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Representation of state

We must relate the representation of state in the system specification to the representation in this architecture. We can do this in two steps. First, we split the system into stores (see Figure 16.16). Then we map from the refined design to the spec. We are given the following ... [Pg.700]

Fig. 6. Representation of states for a hypothetical protein composed of two cooperative folding units. Free energy differences designated in uppercase letters represent the intrinsic stabilities of the cooperative units and have a contribution to the statistical weights designated by k. Free energy differences designated in lowercase letters represent the interaction between cooperative units and have a contribution to the statistical weights designated by . [Reprinted from Freire and Murphy (1991).]... Fig. 6. Representation of states for a hypothetical protein composed of two cooperative folding units. Free energy differences designated in uppercase letters represent the intrinsic stabilities of the cooperative units and have a contribution to the statistical weights designated by k. Free energy differences designated in lowercase letters represent the interaction between cooperative units and have a contribution to the statistical weights designated by <t>. [Reprinted from Freire and Murphy (1991).]...
Figure 4.20. The two-electron two-orbital model a) for a homosymmetric biradicaloid and b) for a heterosymmetric biradicaloid schematic representation of state energies, relative to the T state, as a function of the interaction integral y or as a function of the electronegativity difference 6 of the orbitals x and Xt (by permission from Michl and Bona i(5-Koutecky. 1990). Figure 4.20. The two-electron two-orbital model a) for a homosymmetric biradicaloid and b) for a heterosymmetric biradicaloid schematic representation of state energies, relative to the T state, as a function of the interaction integral y or as a function of the electronegativity difference 6 of the orbitals x and Xt (by permission from Michl and Bona i(5-Koutecky. 1990).
To understand dynamics in multidimensional Hamiltonian systems, adequate representation of states is important. [Pg.442]

Representation of State. By virtue of its features, the density operator 0 is the index of the measurement statistics of quantum physics. It will be seen from Postulate 4 below that p is also the seat of causality for certain types of changes of state. In addition, it will be shown that, for an ensemble of identically prepared replicas of a system, 0 is irreducible i.e., the ensemble cannot be subdivided into subensembles each of which would yield upon measurement statistics different from the statistics of 0. Alternatively, for an ensemble of identically prepared replicas of a system, p corresponds to irreducible uncertainties of measurement results. [Pg.265]

For carbon atoms, however, the ab initio configuration interaction calculations of Blint and Newton on the reactions of S, D, and P electronic states with molecular hydrogen have made an important contribution (73). A schematic representation of states and pathways is given in Figure 4. The calculations indicate that carbon will not react with H2, a result also obtained by Husain from a symmetry-derived correlation diagram (74). Therefore, the reactions of only the two lowest states of atomic carbon, and P, were considered. The formation of methyne CH from the state and insertion by P recoiling carbon atoms was indicated. [Pg.20]

State traversal techniques like finite state machine (FSM) equivalence checking (O. Coudert, C. Berthet J.C. Madre 1990) and temporal logic model checking (J.R. Burch, E.M. Clarke, K.L. McMillan, D.L. Dill L.J. Hwang 1990) have established themselves as the predominant techniques for hardware verification. This is due to the fact that diey allow the fully-automated verification of systems. These can be of considerable size due to symbolic traversal techniques, based on the symbolic representation of state sets by characteristic functions and the transition system by a transition relation. Both may be represented efficiently using ROBDDs (R.E. Bryant 1986). Moreover, mostly CTL as an efficiently checkable temporal logic is used (E.M. Clarke, E.A. Emerson A.P. Sistla 1986). [Pg.146]

We introduced the logic CCTL which allow a comfortable description of time properties. By using extended characteristic functions we presented die representation of state sets with associated clock values and the transition relation with interval edges. Based on these data structures we developed the new model checking algorithm. [Pg.162]

Figure 4.19 shows a schematic representation of state-of-the-art expression apparatus. The more conventional piston press apparatus described in Section 4.5.1 is augmented with the addition of a computer driven pressure regulator which allows the pressure applied to the piston to be carefully controlled and varied according to a preset pattern (e.g. ramp, sinusoidal etc.). The interfaced rotary or linear encoder, force transducer and electronic balance allow semi-continuous measurements of piston displacement, transmitted pressure and... [Pg.195]

Defense is a literal manifestation of power. Defensive works are strong representations of state power. The earliest list of wonders included the walls of Babylon, an expression of Babylonian military authority. [Pg.19]

Having considered the representation of states and operators in second quantization, let us now turn our attention to expectation values. As in first quantization, the evaluation of expectation values is carried out by means of density matrices [4]. Consider a general one- and two-electron Hermitian operator in the spin-orbital basis... [Pg.19]


See other pages where Representation of state is mentioned: [Pg.220]    [Pg.25]    [Pg.329]    [Pg.183]    [Pg.30]    [Pg.358]    [Pg.86]    [Pg.329]    [Pg.287]    [Pg.28]    [Pg.291]    [Pg.145]   
See also in sourсe #XX -- [ Pg.265 ]




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