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Babinet principle

When a target crosses the baseline of a bistatic radar the RCS can be greatly enhanced. This is due to the forward scatter phenomenon or Babinets principle. Here the RCS of a target at the bistatic baseline is calculated from... [Pg.5]

Babinet principle. Identical diffraction patterns of a substance are produced by two diffraction screens one of which is the exact negative of the other. [Pg.116]

Especially in protein crystals, but also in other structures that show relatively large voids or cavities, one can find solvent molecules that do not show any order at all. Such solvent regions can be interpreted as a liquid that is amorphously frozen during data collection (assuming that you collect the data at low temperature as you always should). Following the Babinet Principle, this extreme case of disorder is described as bulk solvent and can be refined using a two-parameter approximation (Moews and Kretsinger, 1975). See Example 5.3.5. [Pg.59]

Figure 26 Schematic illustration of the two possible models of the lamellar stack of semirigid chain polymers. Left, stacks with thin crystals and thicker interlamellar amorphous regions. Right stacks with thicker crystals and thinner interlamellar amorphous regions. The ambiguity of the microstructural model Is due to the Babinet principle, which makes the scattering from the two structures indistinguishable. Figure 26 Schematic illustration of the two possible models of the lamellar stack of semirigid chain polymers. Left, stacks with thin crystals and thicker interlamellar amorphous regions. Right stacks with thicker crystals and thinner interlamellar amorphous regions. The ambiguity of the microstructural model Is due to the Babinet principle, which makes the scattering from the two structures indistinguishable.
An important group of nanoantennas are those based on the Babinet principle. A metal shape surrounded by dielectric and a dielectric-filled hole in metal with identical shape and size have identical diliiaction patterns. Thus bowtie shaped holes in metal can be used, two holes are a Babinet equivalent of a nanodimer, arrays of nanoholes are equivalent of arrays of nanoparticles, crossed arrays of nanoholes correspond to crossed arrays of nanoparticles, etc. [318]. [Pg.125]

Following the Babinet principle, we cannot exclude the possibility that Rg is a size of void (polymer-poor region) instead of cluster (polymer-rich region), since the scattering intensity is proportional to the square of tte Ap whether Ap is positive or negative cannot be judged by the present scattering experiments. A similar calculation with the void model is also possible, and will be described elsewhere. [Pg.222]

For this system, the Babinet principle is not valid as it contains polymers and solvent molecules. If one matches the scattering length of the solvents and the averaged one of the polymers ( bpoiy = Obo + (1- ) bn) according to bpoiy = bo ( zero contrast), the second term of eqn [39] does not contribute to the scattering and, consequently, the single-chain form factor can be determined according to... [Pg.340]

Keywords radar bistatic radar multistatic radar ambiguity function parasitic radar forward scatter Babinet s principle passive coherent location netted radar. [Pg.1]

Although we shall be interested primarily in diffraction by an opaque circular disk, no extra labor is entailed if the shape of the planar obstacle is unrestricted at this stage of our argument (Fig. 4.1a). It is more convenient to consider diffraction by a planar aperture, with the same shape and dimensions as the obstacle, in an otherwise opaque screen (Fig. 4.1b). If xp(P) is the value of the wave function at P when the aperture is in place, we can invoke Babinet s principle,... [Pg.108]

To account for the total directional scattering from a large sphere, effects of both diffraction and reflection must be considered. When a spherical particle is in the path of incident radiation, the diffracted intensity may be obtained from Babinet s principle, which states that the diffracted intensity is the same as that for a hole of the same diameter. The phase function for diffraction by a large sphere is given by [Van de Hulst, 1957]... [Pg.147]

Some attention has to be given to the degree of circular polarization y and thus to the creation of cpl. Two experimental principles are common the use of a quarter wavelength plate and the use of a Fresnel rhomb or a Solcil-Babinet compensator in a few experiments, radiation from a cyclotron after passage through a polarizing undulator was used. The degree of circular polarization is easily jeopardized when a X/4 plate is employed, as this is an interference device... [Pg.5]

Babinet s principle The sum of the fields diffracted by two complementary screens (corresponding to a situation in which the second screen is obtained from the first one by interchanging apertures and opaque portions) coincides with the field in the absence of any screen. [Pg.229]

Fraunhofer diiliraction applies to particles that are much larger than wavelength and for which all radiation that is incident on the particle surface is either absorbed or redirected by reflection and refraction. The only forward scattering results from the difiiraction at the edges of the particle. In that sense, the particle can be replaced by an opaque, planar obstacle. According to Babinet s principle, this is complementary to the dififaction at an aperture of the same shape. The amplitude function for that case is given as ... [Pg.318]

This equation expresses the phase lag between x-axis polarization and y-axis polarization when the light passes through normal to the sample. The polarizer and analyzer are placed normal to each other. They are placed at 45° with respect to the x andy axes. Botii components deviate by b only when they pass through the sample. Figure 10 illustrates the principle of the measiuement. Babinet s compensator is positioned between the sample... [Pg.400]

That the contrast factor is the square of the difference of the scattering amplitudes is equivalent to Babinet s principle in optics, which states that the diffraction pattern from an opaque body is identical to that from a hole of the same size and shape. For instance, a circular hole scatters like a circular disc of the same diameter. [Pg.55]

If we interchange the dielectric in the aperture opening and the thin film metal, we get a complementary structure, which is an antenna. Is there any relation between the resonance properties of the two structures If we assume that the aperture metal film is infinitesimally thick, and that the metal is a perfect electrical conductor (PEC), the aperture and the complementary antenna structure are connected by a form of Babinet s principle. Supgose that the aperture is illuminated by an incident electric field Ei The interaction with the aperture will set up a total electric field E. Now, suppose that the complementary antenna structure is illuminated by an incident magnetic field that is vectorially equal to the incident electric field in the aperture case. Thus, the mcident magnetic field in the anteima case is E. In this case, let H2 be the total magnetic field. The particular form of Babinet s principle states that... [Pg.92]


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See also in sourсe #XX -- [ Pg.124 ]




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Babinet’s principle

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