]    [Pg.1285]    [Pg.280]   


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