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Polarization cooling vector

Figure 5. Total kinetic energy spectrum of the H + SH(X) fragments resulting from 213.3-nm photolysis of a jet-cooled sample of HjS. The photolysis laser was linearly polarized, with its e vector aligned perpendicular to the TOF axis. The energies corresponding to various rotational levels of the two spin-orbit components of the SH(X) t = 0 fragments are indicated via the combs positioned above the spectrum. Figure 5. Total kinetic energy spectrum of the H + SH(X) fragments resulting from 213.3-nm photolysis of a jet-cooled sample of HjS. The photolysis laser was linearly polarized, with its e vector aligned perpendicular to the TOF axis. The energies corresponding to various rotational levels of the two spin-orbit components of the SH(X) t = 0 fragments are indicated via the combs positioned above the spectrum.
The isotropic phase formed by achiral molecules has continuous point group symmetry Kh (spherical). According to the group representations [5], upon cooling, the symmetry Kh lowers, at first, retaining its overall translation symmetry T(3) but reduces the orientational symmetry down to either conical or cylindrical. The cone has a polar symmetry Coov and the cylinder has a quadrupolar one Dooh- The absence of polarity of the nematic phase has been established experimentally. At least, polar nematic phases have not been found yet. In other words, there is a head-to-tail symmetry taken into account by introduction of the director n(r), a unit axial vector coinciding with the preferred direction of molecular axes dependent on coordinate (r is radius-vector). [Pg.44]

Fig. 13.29 Bent-shape molecules form polar smectic layers in the polar plane xz with polarization (a). Upon cooling, the molecules can spontaneously acquire a tilt forward or back within the tilt plane yz. The stack of the layers may be either synclinic SmCs or anticlinic SmCA (b). Additionally, depending on the direction of polarization P both the synclinic and anticlinic structure may have uniform (ferroelectric Pp) or alternating (antiferroelectric P ) distribution of polarization within the stack. In the field absence there are four stractures marked by symbols below. Note that the leftmost structure is chiral SmC and rightmost structure is also chiral because, for any pair of neighbours, the directions of the tilt and polarization change together leaving the same handedness of the vector triple. In the electric field, the phase transitions fixjm chiral SmCAPA <> chiral SmCsPp and from racemic SmCsPA to racemic SmCAPp structures are possible (shown by ark arrows)... Fig. 13.29 Bent-shape molecules form polar smectic layers in the polar plane xz with polarization (a). Upon cooling, the molecules can spontaneously acquire a tilt forward or back within the tilt plane yz. The stack of the layers may be either synclinic SmCs or anticlinic SmCA (b). Additionally, depending on the direction of polarization P both the synclinic and anticlinic structure may have uniform (ferroelectric Pp) or alternating (antiferroelectric P ) distribution of polarization within the stack. In the field absence there are four stractures marked by symbols below. Note that the leftmost structure is chiral SmC and rightmost structure is also chiral because, for any pair of neighbours, the directions of the tilt and polarization change together leaving the same handedness of the vector triple. In the electric field, the phase transitions fixjm chiral SmCAPA <> chiral SmCsPp and from racemic SmCsPA to racemic SmCAPp structures are possible (shown by ark arrows)...

See other pages where Polarization cooling vector is mentioned: [Pg.384]    [Pg.384]    [Pg.1004]    [Pg.82]    [Pg.189]    [Pg.172]    [Pg.227]    [Pg.498]    [Pg.15]    [Pg.92]    [Pg.220]    [Pg.498]    [Pg.66]    [Pg.1084]    [Pg.122]    [Pg.1599]    [Pg.102]    [Pg.361]    [Pg.522]    [Pg.743]    [Pg.867]    [Pg.225]   
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