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Polarisation response

For each sample two sets of measurements were performed, using geometry 1 and 2, respectively. Only measurements made in geometry 1 will be described here [21]. The time resolved rotation (or ellipticity) and reflectivity signals were simultaneously recorded for different orientations of the pump quarter wave plate. In this paper, only the polarisation response on time scales of a few hundreds of femtoseconds is discussed. The rise of a transient reflectivity response with much longer relaxation time was used here only to verify the zero time delay position. [Pg.211]

Figure 6. The SIFE and SOKE contributions to the transient polarisation response (symbols are data points, and solid curves are fits to equation (4), as explained below) are shown with the pump-probe intensity cross-correlation for the different samples measured. Figure 6. The SIFE and SOKE contributions to the transient polarisation response (symbols are data points, and solid curves are fits to equation (4), as explained below) are shown with the pump-probe intensity cross-correlation for the different samples measured.
Early exposure to low levels of inhalant allergens in the absence of sufficient microbial exposure may trigger low zone tolerance resulting in either weak Thl-like immunity, or Th2-polarised responses. This may increase the risk for IgE sensitisation. [Pg.195]

The principles of nonlinear optics and the main techniques used to evaluate the second-order NLO properties are briefly presented here. Major details can be found in more specialised reviews and books. At the molecular level, the interaction between polarisable electron density and the alternating electric field of the laser light beam (E) induces a polarisation response (Afi) that can be expressed following Equation 1.1 ... [Pg.3]

Cyclic voltammetry (adsorption, monolayers) Potentiodynamic polarisation (passivation, activation) Cathodic reduction (thickness) Frequency response analysis (electrical properties, heterogeneity) Chronopotentiometry (kinetics)... [Pg.30]

In the operation of ferroelectric liquid crystal devices, the applied electric field couples directly to the spontaneous polarisation Ps and response times depend on the magnitude E Ps. Depending on the electronic structure (magnitude and direction of the dipole moment as well as position and polarity of the chiral species) and ordering of the molecules P can vary over several orders of magnitude (3 to 1.2 x 10 ), giving response times in the range 1-100 ps. [Pg.14]

Although the trend in the viscosity of the system tended to decrease, which facilitated filtration, a gel occasionally appeared during the filtration and a polarisation layer was always formed. The first line (1-5 h) of Figure 4 is based on an assay in which the filtration started after a reaction time of 1.5 hours, when there were still polymers and the viscosity of the system was high. A sharp decrease in the permeate flux was obtained because a gel appeared among the hollow fibers, as did a polarisation layer. The second line (4-11 h) of Figure 4 is from an assay in which the filtration started after a reaction time of 4.5 hours, when there were no polymers and the viscosity of the system was low. In this experiment no sharp decrease in the permeate flux was obtained and no gel appeared between the hollow fibers. Only the appearance of the polarisation layer was responsible for the decrease of the flux from 250 mL/h (initial flux) to almost 200 mL/h. [Pg.987]

Bancroft, A.J., Else, K.J. and Grencis, R.K. (1994) Low level infection of Trichuris muris significantly affects the polarisation of the CD4 response. European Journal of Immunology 24, 3113-3118. [Pg.365]

The question also arises as to where the chiral molecules came from. Were the L-amino acids or the D-sugars selected on the primeval Earth, or are exuaterresuial sources responsible for the homochirality This second possibility is dealt with by hypotheses on the effect of circularly polarised light, of extraterrestrial origin, on chiral molecules in the molecular clouds from which the solar system was formed. One such hypothesis was proposed by Rubenstein et al. (1983) and developed further by others, particularly A. W. Bonner (Bonner and Rubenstein, 1987) both scientists worked at Stanford University. The authors believe that the actual radiation source was synchrotron radiation from supernovae. The excess of one enantiomeric form generated by this irradiation process would have needed to be transported to Earth by comets and meteorites, probably during the bombardment phase around 4.2-3.8 billion years ago. [Pg.250]

The different interaction principles also explain why strongly IR-active vibrations typically exhibit weak Raman bands and vice versa, even if the selection rules would allow a vibration. If a strong dipole exists in a molecule, the electron cloud is strongly polarised. A change of polarisation in response to the electric field of a photon is therefore not very likely. [Pg.127]

Permeabilities measured for pure gases can serve as a rough guide for selection of membrane materials. For design, data must be obtained on gas mixtures, where selectivities are often found to be much lower than those calculated from pure-component measurements. This effect is often due to plasticisation of the membrane by sorption of the most soluble component of the gas. This allows easier penetration by the less-permeable components. The problem of concentration polarisation, which is often encountered in small-scale flow tests, may also be responsible. Concentration polarisation results when the retention time of the gas in contact with the membrane is long. This allows substantial depletion of the most permeable component on the feed side of the membrane. The membrane-surface concentration of that component, and therefore its flux through the membrane, decreases. [Pg.108]

Scheme 1.14 Possible mechanisms for the transfer of polarisation from parahydrogen onto cyclooctene via [Rh(COD)(dppb)] (a) and (b) are the possible intermediate dihydride species responsible for the polarisation transfer at cyclooctene. Scheme 1.14 Possible mechanisms for the transfer of polarisation from parahydrogen onto cyclooctene via [Rh(COD)(dppb)] (a) and (b) are the possible intermediate dihydride species responsible for the polarisation transfer at cyclooctene.

See other pages where Polarisation response is mentioned: [Pg.355]    [Pg.799]    [Pg.216]    [Pg.218]    [Pg.219]    [Pg.112]    [Pg.116]    [Pg.40]    [Pg.766]    [Pg.11]    [Pg.341]    [Pg.126]    [Pg.355]    [Pg.799]    [Pg.216]    [Pg.218]    [Pg.219]    [Pg.112]    [Pg.116]    [Pg.40]    [Pg.766]    [Pg.11]    [Pg.341]    [Pg.126]    [Pg.180]    [Pg.276]    [Pg.95]    [Pg.568]    [Pg.1162]    [Pg.1198]    [Pg.1239]    [Pg.1301]    [Pg.747]    [Pg.13]    [Pg.16]    [Pg.76]    [Pg.51]    [Pg.107]    [Pg.60]    [Pg.143]    [Pg.763]    [Pg.241]    [Pg.97]    [Pg.117]    [Pg.253]    [Pg.24]    [Pg.50]    [Pg.336]    [Pg.365]   
See also in sourсe #XX -- [ Pg.3 ]




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Polarisable

Polarisation

Polariser

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