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Local transformation

Fig. 6. Input transformation in (a) methods based on linear projection, (b) methods based on nonlinear projection, nonlocal transformation, (c) methods based on nonlinear projection, local transformation, and (d) partition-based methods. (From Bakshi and Utojo, 1998.)... Fig. 6. Input transformation in (a) methods based on linear projection, (b) methods based on nonlinear projection, nonlocal transformation, (c) methods based on nonlinear projection, local transformation, and (d) partition-based methods. (From Bakshi and Utojo, 1998.)...
A few examples of local transformations appear in Example II-4. The reader can verify for each pair of subschemes R and S, that if a scheme P is transformed by replacing subschema S by subscheme R in such a way that entry point lg of S is replaced by entry point 1 of R and exit point eg of S by exit point of R (or egg by egg and eg by if there are two corresponding exit... [Pg.41]

An alternative method of proof uses repeated applications of a local transformation, the duplicate operation, which also preserves graph homomorphic images. Call a direct connection in P from n to m anomalous if n m and n... [Pg.103]

It was demonstrated by Higgs [50] that the appearance of massless bosons can be avoided by combining the spontaneous breakdown of symmetry under a compact Lie group with local gauge symmetry. The potential V() which is invariant under the local transformation of the charged field... [Pg.172]

Cartesian coordinates is a product of N — 1 Jacobians for the local transformations from polar to Cartesian components for each bond vector Q for j < — 1, times the Jacobian det[A ]p = 1 for the transformation of Q... [Pg.80]

The GMH method of Cave and Newton [39, 40] is based on the assumption that the transition dipole moment between the diabatic donor and acceptor states vanishes, i.e., the off-diagonal element of the corresponding dipole moment matrix is zero. Thus, in the localization transformation one diagonalizes the dipole moment matrix of the adiabatic states ij/i and ij/z. For a two-state model, the rotation angle ft) can be expressed with the help of the transition dipole moment and the difference of the dipole mo-... [Pg.44]

Let G be a local transformation group that acts on M and is the symmetry group of system (5). Next, let the basis operators of the Lie algebra g of the group G be of the form... [Pg.275]

It was shown that the formation of the doubly oxidized 1,2-dihydroxypor-phyrin Zn TPPS — (OH)2 is not the last step of photochemical ring localized transformations. Prolonged photolysis causes the formation of the complex Zn TPPS — (OH)4). In all the above mentioned hydroxyporphyrins the axial positions are occupied by OH- and/or HzO ligands depending on the pH value of the irradiated solutions. [Pg.175]

Wiggins et al. [22] pointed out that one can always locally transform a Hamiltonian to the form of Eq. (1.38) if there exists a certain type of saddle point. Examination of the associated Hamilton s equations of motion shows that q = Pn = 0 is a fixed point that defines an invariant manifold of dimension 2n — 2. This manifold intersects with the energy surface, creating a (2m — 3)-dimensional invariant manifold. The latter invariant manifold of dimension 2m — 3 is an excellent example of an NHIM. More interesting, in this case the stable and unstable manifolds of the NHIM, denoted by W and W ,... [Pg.21]

This is also the Hamiltonian of the activated complex. We will encounter it in Eq. (23) with the customary symbol H. Regardless of its stability properties or the size of the nonlinearity, Eq. (12) is always an invariant manifold. However, we are interested in the case when it is of the saddle type with stable and unstable manifolds. If the physical Hamiltonian is of the form of Eq. (1), then a preliminary, local transformation is not required. The manifold (12) is invariant regardless of the size of the nonlinearity. Moreover, it is also of saddle type with respect to stability in the transverse directions. This can be seen by examining Eq. (1). On qn = Pn = 0 the transverse directions, (i.e., q and p ), are still of saddle type (more precisely, they grow and decay exponentially). [Pg.187]

En particulier, un foncteur de nature locale transforme sommes directes en pro-duits. Comme tout foncteur representable est un faisceau, cette topologie est moins fine que la topologie canonique. ... [Pg.239]

The present work treats the adsorption of CH, CH and H on a Ni(lll) surface in the context of a many-electron theory that permits the accurate computation of molecule-solid surface interactions at an initio configuration interaction level. The adsorbate and local surface region are treated as embedded in the remainder of the lattice electronic distribution which is modelled as a 26-atom, three layer cluster, extracted from a 62-atom cluster by an orbital localization transformation. [Pg.141]

Localized transformation processes such as those observed in scarred liver (s. p. 405) are not considered to be cirrhosis. The loss of parenchyma in scarred liver is generally the result of reduced blood supply in the respective area. Deep-set scars create the picture of a funnel-shaped liver (s. p. 406). Similarly, pronounced liver fibrosis (s. p. 405) does not fulfil the criteria of cirrhosis, since the lobular architecture as well as the intrahepatic and intra-acinar vascular supply are uncompromised. While fibrosis constitutes a precirrhotic stage, it does not necessarily progress to cirrhosis itself Fibrosis can regress Thus, liver cirrhosis is characterized by the following five criteria ... [Pg.716]

Finding a localization transformation is usually done by satisfying a given optimum criterion. Some well-known optimum criteria can be summarized as searching for the maximum or minimum value of the functional... [Pg.46]


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See also in sourсe #XX -- [ Pg.164 , Pg.165 , Pg.167 ]




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Density functional theory local-scaling transformation

Hartree-Fock level in the context of local-scaling transformations

Independent local-scaling transformations

Kohn-Sham orbitals and potentials for beryllium by means of local scaling transformations

Local Approximations to the Exact-Decoupling Transformation

Local gauge transformation

Local phase transformation

Local scaling transformation

Local-scaling transformation of the

Local-scaling transformations, for

Localized orbital transformation

Orbital local-scaling transformation

SOME LOCAL EQUIVALENCE PRESERVING TRANSFORMATIONS

Transformation Between Local and Normal Mode Limits

Transformation between 4-Parameter Forms of the Normal and Local Mode Basis Sets

Transformation localizing

Transformation localizing

Transformation normal<->local mode

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