Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Density of states for

The density of states for a one-dimensional system diverges as 0. This divergence of D E) is not a serious issue as the integral of the density of states remains finite. In tliree dimensions, it is straightforward to show that... [Pg.93]

Figure Al.3.15. Density of states for silieon (bottom panel) as ealeulated from empirieal pseudopotential [25], The top panel represents the photoemission speetra as measured by x-ray photoemission speetroseopy [30], The density of states is a measure of the photoemission speetra. Figure Al.3.15. Density of states for silieon (bottom panel) as ealeulated from empirieal pseudopotential [25], The top panel represents the photoemission speetra as measured by x-ray photoemission speetroseopy [30], The density of states is a measure of the photoemission speetra.
Figure Al.3.19. Simplest possible critical point structure in the joint density of states for a given energy band. Figure Al.3.19. Simplest possible critical point structure in the joint density of states for a given energy band.
RRKM theory, since steps are expected in M( ) even if all the states of the reactant do not participate in p( ). However, if the measured tln-eshold rate constant k(Eo) equals the inverse of the accurate anliannonic density of states for the reactant (difficult to detemiine), RRKM theory is verified. [Pg.1034]

Bhuiyan L B and Hase W L 1983 Sum and density of states for enharmonic polyatomic molecules. Effect of bend-stretch coupling J. Chem. Phys. 78 5052-8... [Pg.1040]

Fig. 20. Electronic 1D density of states per unit cell of a 2D graphene sheet for two (n, 0) zigzag nanotubes (a) the (10,0) nanotube which has semiconducting behavior, (b) the (9, 0) nanotube which has metallic behavior. Also shown in the figure is the density of states for the 2D graphene sheet (dotted line) [178]. Fig. 20. Electronic 1D density of states per unit cell of a 2D graphene sheet for two (n, 0) zigzag nanotubes (a) the (10,0) nanotube which has semiconducting behavior, (b) the (9, 0) nanotube which has metallic behavior. Also shown in the figure is the density of states for the 2D graphene sheet (dotted line) [178].
Although still preliminary, the study that provides the most detailed test of the theory for the electronic properties of the ID carbon nanotubes, thus far, is the combined STM/STS study by Oik and Heremans[13]. In this STM/STS study, more than nine individual multilayer tubules with diameters ranging from 1.7 to 9.5 nm were examined. The 7-Fplots provide evidence for both metallic and semiconducting tubules[13,14]. Plots of dl/dV indicate maxima in the ID density of states, suggestive of predicted singularities in the ID density of states for carbon nanotubes. This STM/ STS study further shows that the energy gap for the semiconducting tubules is proportional to the inverse tubule diameter l/<7, and is independent of the tubule chirality. [Pg.32]

Fig. 4. Calculated density of states for two zigzag individual SWCNTs with (a) semiconducting (10, 0) and (b) metallic (9, 0) configurations. Tight-binding approximation was used for the calculation [6]. Fig. 4. Calculated density of states for two zigzag individual SWCNTs with (a) semiconducting (10, 0) and (b) metallic (9, 0) configurations. Tight-binding approximation was used for the calculation [6].
Fig. 8.7 Superposition of density-of-states for B-N bonding BN>. states with corresponding metal states, reflected by their valence states from alkaline-earth (as Ca), lanthanide (as La), and 3d-metal (as Ni), and corresponding block schemes... Fig. 8.7 Superposition of density-of-states for B-N bonding BN>. states with corresponding metal states, reflected by their valence states from alkaline-earth (as Ca), lanthanide (as La), and 3d-metal (as Ni), and corresponding block schemes...
Fig. 9.10 CASTER densities of states for LigZn2Ge3. Nonbonding electron density distribution over selected bunches of crystal orbitals in the valence-band dispersion (a) six orbitals between -2.4 and -0.7 eV, (b) four orbitals ranging from -3.3 to -1.9 eV. Fig. 9.10 CASTER densities of states for LigZn2Ge3. Nonbonding electron density distribution over selected bunches of crystal orbitals in the valence-band dispersion (a) six orbitals between -2.4 and -0.7 eV, (b) four orbitals ranging from -3.3 to -1.9 eV.
Figure 6.12. Energy as a function ofthe reciprocal wave vector and the density of states for a free electron gas. Figure 6.12. Energy as a function ofthe reciprocal wave vector and the density of states for a free electron gas.
Why is the d-band of a metal narrower at the surface than in the interior Draw a simple version of the density of states for the electron bands of a metal (a good conductor), a semiconductor and a perfect insulator. [Pg.408]

Figure 4. Electrons in a three-dimensional bulk metal, (a) The energy of electrons varies with the square of the wave number. Dependence on k is described by a parabola, (b) Density of states for free electrons is quasi-continuous. (Reprinted from Ref. [5], 2004, with permission from Wiley-VCH.)... Figure 4. Electrons in a three-dimensional bulk metal, (a) The energy of electrons varies with the square of the wave number. Dependence on k is described by a parabola, (b) Density of states for free electrons is quasi-continuous. (Reprinted from Ref. [5], 2004, with permission from Wiley-VCH.)...
Figure 1. Density of states for various Ag clusters computed for 4d-, 5 s-, and 5p-orbitals within the extended Hiickel method. (Reprinted from Ref [32], 1981, with permission from Elsevier.)... Figure 1. Density of states for various Ag clusters computed for 4d-, 5 s-, and 5p-orbitals within the extended Hiickel method. (Reprinted from Ref [32], 1981, with permission from Elsevier.)...
The valence DOS has been computed for Ni and Ag clusters within the CNDO formalism. Blyholder [54] examined the Nis and M13 clusters. In both cases of s- and p-orbitals are occupied and lie well below the d-orbitals. Most of the intensity is near the middle of the d-orbitals with a fall-off in intensity as the HOMO is approached. Density of states for Agv, Agio, Agi3, and Agig clusters shows a strong d-component cc. 3.5 eV wide. The... [Pg.83]

The DOS diagram results from the superposition of the densities of states of the different bands (Fig. 10.10). The dxy band is narrow, its energy levels are crowded, and therefore it has a high density of states. For the wide dz2 band the energy levels are distributed over a larger interval, and the density of states is smaller. The COOP contribution of every... [Pg.98]

Figure 4.3 Density of states for (a) metal and (b) semiconductor nanocrystals. The HOMO-LUMO gap increases in semiconductor nanocrystals of smaller sizes. Adapted from [19], reproduced with permission from Wiley-VCH Verlag GmbH. Figure 4.3 Density of states for (a) metal and (b) semiconductor nanocrystals. The HOMO-LUMO gap increases in semiconductor nanocrystals of smaller sizes. Adapted from [19], reproduced with permission from Wiley-VCH Verlag GmbH.
Wang, F. Landau, D. P., Determining the density of states for classical statistical models a random walk algorithm to produce a flat histogram, Phys. Rev. E 2001, <54, 05 6101... [Pg.117]

Figure 5. Energy bands (—), dipole transition moment (- -), and density of states (—) for bond alternated chain. Figure 5. Energy bands (—), dipole transition moment (- -), and density of states (—) for bond alternated chain.
Fig. 3. Sketch of the energy dependence of the density of states for unhydrogenated amorphous silicon and hydrogenated amorphous silicon (Madan et al., 1976). Fig. 3. Sketch of the energy dependence of the density of states for unhydrogenated amorphous silicon and hydrogenated amorphous silicon (Madan et al., 1976).
As a rule, the density of states for molecular lattice vibrations is negligible as compared to that for crystal phonons. Therefore, the K-mode of a molecular lattice is coupled with the crystal phonons specified by the same wave vector K. Besides, the low-frequency collective mode m of adsorbed molecules can be considered as a... [Pg.175]

With this new cell geometry for planar electrodes the threshold energy is no longer dependent on the degree of electronic compensation for the IR drop and always coincides closely with the excitation energy. Therefore, these spectra are more likely to represent the true joint optical density of states for the system than those reported previously /1-4/. Consequently, this data does merit more rigorous interpretation with respect to the spectral distribution of the emitted light and the polarisation dependence of the emission. [Pg.241]


See other pages where Density of states for is mentioned: [Pg.115]    [Pg.1012]    [Pg.1019]    [Pg.1021]    [Pg.1029]    [Pg.1033]    [Pg.1689]    [Pg.72]    [Pg.53]    [Pg.213]    [Pg.67]    [Pg.147]    [Pg.413]    [Pg.194]    [Pg.246]    [Pg.4]    [Pg.101]    [Pg.43]    [Pg.166]    [Pg.101]    [Pg.101]    [Pg.404]    [Pg.251]    [Pg.93]    [Pg.251]    [Pg.254]   


SEARCH



Density of states

State density

© 2024 chempedia.info