Conductivity, electronic optical

Starrost F, Krasovskll E E, Schattke W, Jockel J, Simon U, Adelung R and Kipp L 2000 Cetineltes electronic, optical, and conduction properties of nanoporous chalcogenoantimonates Phys. Rev. B 61 15 697... 

It should be emphasized that the electrochemical carbonization proceeds, in contrast to all other common carbonization reactions (pyrolysis), already at the room temperature. This fact elucidates various surprising physicochemical properties of electrochemical carbon, such as extreme chemical reactivity and adsorption capacity, time-dependent electronic conductivity and optical spectra, as well as its very peculiar structure which actually matches the structure of the starting fluorocarbon chain. The electrochemical carbon is, therefore, obtained primarily in the form of linear polymeric carbon chains (polycumulene, polyyne), generally termed carbyne. This can be schematically depicted by the reaction ... 

When the size of metals is comparable or smaller than the electron mean free path, for example in metal nanoparticles, then the motion of electrons becomes limited by the size of the nanoparticle and interactions are expected to be mostly with the surface. This gives rise to surface plasmon resonance effects, in which the optical properties are determined by the collective oscillation of conduction electrons resulting from the interaction with light. Plasmonic metal nanoparticles and nanostructures are known to absorb light strongly, but they typically are not or only weakly luminescent [22-24]. 

The electronic structure and hence optical properties of nanomaterials depend on the core size. For example, nanoparticles of core size >3 nm show surface plasmon resonance, which is due to the excitation of surface plasmons of nanoparticles by light. When the size of gold nanoparticles comes down to around 1 nm, which is equal to the de Broglie wavelength of the conduction electrons, the electronic bands... 

EXAMPLE 4.2 Sodium is a metal with a density of conduction electrons N = 2.65 X 10 cm f Determine (a) its plasma frequency, (b) the wavelength region of transparency, and (c) the optical density at very low frequencies for a Na sample of 1 mm thickness. 

The optical and electronic functions of polysilanes owe to their delocalized highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) that are occupied by holes and conduction electrons, respectively. The polymer does not show high conductivity or optical nonlinearity if the electrons or holes are localized on a small part of the polymer chain. To elucidate the structure of HOMO and LUMO is therefore important for the molecular design of polysilanes as functional materials. 

The shapes of the absorption band cease to be independent of size for particles smaller than about 26 A, which suggests that the bulk dielectric function is inapplicable. Indeed, the broadening and lowering of the absorption peak can be explained by invoking a reduced mean free path for conduction electrons (Section 12.1). Thus, the major features of surface modes in small metallic particles are exhibited by this experimental system of nearly spherical particles well isolated from one another. But when calculations and measurements with no arbitrary normalization are compared, some disagreement remains. Measurements of Doremus on the 100-A aqueous gold sol, which agree with those of Turkevich et al., are compared with his calculations in Fig. 12.18 the two sets of calculations are for optical constants obtained... 

The application of band theory to account for detailed electrical, optical and magnetic properties has so far had only limited success (28). Electronic conduction and optical absorption resulting in the onset of u.v.-visible opaqueness involve the transference of electrons from one ion to another, and it would therefore seem worth applying the principles of optical electronegativity to these problems. Any resulting correlations are expected to be of a much more qualitative nature than results given by applying band theory. 

Size effects in optics of M nanocrystals are caused by influence of a crystal surface on movement of conductivity electrons in alternating electromagnetic field. Under action of a field with frequency co oscillations of conductivity electrons, which unlike valent electrons are not bonded to cations of M crystal, are determined by the Eq. (3) [14]... 

Features of nanocrystals optics are shown in visible and near UV spectrum where absorption is determined by behavior of conductivity electrons [16, 17]. 

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