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Limitations linear polarization

Other limitations of this instrument are the same as those of linear polarization instruments discussed earlier. [Pg.1314]

Steady-State Fluorescence Depolarization Spectroscopy. For steady state depolarization measurements, the sample is excited with linearly polarized lig t of constant intensity. Observed values of P depend on the angle between the absorption and emission dipole moment vectors. In equation 2 (9), Po is the limiting value of polarization for a dilute solution of fluorophores randomly oriented in a rigid medium that permits no rotation and no energy transfer to other fluorophores ... [Pg.183]

A simplification of the polarization resistance technique is the linear polarization technique in which it is assumed that the relationship between E and i is linear in a narrow range around E . Usually only two points ( , 0 are measured and B is assumed to have a constant value of about 20 mV. This approach is used in field tests and forms the basis of commercial corrosion rate monitors. Rp can also be determined as the dc limit of the electrochemical impedance. Mansfeld et al. used the linear polarization technique to determine Rp for mild steel sensors embedded in concrete exposed to a sewer environment for about 9 months. One sensor was periodically flushed with sewage in an attempt to remove the sulfuric acid produced by sulfur-oxidizing bacteria within a biofilm another sensor was used as a control. A data logging system collected Rp at 10-min intervals simultaneously for the two corrosion sensors and two pH electrodes placed at the concrete surface. Figure 2 shows the cumulative corrosion loss (Z INT) obtained by integration of the MRp time curves as ... [Pg.211]

The dipole is, in principle, a space vector but the response is usually concentrated along a prefered axis. In the case of a laser excitation, for example, the dipole motion is concentrated along the laser polarization axis (when a linearly polarized laser is used) which me will then take as z axis. Note that in the definition Eq. (9), the space integration is limited to an analyzing volume V. We take in practice a region with a broad margin of 2-3 Wigner-Seitz radii rs around the cluster volume [24], For details on the interest and impact (or rather the lack of impact) on the spectral analysis, as well as on the ionization (section 2.2.2), see [21],... [Pg.94]

Polarization of the CMB was shown to be < 300 fiK (Lubin and Smoot, 1981). This observation used a differential polarimeter that was only sensitive to linear polarization. COBE put a limit of < 15 fiK on the polarization anisotropy. The linear polarization of the CMB was first detected by DASIPOL (Kovac et al., 2002), and the cross-correlation of the temperature and polarization anisotropies was confirmed by WMAP (Kogut et al., 2003). [Pg.154]

The limiting values of aPo/aPo for arbitrary k and an infinitely large parameter x 00 equal, in the case of linearly polarized Q-absorption of light ... [Pg.55]

Fig. 3.4 shows aPo/aPo dependences for linear polarized (P, P)-type excitation (in the same geometry as shown in Fig. 3.3). It must be noted that aPo/aPo is positive for all ranks k the limiting values at y —> oo are also presented in Table 3.3. Fig. 3.4 shows aPo/aPo dependences for linear polarized (P, P)-type excitation (in the same geometry as shown in Fig. 3.3). It must be noted that aPo/aPo is positive for all ranks k the limiting values at y —> oo are also presented in Table 3.3.
Fig. 3.7. Spatial quantization of the angular momentum Ja with quantum number J" = 3 at Q-absorbtion (x = 2) of linearly polarized light with E z. The figures show the values of M" = p. The solid line indicates the spatial distribution of Ja in the classic limit (J —> oo). Fig. 3.7. Spatial quantization of the angular momentum Ja with quantum number J" = 3 at Q-absorbtion (x = 2) of linearly polarized light with E z. The figures show the values of M" = p. The solid line indicates the spatial distribution of Ja in the classic limit (J —> oo).
Kotlikov, E.N. and Chaika, M.P. (1983). Origin of orientation irradiation by linearly polarized nonresonant light. I. Description in the limits of classical-oscillator model, Optika i Spektroskopiya, 55, 242-245. [Opt. Spectrosc. (USSR), 55, 142-144],... [Pg.282]

Naturally, since this expression is for a property measured in the reference frame connected to the molecule, molecular rotations do not appear in this expression. The range of L in the summation Eq. (53) is 0... 2/m ix, and includes both odd and even values. In general, the MF PAD is far more anisotropic than the LF PAD, for which L = 0,2,4 in a two-photon linearly polarized pump-probe experiment in the perturbative limit. Clearly, the MF PAD contains far more detailed information than the LF PAD concerning the ionization dynamics of the molecule, as well as the structure and symmetry of the electronic state from which ionization occurs, since the partial waves that may interfere are no longer geometrically limited as they are for the LF PAD. The contributing MF ionization transition dipole components are determined by the laser polarization... [Pg.525]


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Linear limit

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