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X representation

The reduction of the x representation, like all such reductions, gives a unique set of irreducible representations which is... [Pg.95]

The X representation details an atom s number of electrons, number of protons, number of neutrons, charge and atomic mass number. [Pg.59]

What is the X representation What information about an atom can it detail ... [Pg.62]

Supposons pour terminer X representable. On a vu qu une section de au-dessus de X s identifie a un I -automorphisme de Xj. induisant... [Pg.58]

Using the semiclassical solution of Eq.(28) for the amplitudes in p -representation, we can obtain the diabatic wave functions in x -representation as... [Pg.110]

Let us focus on the subensemble of tube-pairs in which each tube is occupied by exactly one atom. In the ID optical lattice, the single-atom Hamiltonian in x representation is... [Pg.379]

Figure 10. Simulation of the EPR state preparation in an optical lattice with 25 sites, at three consecutive times. First row shows the joint probability distribution in x representation, the second one in p representation, (ol) and (a2) initially (t = 0), the atoms are cooled down to the external harmonic potential ground state, whereas the LIDDI is off. (61) and (62) at t = 1.4 x 10-4 s LIDDI and the repulsive linear potential (with the slope 0.04 Erec per lattice site) are on, whereas the harmonic potential is off. The diatoms are moving through the lattice very slowly in comparison to the single atoms, (cl) and (c2) at t = 2.16 x 10 4 s single atoms are ejected out of the lattice and discarded and the diatoms are separated out. Figure 10. Simulation of the EPR state preparation in an optical lattice with 25 sites, at three consecutive times. First row shows the joint probability distribution in x representation, the second one in p representation, (ol) and (a2) initially (t = 0), the atoms are cooled down to the external harmonic potential ground state, whereas the LIDDI is off. (61) and (62) at t = 1.4 x 10-4 s LIDDI and the repulsive linear potential (with the slope 0.04 Erec per lattice site) are on, whereas the harmonic potential is off. The diatoms are moving through the lattice very slowly in comparison to the single atoms, (cl) and (c2) at t = 2.16 x 10 4 s single atoms are ejected out of the lattice and discarded and the diatoms are separated out.
It is interesting to notice that the condition that the dynamical quantity f be represented by a diagonal matrix f in the x representation can be expressed as a differential equation. In order for V to be a diagonal matrix, must equal 0 for m not equal to n and a constant value, / - >, say, for m = n. This means that on expanding /oP.Xi> in terms of the complete set of functions X only the one term fn-n-Xn will occur that is, that... [Pg.424]

We shall limit ourselves here to the determination of the symmetry-adapted A" and E" orbitals in the Fj,x representation. Table 6.25 shows the action of all the symmetry operations of the D h point group on the generating functions pxi and (px2 — Pxs), as well as the characters of the A" and E" irreducible representations. [Pg.245]

The differential equation form of the logistic model of cell growth is basically a two-parameter (k and X ) representation of cell growth that is largely empirical in character. There have been numerous attempts to extend and interpret the model so as to identify parameters in other variations or extensions of the model. One approach commonly described in the literature begins by expressing the Monod equation (13.1.13) for the rate of substrate consumption as... [Pg.476]

It is well known that coexistence curves for binary mixtures are frequently more nearly symmetric in a T, representation than in a T, x representation." Simon, Fannin, and Knobler found, in analysing their vapour-pressure measurements on the system CH4 + CF4, that plots of A vs. [where their definition of takes the molar volumes in equation (28) as those of the pure... [Pg.253]

You may recall a strange omission in the character tables of Chapter 6 with one exception, the symbols of the irreducible representations may be written using a capital letter (for overall symmetry) or a lower case letter (for the symmetry of a single-coordinate function, such as an orbital wavefunction). The exception is that the X representations of the linear molecule point groups are always written using capital letters, because X symmetry is not possible Irom a one-coordinate function. For example, tr molecular orbitals are always symmetric upon reflection through any vertical mirror plane, whereas X electronic states (which are antisymmetric under (7y)... [Pg.346]

At the end of this chapter are the / plots that correspond to the types 1-VI isotherms given in Figs. 3-8. In addition a second type VI plot is presented that differs from the one presented in Fig. 8, which has the / plot feature 5. When transformed, types II and in are identical and so are types IV and V. Thus, the x representation cuts down on the number of isotherms to consider and specifies exactly the physical feature that each / plot feature corresponds to. One of the possible type VI isotherms that shows feature 5 in Table 3 above can be distinguished from the pore-filUng feature 3 in the X plot, whereas in the isotherm this discernment is not possible. [Pg.10]

This is basically the same equation as Eq. (100) with the quantity in the square brackets replacing the step function (and indeed becomes as [Pg.108]

The log-normal energy distribution has been expressed in Eq. (119), which yields the isotherm in the x representation as expressed in Eq. (120). The DP isotherms may all be expressed as... [Pg.123]

In addition to his own work [11,12] of Ar adsorption on sulfate salts, Bradley cited the work of McGavack and Patrick [13] of SO2 adsorption on Si02 and water adsorption on CuO by Bray and Draper [ 14]. Although these data are quite old, there is no reason to suspect that they are not accurate. Furthermore, they represent some rather unique isotherms which provide here a broader perspective. Figs. 71 and 72 show the isotherms of Ar on CUSO4 and Al2(S04)3 by Bradley in the x representation. [Pg.136]

Fig. 2. Schematic bifurcation diagrams in the amplitude (modulus i )/bifurcation parameter (/x) representation (a) amplitudes of the stationary solutions of hexagonal symmetry as given by Equation (26) (b) amplitudes of both the hexagonal and stripe solutions as given by Equation (27). Thick (broken) lines indicate stable (unstable) branch of solutions. Fig. 2. Schematic bifurcation diagrams in the amplitude (modulus i )/bifurcation parameter (/x) representation (a) amplitudes of the stationary solutions of hexagonal symmetry as given by Equation (26) (b) amplitudes of both the hexagonal and stripe solutions as given by Equation (27). Thick (broken) lines indicate stable (unstable) branch of solutions.
FIGURE 3.8 (a) Orthogonal hardness-electronegativity (// - x) representation for an electronic system with coordinate A (b) the ABB mechanism of frontier chemical... [Pg.265]


See other pages where X representation is mentioned: [Pg.87]    [Pg.52]    [Pg.470]    [Pg.145]    [Pg.244]    [Pg.59]    [Pg.117]    [Pg.34]    [Pg.34]    [Pg.418]    [Pg.574]    [Pg.81]    [Pg.279]    [Pg.433]    [Pg.627]    [Pg.56]    [Pg.145]    [Pg.34]    [Pg.123]   
See also in sourсe #XX -- [ Pg.59 ]




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Graphical Representation on the Y-X Diagram

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