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Diffraction, first order

A LEED pattern is obtained for the (111) surface of an element that crystallizes in the face-centered close-packed system. Show what the pattern should look like in symmetry appearance. Consider only first-order nearest-neighbor diffractions. [Pg.312]

Kinoforms are phase-only masks which are prepared by setting the amphtude values to unity and changing only the phase across the hologram (30). The kinoform has the advantage that proper preparation can lead to holograms which can diffract almost ah. of the light into the usefiil first order. [Pg.162]

The following calculation for carbon illustrates the use of a grating. The values = 0.75°, d = 8333 A, and A carbon Ka = 44,4 A substituted in the grating formula, give 6.3° for the angle between the grating and the first-order diffracted beam, which corresponds to a 26 of only 7°. [Pg.319]

The results of x-ray structure analysis and neutron diffraction, as well as spectroscopic experiments (J(HSi) = 70.8 Hz for 30), can be interpreted in the sense mentioned above. The observed reactivity of 30 is also consistent with this view, the coordinated silanes can be displaced smoothly by phosphines, according to first-order reaction kinetics. [Pg.15]

Baranowski [680] concluded that the decomposition of nickel hydride was rate-limited by a volume diffusion process the first-order equation [eqn. (15)] was obeyed and E = 56 kJ mole-1. Later, Pielaszek [681], using volumetric and X-ray diffraction measurements, concluded from observations of the effect of copper deposited at dislocations that transportation was not restricted to imperfect zones of the crystal but also occurred by diffusion from non-defective regions. The role of nickel hydride in catalytic processes has been reviewed [663]. [Pg.156]

This expression fitted the acceleratory period of the a—time curves, followed by first-order decay and E = 122 2 kJ mole-1. No disintegration of small crystals was observed but pre-irradiated crystals [909] shattered on completion of the induction period. X-ray diffraction studies [910] confirm the existence of strain during the formation of decomposition product. Addition of small amounts (5% by mass) of ZnO or Th02 accelerated the decomposition of AgMn04 at 388 K. Ti02 reduced the rate, while NiO and Co304 had no effect [911]. [Pg.194]

Fig. 4.6 Layer sequence and X-ray diffraction (CuK ) of 8f period 4PbTe/4PbSe superfattice. Buffer layer is a fO-cycfe PbSe. Angle of incidence is 1°. The (111) diifraction peak (So), along with both first-order satellite peaks, and one second-order peak, are evident and indicative of the formation of a superlattice. (The XRD diagram is reprinted with permission from [76], Copyright 2009, American Chemical Society)... Fig. 4.6 Layer sequence and X-ray diffraction (CuK ) of 8f period 4PbTe/4PbSe superfattice. Buffer layer is a fO-cycfe PbSe. Angle of incidence is 1°. The (111) diifraction peak (So), along with both first-order satellite peaks, and one second-order peak, are evident and indicative of the formation of a superlattice. (The XRD diagram is reprinted with permission from [76], Copyright 2009, American Chemical Society)...
The spatially periodic temperature distribution produces the corresponding relxactive index distribution, which acts as an optical phase grating for the low-power probing laser beam of the nonabsorbed wavelength in the sample. The thermal diffusivity is determined by detecting the temporal decay of the first-order diffracted probing beam [°o exp(-2t/x)] expressed by... [Pg.189]

Similarly, the first-order expansion of the p° and a of Eq. (5.1) is, respectively, responsible for IR absorption and Raman scattering. According to the parity, one can easily understand that selection mles for hyper-Raman scattering are rather similar to those for IR [17,18]. Moreover, some of the silent modes, which are IR- and Raman-inactive vibrational modes, can be allowed in hyper-Raman scattering because of the nonlinearity. Incidentally, hyper-Raman-active modes and Raman-active modes are mutually exclusive in centrosymmetric molecules. Similar to Raman spectroscopy, hyper-Raman spectroscopy is feasible by visible excitation. Therefore, hyper-Raman spectroscopy can, in principle, be used as an alternative for IR spectroscopy, especially in IR-opaque media such as an aqueous solution [103]. Moreover, its spatial resolution, caused by the diffraction limit, is expected to be much better than IR microscopy. [Pg.94]

Method employed to establish first-order character of transition cal = calorimetry DSC = differential scanning calorimetry X-ray = X-ray diffraction ME = Mossbauer effect... [Pg.64]

In this section we will discuss perturbation methods suitable for high-energy electron diffraction. For simplicity, in this section we will be concerned with only periodic structures and a transmission diffraction geometry. In the context of electron diffraction theory, the perturbation method has been extensively used and developed. Applications have been made to take into account the effects of weak beams [44, 45] inelastic scattering [46] higher-order Laue zone diffraction [47] crystal structure determination [48] and crystal structure factors refinement [38, 49]. A formal mathematical expression for the first order partial derivatives of the scattering matrix has been derived by Speer et al. [50], and a formal second order perturbation theory has been developed by Peng [22,34],... [Pg.166]

Also known for some time is a phase transition at low temperature (111K), observed in studies with various methods (NQR, elasticity measurement by ultrasound, Raman spectrometry) 112 temperature-dependent neutron diffraction showed the phase transition to be caused by an antiphase rotation of adjacent anions around the threefold axis ([111] in the cubic cell) and to lower the symmetry from cubic to rhombohedral (Ric). As shown by inelastic neutron scattering, this phase transition is driven by a low-frequency rotatory soft mode (0.288 THz 9.61 cm / 298 K) 113 a more recent NQR study revealed a small hysteresis and hence first-order character of this transition.114 This rhombohedral structure is adopted by Rb2Hg(CN)4 already at room temperature (rav(Hg—C) 218.6, rav(C—N) 114.0 pm for two independent cyano groups), and the analogous phase transition to the cubic structure occurs at 398 K.115... [Pg.1261]

First-order phase transitions can be detected by various thermoanalytical techniques, such as DSC, thermogravimetric analysis (TGA), and thermomechanical analysis (TMA) [31]. Phase transitions leading to visual changes can be detected by optical methods such as microscopy [3], Solid-solid transitions involving a change in the crystal structure can be detected by X-ray diffraction [32] or infrared spectroscopy [33], A combination of these techniques is usually employed to study the phase transitions in organic solids such as drugs. [Pg.600]

X-ray diffraction from cast films provide useful information of bilayer structure. Periodic peaks in small and middle-angle diffraction from cast films on glass plates are attributed to the reflections from (h, 0,0) planes of the multiple lamella structure. The spacing of higher order reflections (h > 1) satisfies with numerical relation of 1 / h of the long period calculated from the first order reflection =1), which is equivalent to the bilayer thickness. Every cast film measured in this experiment showed more than 6 reflection peaks. [Pg.58]

Gratings also diffract light in the second, third and higher orders. If a grating reinforces light at 600 nm in the first order, it will also reinforce fight at 300 nm in the second order and 200 nm in the third order. Gratings are usually paired with simple optical filters to remove unwanted... [Pg.140]

What wavelength will be observed at a detector that is placed at 23.5° when the light source strikes the reflection grating at an angle of 45.3° and the grating has 1250 lines per mm. Assume that the order of diffraction is first order. What is the second order wavelength observed ... [Pg.161]


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See also in sourсe #XX -- [ Pg.40 ]




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Diffractive order

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