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Range Interaction

A few groups replace the Lennard-Jones interactions by interactions of a different form, mostly ones with a much shorter interaction range [144,146]. Since most of the computation time in an off-lattice simulation is usually spent on the evaluation of interaction energies, such a measure can speed up the algorithm considerably. For example, Viduna et al. use a potential in which the interaction range can be tuned... [Pg.648]

Morse potential). The constant C is defined such that t/ (r) = 0 at the cutoff distance R. The interaction range is determined by the parameter a, which Viduna et al. choose very large, a = 24. Hence the cutoff distance can be made small (R = 1.25cr in [144]). This model was first used by Gerroff et al. [147] and is discussed in some detail in Chapter 12 of this book. [Pg.648]

D. Heskett, The interaction range in alkali metal-promoted systems, Surf. Sci. 199, 67-86 (1988). [Pg.472]

The final component of the AFM is the tip-sample approach mechanism. Bringing the probe tip and the sample within interaction range in a nondestructive manner involves mounting one surface on an approach mechanism with subangstrom sensitivity. Most approach devices normally combine some form of stepper or slider with single step sizes of the order of microns, with a piezo device providing displacements of the order of one tenth of an angstrom up to a maximum of several microns. In microscopy mode, the piezo device... [Pg.28]

The reaction of the tetranuclear mercuracarborand 166 with 2 or 3 equiv. of KNO3/I8-C-6 in acetone affords two different nitrate complexes namely [166-(N03)2(H20)]2 and [166-(N03)2]2 (Figures 15 and 16). In both cases, the nitrate anions are ligated to the mercury centers by Hg-O interactions ranging from 2.60 to 3.08 A. In [166-(N03)2]2, the two anions coordinate with all four mercury atoms in a face-on trihapto fashion from either side of the plane.216... [Pg.454]

The gradient-squared term in the above equation represents the energy of the interface separating the phases the constant C can be interpreted as a measure of the interaction range. The bulk potential /(< )) has the Landau-Ginzburg (GL) 4>4 (double-well) structure... [Pg.176]

In the literature [55], typical energies involved in the nuclear quadrupole moments -crystalline electric field gradient interactions range up to A E 2x 10-25 J. The measured AE seems to confirm the hypothesis that the excess specific heat of the metallized wafer is due to boron doping of the Ge lattice. [Pg.302]

The concept of turbulent reacting flows encompasses many different meanings and depends on the interaction range, which is governed by the overall character of the flow environment. Associated with various flows are different characteristic times, or, as more commonly used, different characteristic lengths. [Pg.215]

The involvement of specific attractive interactions of molecules with the electrode surface (adsorption) makes the electrode process even more complex. The intensity of such interactions ranges from weak (physisorption) to strong (chemical bonds formed between adsorbate and electrode). [Pg.6]

For thick substrates, backscattered electrons from the substrate decrease contrast and the minimum dimension increases to about 20 nm. For thick resists, and samples thick compared to the primary electron penetration range, electron scattering in the resist (forward scattering) and backscattering of electrons from the substrate, become more important than the electron interaction range. In these cases, exposure dose is sometimes altered according to the local pattern density to compensate for variations in the backscattered... [Pg.25]

Exercise. Justify (2.3) as follows. Let co be a volume element with diameter of the order of the interaction range between molecules. The probability for having in co the set sj of molecules needed for a reaction is, according to (1.1.5),... [Pg.173]

Figure 1. Diagram of the intensity / (W/cm2) vs. duration of laser pulse tp(s) with various regimes of interaction of the laser pulse with a condensed medium being indicated very qualitatively. At high-intensity and high-energy fluence 4> = rpI optical damage of the medium occurs. Coherent interaction takes place for subpicosecond pulses with tp < Ti, tivr. For low-eneigy fluence (4> < 0.001 J/cm2) the efficiency of laser excitation of molecules is very low (linear interaction range). As a result the experimental window for coherent control occupies the restricted area of this approximate diagram with flexible border lines. Figure 1. Diagram of the intensity / (W/cm2) vs. duration of laser pulse tp(s) with various regimes of interaction of the laser pulse with a condensed medium being indicated very qualitatively. At high-intensity and high-energy fluence 4> = rpI optical damage of the medium occurs. Coherent interaction takes place for subpicosecond pulses with tp < Ti, tivr. For low-eneigy fluence (4> < 0.001 J/cm2) the efficiency of laser excitation of molecules is very low (linear interaction range). As a result the experimental window for coherent control occupies the restricted area of this approximate diagram with flexible border lines.
A similar study of the magnetic susceptibilities of the Cu2(R2Dtc)2Cl2 complexes was reported by Furneaux (259) (R2 = Bz-n-Pr). In his analysis intradimer interactions ranging from 27 = -98 to 27 = -140 were reported for the different R groups and interdimer interactions were considered unimportant. [Pg.329]

We performed numerical simulations of the annihilation process for the Sierpinski gaskets up to the 12th stage, starting with 10 percent of all sites randomly filled with A particles and another 10 percent with B particles. We chose the interaction range ro = 4.27 (in units of the nearest-neighbor distance ao, which leads to the dimensionless initial reactant concentration n(0) = 1 (in units of r d, d = 1.585). Note, that time is still measured in units of... [Pg.313]

A common result of all the experiments is that most molecules quench the alkali resonance radiation very effectively with total cross sections ranging from 10 A2 to over 200 A2. However, if the molecule BC is replaced by a rare-gas atom, the quenching cross sections become very small at thermal energies. They are probably below 10 2 A2 for quenching by helium, neon, argon, krypton, and xenon.55 The latter result is easily understood in terms of Massey s adiabatic criterion.67 If Ar is a characteristic interaction range, v the impact velocity, and AE the energy difference between initial and final electronic states E(3p) and E(3s), respectively, then we must have a Massey parameter... [Pg.351]

This crossover theory has been repeatedly tested with regard to MC simulations of the 3D lattice gas with variable interaction range. For example, a recently developed MC algorithm [318] allows the ratio of t/Na to be varied over eight orders of magnitude to cover the full crossover region [319]. The crossover theory gives an excellent representation of these data [320]. [Pg.54]

Peculiarly enough, the rare-earth vibronic intensities depend on the concentration of the rare-earth ion [32]. From this effect an interaction range between the rare-earth ions of some 10 A can be estimated. The nature of this interaction is not yet clear, but covalency seems to play a role. [Pg.17]


See other pages where Range Interaction is mentioned: [Pg.653]    [Pg.2254]    [Pg.643]    [Pg.385]    [Pg.163]    [Pg.17]    [Pg.29]    [Pg.579]    [Pg.98]    [Pg.322]    [Pg.189]    [Pg.121]    [Pg.263]    [Pg.380]    [Pg.206]    [Pg.182]    [Pg.137]    [Pg.359]    [Pg.17]    [Pg.104]    [Pg.440]    [Pg.265]    [Pg.586]    [Pg.154]    [Pg.282]    [Pg.739]    [Pg.349]    [Pg.351]    [Pg.440]    [Pg.85]    [Pg.37]    [Pg.285]    [Pg.250]   
See also in sourсe #XX -- [ Pg.450 ]




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