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Long-range interaction problem

Therefore, the total energy per unit cell amounts to [Pg.475]

The formula is correct, but we can easily see that we are to be confronted with some serious problems. For example, the summation over nuclei represents a divergent series and we will get -l-oo. This problem appears only because we are dealing with an infinite system and we confront the long-range interactions. We have to manage the problem somehow. [Pg.475]

What is left to be clarified are some problems about how to go with N to infinity It will be soon shown how dangerous this problem is. [Pg.475]

We see from eqs. (9.65) and (9.74) that, despite using the translational q mme-try to simplify the problem, we may treat each k separately. There are an infinite [Pg.475]

Electronic Motion in the Mean Field Periodic Systems [Pg.476]


Sutton and Chen extended the potential to longer range to enable the study of certain problems such as the interactions between clusters of afoms [Sutton and Chen 1990]. Their objective was to combine the superior Fiimis-Sinclair description of short-range interactions with a van der Waals tail to model the long-range interactions. The form of the Sutton-Chen potential is ... [Pg.261]

The performance of VASP for alloys and compounds has been illustrated at three examples The calculation of the properties of cobalt dislicide demonstrates that even for a transition-metal compound perfect agreement with all-electron calculations may be achieved at much lower computational effort, and that elastic and dynamic properties may be predicted accurately even for metallic systems with rather long-range interactions. Applications to surface-problems have been described at the example of the. 3C-SiC(100) surface. Surface physics and catalysis will be a. particularly important field for the application of VASP, recent work extends to processes as complex as the adsorption of thiopene molecules on the surface of transition-metal sulfides[55]. Finally, the efficiciency of VASP for studying complex melts has been illustrate for crystalline and molten Zintl-phases of alkali-group V alloys. [Pg.80]

It was further pointed out by Rashin and Honig that the form of Eqs. (32) and (42) precludes significant dependence upon e once it is greater than roughly 30.88 However these equations also emphasize the importance of long-range interactions (1/2R 16 kcal/mole for R = 10 A), and the authors correctly anticipate the problems encountered in simulations due to the limited sizes of the... [Pg.64]

The problem of nonlocality due to instantaneous long-range interaction is now considered both in electromagnetic and in gravitational theory. [Pg.50]

Apart from the ill-definitiveness of the inverse vibrational problem two principal objections are usually posed against the standard VFF model [5], First, the neglect of the long range interactions is not always physically justified and often contradicts with the real electronic structure of the molecule under study. Second, the transferability of force-constants is still a disputable topic, especially when the force-constants are transferred between neutral molecules and the corresponding ionized forms, or between conformational isomers [6, 7],... [Pg.342]

DFT or the admixtures discussed so far give a good description. A brief mention of MP2 was given in the introduction and this extension of HF is able to treat the weak interactions of alkanes with zeolite frameworks [8]. However, this is likely to remain a computationally expensive option in the solid state. New functionals are appearing in this area specifically aimed at the long-range correlation problem and promise to advance the field further [135]. [Pg.385]


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Long range

Long-range interactions

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