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A Quantum Solution

Similar modelling has been performed for both of these systems, based on the cube model. Following Hand and Harris, the molecular motion was coupled to the surface oscillator via a rigid shift of the Z-coordinate in the PES, i.e. V(Z, r,. .., y) = V(Z — y, r...), where y is the oscillator coordinate. For the H2/Pd system [80], six molecular degrees-of-freedom were included in a classical treatment, while four molecular degrees-of-freedom were included in a quantum solution for the H2/Cu system [81, 82]. In the classical calculations, the surface temperature dependence was introduced by sampling the surface vibration from a Boltzmann distribution. In quantum calculations, this is not possible, and many calculations were required, each in a different initial surface oscillator state. The results... [Pg.42]

Xq is the origin of the path corresponding to t = 0, or 1, and aj is the th Fourier variable, t describes the evolution along the path and progresses from 0 to 1. Then the quantum potential distribution theorem (Beck, 1992 Beck and Marchioro, 1993 Wang et al, 1997 Beck, 2006) for a quantum solute with no internal structure is... [Pg.56]

The quantum communication protocols described above may be used to implement quantum counterparts to the classical solutions of cryptographic tasks mentioned in Section VIII.A. Until now most of the efforts were devoted to a quantum solution of the key-distribution problem, which may readily be applied to secure message exchange or can be used as a building block for different cryptographic schemes. [Pg.571]

In this review, almost all of the simulations we have described use only classical mechanics to describe the nuclear motion of the reaction system. However, a more accurate analysis of many reactions, including some of the ones that have already been simulated via purely classical mechanics, will ultimately require some infusion of quantum mechanical methods. This infusion has already taken place in several different types of reaction dynamics electron transfer in solution, > i> 2 HI photodissociation in rare gas clusters and solids,i i 22 >2 ° I2 photodissociation in Ar fluid,and the dynamics of electron solvation.22-24 Since calculation of the quantum dynamics of a full solvent is at present too time-consuming, all of these calculations involve a quantum solute in a classical solvent. (For a system where the solvent is treated quantum mechanically, see the quantum Monte Carlo treatment of an electron transfer reaction in water by Bader et al. O) As more complex reaaions are investigated, the techniques used in these studies will need to be extended to take into account effects involving electron dynamics such as curve crossing, the interaction of multiple electronic surfaces and other breakdowns of the Born-Oppenheimer approximation, the effect of solvent and solute polarization, and ultimately the actual detailed dynamics of the time evolution of the electronic degrees of freedom. [Pg.137]

A more logical response would be looking for a relativistic, rather than a quantum, solution of the cosmological problem in order to avoid the big-bang singularity in a natm-al way. Twenty years ago Maddox (1989) recommended ... [Pg.216]

A proximity focused image intensifier appears therefore as a good solution for both low and high energy applications it combines a sufficient gain to avoid noisy images due to a the quantum sink without some drawbacks of standard image intensifier. [Pg.596]

It should be noted that in the cases where y"j[,q ) > 0, the centroid variable becomes irrelevant to the quantum activated dynamics as defined by (A3.8.Id) and the instanton approach [37] to evaluate based on the steepest descent approximation to the path integral becomes the approach one may take. Alternatively, one may seek a more generalized saddle point coordinate about which to evaluate A3.8.14. This approach has also been used to provide a unified solution for the thennal rate constant in systems influenced by non-adiabatic effects, i.e. to bridge the adiabatic and non-adiabatic (Golden Rule) limits of such reactions. [Pg.893]

Figure A3.9.2. Interaction potential for an atom or molecule physisorbed on a surface. A convenient model is obtained by squaring off the potential, which facilitates solution of the Sclirodinger equation for the scattering of a quantum particle. Figure A3.9.2. Interaction potential for an atom or molecule physisorbed on a surface. A convenient model is obtained by squaring off the potential, which facilitates solution of the Sclirodinger equation for the scattering of a quantum particle.
The quantum solution to this problem is much more difficult for a number of reasons. First, it is important to know how to define what we mean by a particle moving in a given direction when V(x) is constant. Secondly, one must detemime the probability that the particle is moving in any specified direction at any desired... [Pg.958]

Heath J R and LeGoues F K 1993 A liquid solution synthesis of single crystal germanium quantum wires Chem. Phys. Lett. 208 263... [Pg.2917]

In a way, the limit set is thus the entire funnel between the two extreme cases qlc, and g o, Fig. 5. This effect is called Takens-chaos, [21, 5, 7]. As a consequence of this theorem each momentum uncertainty effects a kind of disintegration" process at the crossing. Thus, one can reasonably expect to reproduce the true excitation process by using QCMD trajectory bundles for sampling the funnel. To realize this idea, we have to study the full quantum solution and compare it to suitable QCMD trajectory bundles. [Pg.390]

Fig. 3. Quantum solution of the test system of 3.3 for e = 1/100. computed numerically using Fourier pseudospectral methods in space and a syraplectic discretization in time. Reduced g -density f t)j dg versus t and qF Initial... Fig. 3. Quantum solution of the test system of 3.3 for e = 1/100. computed numerically using Fourier pseudospectral methods in space and a syraplectic discretization in time. Reduced g -density f t)j dg versus t and qF Initial...
Semi-empirical methods could thus treat the receptor portion of a single protein molecule as a quantum mechanical region but ab mdio methods cannot. However, both semi-empirical and ab initio methods could treat solvents as a perturbation on a quantum mechanical solute. In the future, HyperChem may have an algorithm for correctly treating the boundary between a classical region and an ab mdio quantum mechanical region in the same molecule. For the time being it does not. [Pg.109]

In aqueous solution, riboflavin has absorption at ca 220—225, 226, 371, 444 and 475 nm. Neutral aqueous solutions of riboflavin have a greenish yellow color and an intense yellowish green fluorescence with a maximum at ca 530 nm and a quantum yield of = 0.25 at pH 2.6 (10). Fluorescence disappears upon the addition of acid or alkah. The fluorescence is used in quantitative deterrninations. The optical activity of riboflavin in neutral and acid solutions is [a]=+56.5-59.5° (0.5%, dil HCl). In an alkaline solution, it depends upon the concentration, eg, [a] J =—112-122° (50 mg in 2 mL 0.1 Ai alcohohc NaOH diluted to 10 mL with water). Borate-containing solutions are strongly dextrorotatory, because borate complexes with the ribityl side chain of riboflavin = +340° (pH 12). [Pg.75]

However, theories that are based on a basis set expansion do have a serious limitation with respect to the number of electrons. Even if one considers the rapid development of computer technology, it will be virtually impossible to treat by the MO method a small system of a size typical of classical molecular simulation, say 1000 water molecules. A logical solution to such a problem would be to employ a hybrid approach in which a chemical species of interest is handled by quantum chemistry while the solvent is treated classically. [Pg.418]

Plutonium(IV), in perchloric acid with ethanol present, is stable under dark conditions but produces Pu(III) when the solution is exposed to UV light. A quantum yield of 0.03 was reported (3 ) for the reaction,... [Pg.267]

The beating of a faint source with a high power coherent source is a well known process to detect its phase and amplitude. The same detection equipment allows the evaluation of the power of the source with theoretical limits similar to a noiseless photon counter. Such detection apparatus are limited by the bandwidth of the electronic component as this bandwidth is rapidly increasing, this may be a competitive solution for quantum limited detection in the far infra red. The phase of a thermal source is an useless information ... [Pg.372]

Historical prelude Kepler s laws Historical prelude Maxwell Theory Axiomatic teaching of Quantum Mechanics Problem lack of reference points Problem imprecise boundaries Problem inaccurate formulation Solution reference points from a journey Solution precise boundaries Solution accurate formulation Intuitive teaching of Quantum Mechanics Conclusion... [Pg.21]

The first reaction filmed by X-rays was the recombination of photodisso-ciated iodine in a CCI4 solution [18, 19, 49]. As this reaction is considered a prototype chemical reaction, a considerable effort was made to study it. Experimental techniques such as linear [50-52] and nonlinear [53-55] spectroscopy were used, as well as theoretical methods such as quantum chemistry [56] and molecular dynamics simulation [57]. A fair understanding of the dissociation and recombination dynamics resulted. However, a fascinating challenge remained to film atomic motions during the reaction. This was done in the following way. [Pg.274]

Chlorine-enhancement may offer a partial solution. The addition of the chlorinated olefin TCE, PCE, or TCP to air/contaminant mixtures has recently been demonstrated to increase quantum yields substantially [1, 2, 6]. We recently have extended this achievement [3], to demonstrate TCE-driven high quantmn efficiency conversions at a reference feed concentration of 50 mg contaminant/m air not only for toluene but also for other aromatics such as ethylbenzene and m-xylene, as well as the volatile oxygenates 2-butanone, acetaldehyde, butsraldehyde, 1-butanol, methyl acrylate, methyl-ter-butyl-ether (MTBE), 1,4 dioxane, and an alkane, hexane. Not 1 prospective contaminants respond positively to TCE addition a conventional, mutual competitive inhibition was observed for acetone, methanol, methylene chloride, chloroform, and 1,1,1 trichloroethane, and the benzene rate was altogether unaffected. [Pg.436]

Instead of postulating Zn," as intermediate, as it has a highly negative potential and is possibly unstable in ZnO, one may write the above mechanism with Zn e pairs. The blue-shift in the absorption upon illumination was explained by the decrease in particle size. The Hauffe mechanism was abandoned after it was recognized that an excess electron on a colloidal particle causes a blue-shift of the absorption threshold (see Fig. 19). In fact, in a more recent study it was shown that the blue-shift is also produced in the electron transfer from CH2OH radicals to colloidal ZnO particles When deaerated propanol-2 solutions of colloidal ZnO were irradiated for longer times, a black precipitate of Zn metal was formed. In the presence of 10 M methyl viologen in the alcohol solution, MV was produced with a quantum yield of 80 %... [Pg.162]


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