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Stripe longitudinal

The charge stripe is normally viewed as a 1D lane, along which the holes can freely move longitudinally, but are constrained in the transverse direction by the antiphase AFM-ordered magnetic domains. Indeed, the pinning at the magic number doping (x=... [Pg.284]

APPEARANCE. Aphid bright green body with two longitudinal stripes on the back the extremities are greyish green. [Pg.146]

APPEARANCE. Midge midge 2.5-3.5 mm in size, with two longitudinal stripes. [Pg.189]

Horn (cattle hom, etc.) Cream, browns to black in patches Almost opaque, except if in thin section, bleached or pressed Longitudinal striations Colours in fine stripes if bleached or very pale Slight fluorescence on pale areas... [Pg.253]

Rhino horn Mid-brown with fine stripes Only in thin sections, e.g. of fine carving Longitudinal striations Not possible Mosdy inert. Some fluorescence on outer surface... [Pg.253]

Blue-black pigmentation involving the palate and facial, pretibial, and subungual areas occurs rarely, but it has been associated with retinopathy (SEDA-11, 584). The nail bed can turn blue-brown and the nail itself may develop longitudinal stripes and show a blue-grey fluorescence (SEDA-11, 584). [Pg.726]

Chloroquine can turn the nail bed blue-brown and the nail itself can develop longitudinal stripes and show a blue-grey fluorescence (SEDA-11, 584). [Pg.727]

Figure 9-19 Phonon dispersion relation (angular frequency vs. relative wave vector) for the three-stripe phase of CH4 on the external surface of a bundle. LI, L2, and L3 are longitudinal branches, i.e., molecular motion parallel to the groove. The dotted curve is the result for a ID adsorbate at the same density. The remaining curves correspond to the dispersion relation of transverse modes. (Adapted from Ref. [89].)... Figure 9-19 Phonon dispersion relation (angular frequency vs. relative wave vector) for the three-stripe phase of CH4 on the external surface of a bundle. LI, L2, and L3 are longitudinal branches, i.e., molecular motion parallel to the groove. The dotted curve is the result for a ID adsorbate at the same density. The remaining curves correspond to the dispersion relation of transverse modes. (Adapted from Ref. [89].)...
Figure 16. Surface phonon dispersion curves for LiF(OOl). The calculated bulk bands are indicated by the vertical-striped regions. The surface localized modes are shown by heavy solid lines, whereas the resonances lying within bulk bands are given by thinner solid lines. The mode label S refers to the Rayleigh wave, to the longitudinal resonance, Sg to the crossing resonance, and S2, S3, and S4 to optical modes. (Reproduced from Fig. 2 of Ref. 58, with permission of Elsevier Science Publishers.)... Figure 16. Surface phonon dispersion curves for LiF(OOl). The calculated bulk bands are indicated by the vertical-striped regions. The surface localized modes are shown by heavy solid lines, whereas the resonances lying within bulk bands are given by thinner solid lines. The mode label S refers to the Rayleigh wave, to the longitudinal resonance, Sg to the crossing resonance, and S2, S3, and S4 to optical modes. (Reproduced from Fig. 2 of Ref. 58, with permission of Elsevier Science Publishers.)...
Figure 34. Surface phonon dispersion for 2H-TaSe2. The HAS data are shown as solid circles except for weak points which appear in the TOP spectra as hybridized longitudinal modes that are shown as crosses. All the data were obtained at 60 K, well into the low-temperature phase. The calculated striped and shaded regions, corresponding to transverse and longitudinal polarizations respectively, are the slab-adapted bulk phonon bands, while the solid line is a calculation for the Rayleigh wave based on the Dispersive Linear Chain Model (shown schematically in Fig. 35). The open circles at g = 0 are from Raman scattering experiments. (This figure has been corrected from Fig. 23 in Ref. 54.)... Figure 34. Surface phonon dispersion for 2H-TaSe2. The HAS data are shown as solid circles except for weak points which appear in the TOP spectra as hybridized longitudinal modes that are shown as crosses. All the data were obtained at 60 K, well into the low-temperature phase. The calculated striped and shaded regions, corresponding to transverse and longitudinal polarizations respectively, are the slab-adapted bulk phonon bands, while the solid line is a calculation for the Rayleigh wave based on the Dispersive Linear Chain Model (shown schematically in Fig. 35). The open circles at g = 0 are from Raman scattering experiments. (This figure has been corrected from Fig. 23 in Ref. 54.)...
Comments Cecid larvae pierce or tear growing hyphae, sucking out the contents. The main loss suffered by commercial growers is contamination of the mushrooms by larvae. H. p gmaea can also carry a bacterium which produces longitudinal brown stripes on the stem. In the infected mushrooms, tiny black droplets of fluid form on the gills, which then become spotted or turn black. [Pg.326]

Preedericksz transition in planar geometry is uniform in the plane of the layer and varies only in the z direction. However, in some exceptional cases, when the splay elastic constant Ki is much larger than the twist elastic constant K2 (e.g., in liquid crystal polymers), a spatially periodic out-of-plane director distortion becomes energetically favourable. The resulting splay-twist (ST) Freedericksz state is manifested in experiments in the form of a longitudinal stripe pattern running parallel to the initial director alignment no x. [Pg.103]

Patterns in nematics are easily observed by optical means where the anisotropy of the refractive index is exploited. In this way the stripe patterns in electroconvection in the planar geometry are easily discriminated from flexodomains the angle a between the wave vector q of the EC stripes and the preferred direction no a is small (normal or oblique rolls) in contrast to a = 90° (longitudinal stripes) in flexodomains. [Pg.104]

A method for the fabrication of a multi-wall package has been described (19). The package consists of biodegradable paper layers, and sheets of adherent films. The film sheet may consist of a corn derivative or PLA. Further, stripes are positioned in such a way that the package is more easily foldable in a lateral direction than in a longitudinal direction. [Pg.206]

The final term in Eq. (1) is the astigmatism factor, K. This accounts for the enhanced coupling of the spontaneous emission to longitudinal modes of the laser. This can be a significant factor in many structures, especially narrow stripe devices in which the gain profile is primarily responsible for the definition of the optical mode, where K = 11 has been observed.However, in single-mode, index-guided SL s, typically, K is very close to unity. [Pg.134]


See other pages where Stripe longitudinal is mentioned: [Pg.125]    [Pg.126]    [Pg.454]    [Pg.125]    [Pg.126]    [Pg.454]    [Pg.182]    [Pg.103]    [Pg.32]    [Pg.220]    [Pg.34]    [Pg.10]    [Pg.14]    [Pg.188]    [Pg.182]    [Pg.87]    [Pg.110]    [Pg.349]    [Pg.212]    [Pg.201]    [Pg.451]    [Pg.464]    [Pg.381]    [Pg.204]    [Pg.285]    [Pg.21]    [Pg.23]    [Pg.175]    [Pg.131]    [Pg.173]    [Pg.563]    [Pg.49]    [Pg.50]    [Pg.105]    [Pg.414]    [Pg.172]    [Pg.71]    [Pg.254]   
See also in sourсe #XX -- [ Pg.105 ]




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