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Electrons highly correlated

The second half of this review deals with newly developed branches of solid state physics. Here it is evident that ESR made major contributions to the physics of electronically highly correlated systems, like heavy-fermion systems and intermediate-valence compounds. In the latter compounds it still has to be proven that the low density of states, which have been detected experimentally, results from the so-called Kondo whole and is a characteristic feature of IVCs. Certainly a further interesting area of ESR will be the study of Kondo insulators. In KI a hybridization gap, as a consequence of the interaction of the band states with the f-electron system, develops at low temperatures. In KI a non-magnetic impurity will reveal an effective spin i and, hence, one expects that non-magnetic impurities become ESR active below a characteristic temperature. So far we are not aware of any ESR experiments of that type in Kondo insulators. [Pg.327]

AFM measures the spatial distribution of the forces between an ultrafme tip and the sample. This distribution of these forces is also highly correlated with the atomic structure. STM is able to image many semiconductor and metal surfaces with atomic resolution. AFM is necessary for insulating materials, however, as electron conduction is required for STM in order to achieve tiumelling. Note that there are many modes of operation for these instruments, and many variations in use. In addition, there are other types of scaiming probe microscopies under development. [Pg.310]

Calculations for Ceo in the LDA approximation [62, 60] yield a narrow band (- 0.4 0.6 eV bandwidth) solid, with a HOMO-LUMO-derived direct band gap of - 1.5 eV at the X point of the fee Brillouin zone. The narrow energy bands and the molecular nature of the electronic structure of fullerenes are indicative of a highly correlated electron system. Since the HOMO and LUMO levels both have the same odd parity, electric dipole transitions between these levels are symmetry forbidden in the free Ceo moleeule. In the crystalline solid, transitions between the direct bandgap states at the T and X points in the cubic Brillouin zone arc also forbidden, but are allowed at the lower symmetry points in the Brillouin zone. The allowed electric dipole... [Pg.47]

Wave-like properties cause electrons to be smeared out rather than localized at an exact position. This smeared-out distribution can be described using the notion of electron density Where electrons are most likely to be found, there is high electron density. Low electron density correlates with regions where electrons are least likely to be found. Each electron, rather than being a point charge, is a three-dimensional particle-wave that is distributed over space in... [Pg.474]

The amount of high precision experimental structural data on conjugated polyenes is limited. Some structure results are presented in Table 5. In gas electron diffraction studies it is difficult to determine closely spaced bond distances accurately, because these parameters are highly correlated with the corresponding vibrational amplitudes. Today it is possible to calculate the vibrational amplitudes accurately, if the vibrational frequencies are known. This was, however, not the case when the GED studies presented in Table 5 were carried out. The observed differences between the terminal and central C=C bonds in the GED studies of traw.s-l,3,5-hexatriene and c/s-l,3,5-hexatricne are probably too large29. A very accurate X-ray study of traw.s-l,3,5-hexatriene has, however, been carried out also in connection with the preparation of this chapter4. Figure 4 shows the molecular structures of trans-1,3-butadiene and trans-l,3,5-hexatriene as found in the crystal lattice. [Pg.34]

The hypothesis of a normal distribution is a strong limitation that should be always kept in mind when PCA is used. In electronic nose experiments, samples are usually extracted from more than one class, and it is not always that the totality of measurements results in a normally distributed data set. Nonetheless, PCA is frequently used to analyze electronic nose data. Due to the high correlation normally shown by electronic nose sensors, PCA allows a visual display of electronic nose data in either 2D or 3D plots. Higher order methods were proposed and studied to solve pattern recognition problems in other application fields. It is worth mentioning here the Independent Component Analysis (ICA) that has been applied successfully in image and sound analysis problems [18]. Recently ICA was also applied to process electronic nose data results as a powerful pre-processor of data [19]. [Pg.156]

It is also possible to employ highly correlated reference states as an alternative to methods that employ Hartree-Fock orbitals. Multiconfigu-rational, spin-tensor, electron propagator theory adopts multiconfigura-tional, self-consistent-field reference states [37], Perturbative corrections to these reference states have been introduced recently [38],... [Pg.140]

Another approach of this kind uses the approximate Brueckner orbitals from a so-called Brueckner doubles, coupled-cluster calculation [39, 40]. Methods of this kind are distinguished by their versatility and have been applied to valence ionization energies of closed-shell molecules, electron detachment energies of highly correlated anions, core ionization... [Pg.140]

There have been a number of improvements in techniques, and more convenient models have been formulated however, the basic approach of the pseudopotential total energy method has not changed. This general approach or standard modd is applicable to a broad spectrum of solid state problems and materials when the dec-trons are not too localized. Highly correlated electronic materials require more attention, and this is an area of active current research. However, considering the extent of the accomplishments and die range of applications (see Table 14.3) to solids, dusters, and molecules, this approach has had a major impact on condensed matter physics and stands as one of the pillars of the fidd. [Pg.262]

A small problem arises when the crystal thickness and temperature factors are refined simultaneously, because these parameters are highly correlated. Raising both the thickness and the temperature factors results in almost the same least-squares sum. This is not an artifact of the calculation method but lies in the behavior of nature. Increasing the Debye-Waller factor of an atom means a less peaked scattering potential, which in turn results in a less sharply peaked interaction with the ncident electron wave. It can be shown that a thickness of 5 nm anc B=2 will give about the same results as a thickness of 10 nm and B=6 A. ... [Pg.364]

As we mentioned before, G(s) is a structure dependent constant that describes the number of scissions per unit absorbed dose and in that sense can be compared to a photochemical quantum efficiency. The G(s) of a radiation-sensitive polymer is a figure of merit that can be used in comparing one material with another. There is a very high correlation between G(s) values to gamma radiation (the radiation most commonly used for determining G(s)) and high sensitivity for lithographic materials used in either electron beam, ion beam or x-ray exposure. [Pg.95]

In this work the electronic predissociation from the A,B and B states has been studied using a time dependent Golden rule approach in an adiabatic representation. The PES s previously reported[31 ] to simulate the experimental spectrum[22] were used. Non-adiabatic couplings between A-X and B-X were computed using highly correlated electroiric wavefunctions using a finite difference method, with the MOLPRO package[42]. [Pg.402]

A problem with the two correlations is that they are highly correlated with each other. Changing carrier concentration is changing the number of electrons in the Cu3dx2 y2-02p d band. Thus, we expect that the Cu-O distance in the Cu02 sheets will increase as the number of electrons increases regardless of whether the copper oxide is n-type or p-type. [Pg.729]


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