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Incident beam

In this theory, the fundamental notion is the concept of beam introduced similarly to that ft om the geometrical optics. The faces of the discontinuity will reflect all the electromagnetic beams due to the zero conductivity of the air filling the discontinuity The edge of the discontinuity will diffract the incident beam similarly to the Fresnel diffraction in optics. [Pg.375]

The sound pressure P was produced at the point D by the ultrasonic sound source which was generated at the point B in "n" order of the munite area AA by the incident beam. The sound pressure P is given by the equation(l)... [Pg.905]

Studies of inelastic scattering are of considerable interest in heterogeneous catalysis. The degree to which molecules are scattered specularly gives information about their residence time on the surface. Often new chemical species appear, whose trajectory from the surface correlates to some degree with that of the incident beam of molecules. The study of such reactive scattering gives mechanistic information about surface reactions. [Pg.310]

SANS Small-angle neutron scattering [175, 176] Thermal or cold neutrons are scattered elastically or inelastically Incident-Beam Spectroscopy Surface vibrational states, pore size distribution suspension structure... [Pg.316]

Explain on what basis the condensation coefficient, c, might be expected to depend on cos 6, where 6 is the angle from the normal of an incident beam of particles (note Ref. 122). [Pg.742]

There is an aspect of nonlinear spectroscopy which we have so far neglected, namely the spatial dependence of the signal. In general, tln-ee incident beams, described by /c-vectors k, k2 and will produce an outgoing beam at each of the directions ... [Pg.256]

Figure A3.9.4. The ratio of specular reflectivity to incident beam intensity ratio for D2 molecules scattering from a Cii(lOO) surface at 30 K [21],... Figure A3.9.4. The ratio of specular reflectivity to incident beam intensity ratio for D2 molecules scattering from a Cii(lOO) surface at 30 K [21],...
CAHRS and CSHRS) [145, 146 and 147]. These 6WM spectroscopies depend on (Im for HRS) and obey the tlnee-photon selection rules. Their signals are always to the blue of the incident beam(s), thus avoiding fluorescence problems. The selection ndes allow one to probe, with optical frequencies, the usual IR spectrum (one photon), not the conventional Raman active vibrations (two photon), but also new vibrations that are synnnetry forbidden in both IR and conventional Raman methods. [Pg.1214]

Another mode of electron diffraction, low energy electron diffraction or FEED [13], uses incident beams of electrons with energies below about 100 eV, with corresponding wavelengths of the order of 1 A. Because of the very strong interactions between the incident electrons and tlie atoms in tlie crystal, there is very little penetration of the electron waves into the crystal, so that the diffraction pattern is detemiined entirely by the... [Pg.1367]

Figure Bl.9.2. Resolution of a plane unpolarized incident beam into polarized scattering components. Figure Bl.9.2. Resolution of a plane unpolarized incident beam into polarized scattering components.
At 20 = 0°, the scattering comprises both components of polarization of the incident beam at 29 = 90°, the scattering comprises only one half of the incident beam. Consequently, the scattered light at 90° will be plane polarized. [Pg.1389]

The temi is related to the incident beam, which is often omitted in the theoretical derivation (as... [Pg.1392]

Figure Bl.10.10. Schematic diagram of the effect of detector view angles on coincidence rate. The view angles of two detectors are shown along with the common view angle. Maximum signal collection efficiency is achieved when the individual view angles have the maximum overlap and when the overlap coincides with the maximum density of the incident beam. Figure Bl.10.10. Schematic diagram of the effect of detector view angles on coincidence rate. The view angles of two detectors are shown along with the common view angle. Maximum signal collection efficiency is achieved when the individual view angles have the maximum overlap and when the overlap coincides with the maximum density of the incident beam.
It is relatively straightforward to detemiine the size and shape of the three- or two-dimensional unit cell of a periodic bulk or surface structure, respectively. This infonnation follows from the exit directions of diffracted beams relative to an incident beam, for a given crystal orientation measuring those exit angles detennines the unit cell quite easily. But no relative positions of atoms within the unit cell can be obtained in this maimer. To achieve that, one must measure intensities of diffracted beams and then computationally analyse those intensities in tenns of atomic positions. [Pg.1752]

Classical ion trajectory computer simulations based on the BCA are a series of evaluations of two-body collisions. The parameters involved in each collision are tire type of atoms of the projectile and the target atom, the kinetic energy of the projectile and the impact parameter. The general procedure for implementation of such computer simulations is as follows. All of the parameters involved in tlie calculation are defined the surface structure in tenns of the types of the constituent atoms, their positions in the surface and their themial vibration amplitude the projectile in tenns of the type of ion to be used, the incident beam direction and the initial kinetic energy the detector in tenns of the position, size and detection efficiency the type of potential fiinctions for possible collision pairs. [Pg.1811]

Fixing the incident beam angle and rotating the crystal about tlie surface nonnal while monitoring the... [Pg.1814]

Figure Bl.24.1. Schematic diagram of the target chamber and detectors used in ion beam analysis. The backscattering detector is mounted close to the incident beam and the forward scattering detector is mounted so that, when the target is tilted, hydrogen recoils can be detected at angles of about 30° from the beam direction. The x-ray detector faces the sample and receives x-rays emitted from the sample. Figure Bl.24.1. Schematic diagram of the target chamber and detectors used in ion beam analysis. The backscattering detector is mounted close to the incident beam and the forward scattering detector is mounted so that, when the target is tilted, hydrogen recoils can be detected at angles of about 30° from the beam direction. The x-ray detector faces the sample and receives x-rays emitted from the sample.

See other pages where Incident beam is mentioned: [Pg.66]    [Pg.216]    [Pg.737]    [Pg.303]    [Pg.306]    [Pg.253]    [Pg.1199]    [Pg.1205]    [Pg.1309]    [Pg.1313]    [Pg.1364]    [Pg.1367]    [Pg.1368]    [Pg.1370]    [Pg.1385]    [Pg.1390]    [Pg.1391]    [Pg.1397]    [Pg.1432]    [Pg.1629]    [Pg.1636]    [Pg.1781]    [Pg.1803]    [Pg.1806]    [Pg.1806]    [Pg.1817]    [Pg.1829]    [Pg.1829]    [Pg.1838]    [Pg.1839]    [Pg.1849]    [Pg.1858]    [Pg.1881]    [Pg.1886]   
See also in sourсe #XX -- [ Pg.544 ]

See also in sourсe #XX -- [ Pg.258 ]




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Beam, light incident

Incident beam aperture

Incident beam characterization

Incident beam monitoring

Incident beam voltage

Incident electron beam, surface analysis

Incident laser beam

Incident neutron beam

Intensity of incident beam

Mean incident beam collimation

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