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Dispersion of radiation along the focal plane AB of a typical prism are shown in

Dispersion of radiation by a prism monochromator

Dispersion of Raman lines for the bond alternation mode in three different conjugated systems

Dispersion of rayon fibers after pellet opening during compounding - SEM cryo fracture surface of injection molded test specimen

Dispersion of regolith material by cratering. According to Shoemaker et al.26

Dispersion of sample zone caused by laminar flow and molecular diffusion.

Dispersion of smoke. Smoke diseharged eontinuously from a stack has an average concentration that is approximately Gaussian. This shape can be predicted from a diffusion theory. However, the smoke is dispersed much more rapidly than would be expected from diffusion coefficients.

Dispersion of spherical particles.

Dispersion of surface states for W along the FM line obtained by ARUPS and comparison with theory

Dispersion of surface states on W experimental photoemission results.

Dispersion of the 2D monolayer polariton

Dispersion of the acoustic sound velocities of TmSea32Tea6

Dispersion of the Brillouin shift f and linewidth To i or the two pentanediols as a function or temperature

Dispersion of the capacity ofann-type Ge electrode with p 25 ohm cm during anodic dissolution in 0.1 N HQ. 500 cps.

Dispersion of the carbon isotopic composition of the hermatypic scleractinian genera Acropora, Porites, and Montipora, all living in shallow-water, surface-reef environments at 18 different, widely-scattered localities. The length of the horizontal bar corresponds to the mean one standard deviation. Figures in parentheses indicate the number of individual coral specimens of the three genera analyzed .

Dispersion of the chirality specific pseudoscalar relative to for the SFG process in optically active l,l -bi-2-naphthol. Configuration Interaction Singles SOS calculation with the cc-pVDZ basis, damping 3000 cm

Dispersion of the colloidal slab in the FPM fluid. The plot presents the changes of the largest cluster size and thermodynamic pressure for the particle system with time. Simulation results come from FPM-MD two-level model.

Dispersion of the electro-optic hyperpolarizabUity for chromophores with different linear absorption properties

Dispersion of the electronic susceptibilities in Eq. as a function of wavevector q for an alternating Hiickel chain with 8 0.20, hopping integral t 1 and unit cell 2a 1. The staggered bond order dominates at 0. Source

Dispersion of the excited state absorption cross section compared with the picosecond photoinduced absorption spectrum in P30T PCBCa 1

Dispersion of the first-order hyperpolarizability 3 —Wq. Wi, -Oi in die two-states model

Dispersion of the grain size in the In O, and SnO films prepared using different methods,

Dispersion of the imaginary part f of the atomic form factor of uranium, f reaches about one third of the non-resonant atomic form factor f 92. This schematic representation has been taken from The International Tables of Crystallography, IV

Dispersion of the imaginary part f of the atomic form factor of uranium, f reaches nearly two-thirds of the non-resonant atomic form factor fp 92. The schematic representation has been taken from The International Tables of Crystallography IV. The dispersion of f shows strong peaks at the M,y and My absorption edges

Dispersion of the nonlinear optical susceptibility djs of DCANP. The curve is a theoretical fit using a two-level model for the nonlinear optical hypeipolarizability of the DCANP molecules.



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