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Periodic calculation

Magnetic interactions in extended systems can also be studied without creating the more or less approximate representation of the material with an embedded cluster. The approach based on the translational symmetry in the crystal naturally leads to the well-known band stmctures of the Bloch functions, periodic one-electron functions. [Pg.193]

Correlated band structures Periodic single determinant approaches are well suited to give qualitative answers or to serve as benchmark for checking the validity of embedded cluster results. On the other hand, the accurate tfeatment of (sfrong) electron correlation effects in crystalline materials, for example to predict the subtle interplay of magnetism and electrical conductance, requires an accurate, balanced description of all states involved, and this is still a challenge. [Pg.196]

Within Green function theory, many-electron effects can be introduced through a non-local and energy-dependent self-energy operator [15]. Since the self-energy is hard to calculate, various approximations are introduced and among the simplest ones is the so-called GW approximation, which is derived from many-body perturbation theory. Although the GW approximation offers in principle a sophisticated account of the electron correlation effects, practical realizations are commonly also based on the LDA method. [Pg.197]

Finally, algorithms have been developed which incorporate electron correlation effects explicitly in wave function based band theory for crystalline solids [16, 17]. These algorithms construct the many-electron Hamiltonian matrix for a periodic system by extracting the matrix elements from calculations on finite embedded clusters. In this way the incorporation of correlation effects leads to many-electron energy bands, not only associated with hole states and added-electron states but also with excited states. More recently, Pisani and co-workers [18] introduced a post-Hartree-Fock program based on periodic local second order Mpller-Plesset perturbation theory. [Pg.197]

A word of warning is in place when these techniques are employed for the study of magnetic interactions. The tiny energy differences associated with these interactions demand that the procedure is capable to deliver not only an accurate but also a balanced treatment of the various states involved. This means that approximate computation and cut-offs of integrals etc. have to be exactly the same for all states. [Pg.197]


As Figure 4-108 shows, increasingly large cash flows develop in later years of operation. These large cash flows are essentially ignored by a simple payback period calculation. [Pg.219]

X-ray diffraction from cast films provide useful information of bilayer structure. Periodic peaks in small and middle-angle diffraction from cast films on glass plates are attributed to the reflections from (h, 0,0) planes of the multiple lamella structure. The spacing of higher order reflections (h > 1) satisfies with numerical relation of 1 / h of the long period calculated from the first order reflection =1), which is equivalent to the bilayer thickness. Every cast film measured in this experiment showed more than 6 reflection peaks. [Pg.58]

The shortest time known for a vessel to rupture from recorded incidents is thought to be 10 minutes. Rupture periods calculated for less than ten minutes should therefore not be assumed, as the historical evidence and the typical growth of a hydrocarbon fire would indicate that the immediate rupture of a vessel does not occur. Further investigations may be carried out verity if fire exposure conditions could produce such results (e.g., flange leak, gas fire exposures, etc.). [Pg.127]

The Bloeh mode ean be defined as a wave eorresponding to the eigenmode of the transfer matrix of one period of the strueture. Let A is the transfer matrix deseribing wave transition from the left to the right of one period, calculated by sueeessive applications of Eq. (13) to each section and Eq. (13) to each interface between sections within the period. The Bloch mode then has to satisfy the condition... [Pg.85]

Figure 4.3 View of a five layer slab model of a surface as used in a fully periodic calculation. In making this image, the supercell is similar to the one in Fig. 4.1 and is repeated 20 times in the x and y directions and 2 times in the z direction. Figure 4.3 View of a five layer slab model of a surface as used in a fully periodic calculation. In making this image, the supercell is similar to the one in Fig. 4.1 and is repeated 20 times in the x and y directions and 2 times in the z direction.
DFT calculations come in two variations cluster and periodic calculations. The difference is in the model of the system. Most calculations of lateral interactions have used periodic calculations, 25,63,76,79,160,174 177 ... [Pg.147]

An advantage of a cluster calculation for the lateral interactions is that one can sometimes make a model that definitely has only one type of lateral interaction. For example, if one wants to compute the pair interaction between two adsorbates, one simply puts just these two adsorbates on the cluster. With a periodic calculation this is not possible the periodicity always gives you an infinite number of adsorbates, and to get the pair interaction of interest one needs to make an assumption about the other lateral interactions that are in principle present. This means that in a periodic calculation one chooses one of... [Pg.148]

In addition to the cluster approach discussed in section 2, it can sometimes be advantageous to use periodic calculations to model bulk and surface phenomena. Some of the methods which we have found useful are described briefly below. [Pg.221]

Both the cluster and the periodic calculations indicate a similarity to the Newns-Anderson model for metal adsorbates, in that both energy shifts, and broadenings need to be included in models of electron transfer, as shown schematically in Fig. 13. It will be a challenge in the near future to incorporate the increasingly accurate calculations of the crucial electronic coupling-strength parameter in existing dynamical models of the surface electron transfer processes. [Pg.242]

Periodic calculations of intercalation, in particular in TiC>2 have successfully provided support and interpretations of several experiments designed to investigate fundamental properties of potential displays and batteries. [Pg.253]

The periodic calculations show good agreement with results of cluster calculations, with small deviations in the geometry parameters of the intercalated molecules and in the distances of hydrogen bonds as a consequence of distinct mutual interactions of intercalated DMSO molecules or interactions between the DMSO molecules and the surface of kaolinite. [Pg.363]

Perchloric acid (HCIO4) can be prepared as shown in the diagram below from Ba(ClGi)2 and HCIO4. Sulfuric acid is supplied in 20% excess to react with Ba(C104)2. If 17,400 lb HCIO4 leave the separator and the recycle is 6125 lb Ba(C104)2 over the time period, calculate ... [Pg.64]

It has been suggested that the gas be disposed of by burning with an excess of air. The gaseous combustion products are then emitted to the air through a smokestack. The local air pollution regulations say that no stack gas is to analyze more than 2 percent SCfc by an Orsat analysis averaged over a 24-hr period. Calculate the minimum percent excess air that must be used to stay within this regulation. [Pg.69]

Impurity and Aperiodicity Effects in Polymers.—The presence of various impurity centres (cations and water in DNA, halogens in polyacetylenes, etc.) contributes basically to the physics of polymeric materials. Many polymers (like proteins or DNA) are, however, by their very nature aperiodic. The inclusion of these effects considerably complicates the electronic structure investigations both from the conceptual and computational points of view. We briefly mentioned earlier the theoretical possibilities of accounting for such effects. Apart from the simplest ones, periodic cluster calculations, virtual crystal approximation, and Dean s method in its simplest form, the application of these theoretical methods [the coherent potential approximation (CPA),103 Dean s method in its SCF form,51 the Hartree-Fock Green s matrix (resolvent) method, etc.] is a tedious work, usually necessitating more computational effort than the periodic calculations... [Pg.84]

Theoretical simulations of the (VO)2P207 surface have advanced greatly in recent years. Periodic calculations, cluster models, and DFT methods have been employed to describe the surface active sites. FIow-ever, in our context, these methods have been extended only to modeling of the (100) surface of vanadyl pyrophosphate (155-159) and to simulation... [Pg.221]

In this part, we will summarize some of our results on the investigation of the toluene intramolecular isomerization pathways." " Both cluster approach and periodic approach methods have been employed which allow giving an illustration of the consequence of the simplistic model in the cluster approach. H-Mordenite (H-MOR) zeolite is used for the periodic calculations. The toluene molecule does not have a problem to fit within the large 12-membered ring channels of this zeolite. Furthermore, the intramolecular transition states do not suffer from steric constraints. It is known that intramolecular aromatics isomerization can proceed via two different reaction pathways (see Figure 7). The first route proceeds through a methyl shift isomerization, whereas the second route involves a dealkylation or disproportionation reaction which results in the formation of a methoxy species and benzene as intermediate. [Pg.11]

Figure II. Reaction energy diagrams of the shift isomerization reaction of toluene catalyzed by acid zeolite. The diagrams using black lines refer to the cluster approach results, and the ones using gray lines to the periodic calculations results (in kJ/mol). ... Figure II. Reaction energy diagrams of the shift isomerization reaction of toluene catalyzed by acid zeolite. The diagrams using black lines refer to the cluster approach results, and the ones using gray lines to the periodic calculations results (in kJ/mol). ...
Figure 16. Front and side views of the transition states and intermediate for the isomerization reaction via disproportionation reaction pathway of xylene molecules catalyzed by an acidic Mordenite as obtained from the periodic calculations (American Chemical Society,... Figure 16. Front and side views of the transition states and intermediate for the isomerization reaction via disproportionation reaction pathway of xylene molecules catalyzed by an acidic Mordenite as obtained from the periodic calculations (American Chemical Society,...
We have shown here, with the support of selected examples, that periodic calculations have become possible on systems of interest. This allows for a deeper understanding of zeolite catalyst reactivity. The full range of the zeolite selectivity can now be investigated by theoretical methods. [Pg.24]

We start by giving a short report of the computational methods employed in our calculations, including a geometrical description of the systems investigated. We describe first the cluster calculations on silica based materials, followed by periodic calculations on noble metals supported on oxides. The results for both systems yield detailed information on structure and bonding on these complexes. [Pg.112]

Data Processing derived values, data conversions, scaling, frequencies, periods, calculations, algorithms, validity checks, error correction... [Pg.208]

The goal of periodic calculations is to generate a reliable estimate for the electron density of the unit cell. However, many chemical concepts of bonding rely on ideas that are not so easily defined, such as atomic charges with which to quanhfy the ionicity of the system. The expression for the electron density in terms of molecular orbitals Equation 8.16 does allow a partihoning of the charge density to be undertaken to access such quantities. In terms of the basis set the density can be re-written ... [Pg.339]

Converging the self-consistent procedure in periodic calculations can be a difficult task, particularly if there are free states within any band. Movement of electrons between almost identical states has little effect on the energy of the system and so the search for the optimal distribution of electrons is hampered by many trivial alterations to the occupation numbers. To make the process more efficient, partial occupancies can be used for states near the highest filled level by introducing a smoothing function which defines the occupancy as a function of state energy, Tj,. The smoothing function used in the MgO calculation was ... [Pg.344]

Two liquid streams are flowing at constant rates into a blender. One is benzene, which flows at a measured rate of 20.0 L/min, and the other is toluene. The blended mixture enters a storage tank (inner diameter = 5.5 m) equipped with a sight gauge. During an interval in which no liquid leaves the storage tank, the liquid level in the tank is observed to increase by 0.15 meters over a one-hour period. Calculate the flow rate of toluene into the blender (L/min) and the composition of the tank contents (wl% benzene). [Pg.214]

Mauri s group have published a number of papers on calculated O NMR parameters. Ref. 167 is particularly interesting as it considers vibrational effects on the NMR shielding by averaging the chemical shift over fluctuations of the nuclear positions. They show that vibrational corrections are crucial to reproducing the temperature dependence of the chemical shift. Truflandier et al have published the first periodic calculations of NMR shielding for a transition metal nucleus, albeit on a d° system (V04 ). [Pg.133]


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See also in sourсe #XX -- [ Pg.115 ]




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