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Quartz mirror

If the flame background emission intensity is reduced considerably by use of an inert gas-sheathed (separated) flame, then an interference filter may be used rather than a monochromator, to give a non-dispersive atomic fluorescence spectrometer as illustrated in Figure 14.36-38 Noise levels are often further reduced by employing a solar blind photomultiplier as a detector of fluorescence emission at UV wavelengths. Such detectors do not respond to visible light. The excitation source is generally placed at 90° to the monochromator or detector. Surface-silvered or quartz mirrors and lenses are often used to increase the amount of fluorescence emission seen by the detector. [Pg.28]

A triangular bent Ge(l 11) monochromator and a segmented quartz mirror are used as optical elements. The fixed wavelength of 1.5 A which is obtained for a monochromator angle of 26.5° is a compromise between the transmission of Beryllium used as a window material, the efficiency of gasfilled detectors and -especially for biological samples — the transmission of water. [Pg.26]

The mirror is also used to suppress the higher harmonics. Thus for a quartz mirror operating in total reflection, the grazing angle is about 3 mrad. Only wavelength longer than given by ... [Pg.27]

Fig. 26. Reflectivity of a quartz mirror as a function of the wavelength at different angles of grazing incidence . An optimum reflectivity at 1.5 A is obtained for an angle of 3 mrad. The mirror acts as a filter cutting at this angle shorter wavelength... Fig. 26. Reflectivity of a quartz mirror as a function of the wavelength at different angles of grazing incidence . An optimum reflectivity at 1.5 A is obtained for an angle of 3 mrad. The mirror acts as a filter cutting at this angle shorter wavelength...
One is limited, however, by the angle of critical reflection as the intensity decreases with increasing angle of total reflection. From this point of view a mirror with heavy atom coating is preferable over a quartz mirror. In view of the use as a small angle scattering camera, low electron density materials have, however, been preferred (Sect. 3.2.2). [Pg.31]

Fig. 3. Schematic representation of the SAXS/WAXS Polymer Beamline A2 at HASYLAB/Ham-burg SI, S2 slits, Mo crystal monochromator, Mi quartz mirror, S3 aperture slit, S4 guard slit and sample position, D detector... Fig. 3. Schematic representation of the SAXS/WAXS Polymer Beamline A2 at HASYLAB/Ham-burg SI, S2 slits, Mo crystal monochromator, Mi quartz mirror, S3 aperture slit, S4 guard slit and sample position, D detector...
Another important parameter that may affect the resolution is the higher harmonic contribution from the Bragg reflector. A fused quartz mirror behind the monochromator has been currently used to reject this high harmonic contribution. Therefore, the energy resolution of the spectrometer is just limited by the Darwin width of the rocking curve and the spatial resolution of the position-sensitive detector [8]. [Pg.186]

The beam line optics consists of a bent Si (111) monochromator. Various crystals with different oblique-cut angles are available, namely a=0°, 6.0°, 7.8°, 9.5°, 11.4°, 13.7° and 16.5° to allow an energy range of 5-25 keV to be covered, by appropriate choice of crystal. There is a bent plane fused quartz mirror (Satow, Mikuni, Kamiya and Ando 1989). [Pg.237]

In certain crystals, e.g. in quartz, there is chirality in the crystal structure. Molecular chirality is possible in compounds which have no chiral carbon atoms and yet possess non-superimposable mirror image structures. Restricted rotation about the C=C = C bonds in an allene abC = C = Cba causes chirality and the existence of two optically active forms (i)... [Pg.91]

The optical activity of quartz and certain other materials was first discovered by Jean-Baptiste Biot in 1815 in France, and in 1848 a young chemist in Paris named Louis Pasteur made a related and remarkable discovery. Pasteur noticed that preparations of optically inactive sodium ammonium tartrate contained two visibly different kinds of crystals that were mirror images of each other. Pasteur carefully separated the two types of crystals, dissolved them each in water, and found that each solution was optically active. Even more intriguing, the specific rotations of these two solutions were equal in magnitude and of opposite sign. Because these differences in optical rotation were apparent properties of the dissolved molecules, Pasteur eventually proposed that the molecules themselves were mirror images of each other, just like their respective crystals. Based on this and other related evidence, in 1847 van t Hoff and LeBel proposed the tetrahedral arrangement of valence bonds to carbon. [Pg.97]

Premier and Schupp have made vapour-density measurements with sulphur enclosed in a quartz bulb heated electrically and connected with a manometer consisting of a spiral of silica tubing attached to a small mirror. The pressure was measured by the amount of unwinding of the spiral. The same method has been used by Bodenstein and Katavama in studving the equilibrium ... [Pg.357]

The occurrence of twinned crystals is a widespread phenomenon. They may consist of individuals that can be depicted macroscopically as in the case of the dovetail twins of gypsum, where the two components are mirror-inverted (Fig. 18.8). There may also be numerous alternating components which sometimes cause a streaky appearance of the crystals (polysynthetic twin). One of the twin components is converted to the other by some symmetry operation (twinning operation), for example by a reflection in the case of the dovetail twins. Another example is the Dauphine twins of quartz which are intercon-verted by a twofold rotation axis (Fig. 18.8). Threefold or fourfold axes can also occur as symmetry elements between the components the domains then have three or four orientations. The twinning operation is not a symmetry operation of the space group of the structure, but it must be compatible with the given structural facts. [Pg.223]

Radicals still less stable than the ones discussed thus far are proposed as reaction intermediates. Many of these have been prepared in the gas phase where they may be detected by the well-known mirror technique. When a stream of a carrier gas, such as hydrogen or nitrogen containing lead tetramethyl vapor, is passed over a hot spot in a quartz tube, lead from the decomposing lead tetramethyl forms a lead mirror at the hot spot. But if there is already a lead mirror not too far downstream from the hot spot, the downstream mirror disappears.44... [Pg.24]

Figure 1. Schematic diagram of specially designed fixtures used to measure, in situ, the evolving rheological properties during UV curing. The sample is placed between the two quartz plates and the incident UV radiation exiting the liquid light guide is reflected by the mirror through the plates and onto the sample. Figure 1. Schematic diagram of specially designed fixtures used to measure, in situ, the evolving rheological properties during UV curing. The sample is placed between the two quartz plates and the incident UV radiation exiting the liquid light guide is reflected by the mirror through the plates and onto the sample.
In recent years, stereochemistry, dealing with the three-dimensional behavior of chiral molecules, has become a significant area of research in modern organic chemistry. The development of stereochemistry can, however, be traced as far back as the nineteenth century. In 1801, the French mineralogist Haiiy noticed that quartz crystals exhibited hemihedral phenomena, which implied that certain facets of the crystals were disposed as nonsuperimposable species showing a typical relationship between an object and its mirror image. In 1809, the French physicist Malus, who also studied quartz crystals, observed that they could induce the polarization of light. [Pg.2]

Six years later Sir John Herschel 13> observed that the algebraic sign of the optical rotation of quartz crystals could be correlated with their shape, and the dextro- and levorotatory crystals look like mutual mirror images. This correlation was extended from crystals to molecules by Pasteur 14>, who postulated that the spatial arrangement of atoms in the molecules is responsible for their optical activity, and the dextro-and levorotatory molecules are in a mirror image relation. [Pg.17]

Rg. 11.2 Single crystals of morphologically enantiomeric quartz. Note the mirror symmetry of the facets on the respective crystals. Unlike amino acids, the component silicon dioxide molecules have no chirality. The spontaneous resolution of quartz into crystals of opposite morphological handedness is an example of local symmetry breaking in the environment. [Pg.179]


See other pages where Quartz mirror is mentioned: [Pg.233]    [Pg.168]    [Pg.27]    [Pg.143]    [Pg.259]    [Pg.162]    [Pg.222]    [Pg.427]    [Pg.396]    [Pg.233]    [Pg.168]    [Pg.27]    [Pg.143]    [Pg.259]    [Pg.162]    [Pg.222]    [Pg.427]    [Pg.396]    [Pg.221]    [Pg.342]    [Pg.666]    [Pg.744]    [Pg.79]    [Pg.189]    [Pg.311]    [Pg.338]    [Pg.5]    [Pg.15]    [Pg.70]    [Pg.70]    [Pg.71]    [Pg.108]    [Pg.152]    [Pg.194]    [Pg.134]    [Pg.446]    [Pg.74]    [Pg.240]    [Pg.367]    [Pg.537]    [Pg.596]   
See also in sourсe #XX -- [ Pg.26 , Pg.27 ]




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