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Scatter azimuth angle

Beam coordinate system, XB, YB, and ZB a Cartesian coordinate system with the origin on the central ray of the incident flux at the sample surface, the XB axis in the PLIN and the ZB axis normal to the surface as shown in Fig. Al. Note The angle of incidence, scatter angle, and incident and scatter azimuth angles are defined with respect to the beam coordinate system ... [Pg.303]

Scatter azimuth angle (s) angle from XB axis to the projection of the scatter direction onto the XB-YB plane ... [Pg.303]

Figure A3.1.7. Direct and restituting collisions in the relative coordinate frame. The collision cylinders as well as the appropriate scattering and azimuthal angles are illustrated. Figure A3.1.7. Direct and restituting collisions in the relative coordinate frame. The collision cylinders as well as the appropriate scattering and azimuthal angles are illustrated.
Figure Bl.23.8. Scattering intensity of 2 keV Ne versus azimuthal angle 6 scans for Pt 110] in the (1 x 2) and (1 X 3) reconstructed phases. Scattering angle 0 = 28° and incident angle a = 6°. Figure Bl.23.8. Scattering intensity of 2 keV Ne versus azimuthal angle 6 scans for Pt 110] in the (1 x 2) and (1 X 3) reconstructed phases. Scattering angle 0 = 28° and incident angle a = 6°.
Figure Bl.23.9. Scattering intensity of 4 keV Ne versus azimuthal angle 8 for a Ni 110] surface in the clean (1 X 1), (1 X 2)-H missing row, and (2 x l)-0 missing row phases. The hydrogen atoms are not shown. The oxygen atoms are shown as small open circles. 0-Ni and Ni-Ni denote the directions along which O and Ni atoms, respectively, shadow the Ni scattering centre. Figure Bl.23.9. Scattering intensity of 4 keV Ne versus azimuthal angle 8 for a Ni 110] surface in the clean (1 X 1), (1 X 2)-H missing row, and (2 x l)-0 missing row phases. The hydrogen atoms are not shown. The oxygen atoms are shown as small open circles. 0-Ni and Ni-Ni denote the directions along which O and Ni atoms, respectively, shadow the Ni scattering centre.
Fig. 3.62. Examples ofTOF-SARS spectra for Kr scattering from CdS -time-of-flight spectrum, scans for the angle of incidence a, and the azimuthal angle S [3.149]. Fig. 3.62. Examples ofTOF-SARS spectra for Kr scattering from CdS -time-of-flight spectrum, scans for the angle of incidence a, and the azimuthal angle S [3.149].
S =(s,, lf) Scattering vector in polar coordinates (polar angle, y/ azimuthal angle). - See the preamble to this List of Abbreviations ... [Pg.13]

Figure 1. The physical arrangement of an oriented polymer sample in a neutron scattering experiment showing the scattering angle, 6, and the azimuthal angle, . Figure 1. The physical arrangement of an oriented polymer sample in a neutron scattering experiment showing the scattering angle, 6, and the azimuthal angle, <j>.
Figure 2. Scattering intensity versus azimuthal angle for a uniaxially oriented elastomer, X is 3, x is 0.2. Phantom network where , f is 3 A, f is 4 V, f is 10. Crosslink junctions fixed, X. Figure 2. Scattering intensity versus azimuthal angle for a uniaxially oriented elastomer, X is 3, x is 0.2. Phantom network where , f is 3 A, f is 4 V, f is 10. Crosslink junctions fixed, X.
We have yet to explain why Cext = 2G is not necessarily observed. To do so it will help if we consider a specific example. The scattering amplitude for a circular disk is independent of the azimuthal angle ... [Pg.110]

It is instructive to consider how p varies with scattering angle 0 for the two azimuthal angles 0° and 90°. For scattering directions in a plane perpendicular to the cylinder axis the phase function p 0,90°) is pe(0,90°)sin2(xsin ), where the envelope... [Pg.211]

The differential scattering cross section dCsc /dQ, a familiar quantity in atomic physics, is defined as the energy scattered per unit time into a unit solid angle about a direction —which may be specified by two angles, the scattering angle 6 and the azimuthal angle (see Fig. 3.3)—for unit incident irradiance. It is expressed in terms of the scattered irradiance Is(0, ), the incident irradiance /, and the distance r to the detector as... [Pg.383]

Fig. 4.7. Normalized scattered intensity vs. angle from surface normal for an azimuthal angle of 0 = 24° with a fixed angle of incidence of 45° on a stepped Pt(553) surface... Fig. 4.7. Normalized scattered intensity vs. angle from surface normal for an azimuthal angle of 0 = 24° with a fixed angle of incidence of 45° on a stepped Pt(553) surface...
Here I0 is the intensity of the x-ray beam, r0 = e2/mc2 is the classical electron radius (2.82 x 10 15 m)., P(9,) is the polarization of the x-rays it depends on the angle between the polarization and the scattering vector. For horizontally polarized x-rays, it takes the form P(0, < >) = 1 - sin220 sin2t)>, where 20 is the scattering angle and < > the azimuthal angle with respect to the vertical direction. The formfactor ) is the Fourier transform of the atomic electron density ... [Pg.343]

For the elastic scattering of a beam of unpolarized projectiles by an unpolarized target, the cross section has axial symmetry about the incident beam direction and therefore no dependence upon the azimuthal angle 4>, so that the differential elastic cross section is related to its integral counterpart by... [Pg.141]

Fig. 11.1. Center-of-mass or Jacobi coordinates R and r used to describe the fragmentation of a triatomic molecule ABC into A and BC. S and s are the centers-of-mass of ABC and BC, respectively, v is the relative velocity of the recoiling fragments in the center-of-mass system. The space-fixed z-axis is parallel to the vector Eo of the electric field, while the body-fixed z -axis is parallel to the scattering vector R at all times. The azimuthal angle ip, which is not indicated in the figure, describes rotation in the plane perpendicular to R. Fig. 11.1. Center-of-mass or Jacobi coordinates R and r used to describe the fragmentation of a triatomic molecule ABC into A and BC. S and s are the centers-of-mass of ABC and BC, respectively, v is the relative velocity of the recoiling fragments in the center-of-mass system. The space-fixed z-axis is parallel to the vector Eo of the electric field, while the body-fixed z -axis is parallel to the scattering vector R at all times. The azimuthal angle ip, which is not indicated in the figure, describes rotation in the plane perpendicular to R.

See other pages where Scatter azimuth angle is mentioned: [Pg.344]    [Pg.344]    [Pg.1635]    [Pg.1800]    [Pg.1806]    [Pg.1814]    [Pg.1816]    [Pg.1818]    [Pg.243]    [Pg.260]    [Pg.216]    [Pg.219]    [Pg.306]    [Pg.51]    [Pg.61]    [Pg.63]    [Pg.97]    [Pg.155]    [Pg.162]    [Pg.397]    [Pg.399]    [Pg.406]    [Pg.290]    [Pg.84]    [Pg.58]    [Pg.262]    [Pg.153]    [Pg.203]    [Pg.313]    [Pg.313]    [Pg.314]    [Pg.315]    [Pg.315]   
See also in sourсe #XX -- [ Pg.303 ]




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