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Highly correlated vacuum

Knowing the values of n, we estimated the number of holes formed in the states of the highly correlated vacuum ( negative-energy states) [28]. [Pg.204]

In high energy heavy ion collisions it might be possible to produce antimatter clusters like d, He, etc. out of the highly correlated vacuum in contrast to their conventional production by fusing antibaryons, step by step, in phase space. [Pg.206]

The bound antinucleons are then pulled down into the (lower) continuum. In this way antimatter clusters may be set free. Of course, a large part of the antimatter will annihilate on ordinary matter present in the course of the expansion. However, it is important that this mechanism for the production of antimatter clusters out of the highly correlated vacuum does not proceed via the phase space. The required coalescence of many particles in phase space suppresses the production of clusters, while it is favored by the direct production out of the highly correlated vacuum. In a certain sense, the highly correlated vacuum is a kind of cluster vacuum (vacuum with cluster structure). The shell structure of the vacuum levels (see Figure 8.21) supports this latter suggestion. Figure 8.23 illustrates this idea. [Pg.120]

FIGURE 8.23 Due to the high temperature and the violent dynamics, many bound holes (antinucleon clusters) are created in the highly correlated vacuum, which can be set free during the expansion stage into the lower continuum. In this way, antimatter clusters can be produced directly from the vacuum. The horizontal arrow in the lower part of the figure denotes the spontaneous creation of baryon-antibaryon pairs, while the antibaryons occupy bound states in the lower potential well. Such a situation, where the lower potential well reaches into the upper continuum, is called supercritical. [Pg.121]

Modem quantum-chemical methods can, in principle, provide all properties of molecular systems. The achievable accuracy for a desired property of a given molecule is limited only by the available computational resources. In practice, this leads to restrictions on the size of the system From a handful of atoms for highly correlated methods to a few hundred atoms for direct Hartree-Fock (HF), density-functional (DFT) or semiempirical methods. For these systems, one can usually afford the few evaluations of the energy and its first one or two derivatives needed for optimisation of the molecular geometry. However, neither the affordable system size nor, in particular, the affordable number of configurations is sufficient to evaluate statistical-mechanical properties of such systems with any level of confidence. This makes quantum chemistry a useful tool for every molecular property that is sufficiently determined (i) at vacuum boundary conditions and (ii) at zero Kelvin. However, all effects from finite temperature, interactions with a condensed-phase environment, time-dependence and entropy are not accounted for. [Pg.82]

Cluster ions are fast ions. The masses of cluster ions may be measured with mass spectrometers, but the possible ion-molecule reactions during the passage of the air through nozzles to the vacuum chamber complicate the measurement. Mass and mobility of cluster ions are highly correlated. The experimented results can be expressed by the empirical formula... [Pg.2301]

One example of a halogen atom with a halogen molecule reaction is known where adiabatic formation of spin-orbit excited P n halogen atom product on the 2 A surface appears to be efficient, namely the l P p ) + IBr -> IBr -1- Bri Pij ) reaction. Houston [16], Wiesenfeld and Wolk [22,77], Spencer and Wittig [94], and Gordon et al. [76] demonstrated a high correlation of product Br( Py ) with reactant Kp Py ). Wiesenfeld and Wolk [22,77] have determined branching ratios for the reactive vs. nonreactive channels by vacuum ultraviolet absorption spectroscopy and found that ca. 80% of IpPy f ) reactive collisions yielded... [Pg.157]

Experiments on transport, injection, electroluminescence, and fluorescence probe the spatial correlation within the film, therefore we expect that their response will be sensitive to the self-affinity of the film. This approach, which we proved useful in the analysis of AFM data of conjugated molecular thin films grown in high vacuum, has never been applied to optical and electrical techniques on these systems and might be an interesting route to explore. We have started to assess the influence of different spatial correlations in thin films on the optical and the electro-optical properties, as it will be described in the next section. [Pg.100]

On his return to Princeton after the war, Hugh Taylor organized catalytic research at the Frick Chemical Laboratory. He applied high vacuum technique, liquid air cryoscopy to the study of adsorptive characteristics of catalysts, correlating rates of catalytic reactions and rates of adsorption. He introduced the concept of activated adsorption and defended it against all comers. ... [Pg.444]


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See also in sourсe #XX -- [ Pg.119 ]




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High vacuum

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