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L State

Urif e[Pg.62]

Even at the equilibrium geometry, it is necessary to treat both of the l+ states in order to get a reasonable description of the electronic wavefunction for the ground state. [Pg.188]

Because the energy of any M state is less than that of any L state, it follows that K/3 will have a shorter wavelength than Ka. In this... [Pg.30]

Fig. 1-17 (Continued). All lines with intensity greater than 1% of the strongest line in the spectral series are shown for the K and L states. As the line is emitted, the electron moves up the arrow the state of the atom moves down. Fig. 1-17 (Continued). All lines with intensity greater than 1% of the strongest line in the spectral series are shown for the K and L states. As the line is emitted, the electron moves up the arrow the state of the atom moves down.
Figure 4. Energy diagram for 532 nm excitation of PuF g). The 5f electron states of PuF are shown at the left. The solid arrows indicate photon absorption or emission processes. The wavy arrows indicate nonradiative processes by which excited states of PuFg may be lost. The laser-fluence dependent fluorescence decay found at this excitation wavelength can be explained in terms of a bimolecular reaction between PuFg(g) in its 4550 cm l state and PuF (g) to form PuFj(g). It is assumed that PuF (g) is formed via dissociation of the initially populated PuF state. Figure 4. Energy diagram for 532 nm excitation of PuF g). The 5f electron states of PuF are shown at the left. The solid arrows indicate photon absorption or emission processes. The wavy arrows indicate nonradiative processes by which excited states of PuFg may be lost. The laser-fluence dependent fluorescence decay found at this excitation wavelength can be explained in terms of a bimolecular reaction between PuFg(g) in its 4550 cm l state and PuF (g) to form PuFj(g). It is assumed that PuF (g) is formed via dissociation of the initially populated PuF state.
Webster, R. L., State College of Washington, Circ. 64 (December 1948). [Pg.55]

In a shooting move a trial path is generated from an old path as follows. First, one of the L states of the old path z(° 8) is selected at random with a uniform probability, i.e., all states on the path have the same probability to be selected.3 The selected state consists of the positions qsmall perturbation (ip to the old momenta... [Pg.258]

Schultz, D. G., and Melsa, J. L., State Functions and Linear Control Systems, McGraw-Hill, New York, 1967. [Pg.264]

For Pa = 0 (rf = 0), the adatom is detached from the surface atom (Fig. 1.1), and 9k is given by the zeros of the two terms in brackets on the left-hand side of (1.26). The first (second) term represents the single N) state(s) contributed by the adatom (substrate) for a total of (N + l) states. The graphical solution of the [term] is displayed in Fig. 1.2 for several values of zs (Goodwin 1939b, Davison and St slicka 1996). Asymptotes occur at... [Pg.7]

The selective and fast catalyst species we want is HM(L) and we have determined that at a certain pressure we need a twenty-fold excess of L in order to have 95 % o/M in the M(L) state. [Pg.163]

Figure 7.9 Light-dependent binding of CO to Ni at the level of the Ni -C state. After mixing of H2-reduced enzyme with CO-saturated buffer in the dark, the Nij-C state is formed within 10 ms. Carbon monoxide does not bind to Ni due to its high valence state. When illuminated at 30 K the Ni -L state is formed, where the charge density at the Ni-Fe site has greatly increased (see also the shift of the FTIR bands in Fig. 7.6). Upon raising the temperature to 200 K in the dark, the nearby CO now can bind to the electron-rich Ni.The Ni. CO species has been earlier characterized by our group. Figure 7.9 Light-dependent binding of CO to Ni at the level of the Ni -C state. After mixing of H2-reduced enzyme with CO-saturated buffer in the dark, the Nij-C state is formed within 10 ms. Carbon monoxide does not bind to Ni due to its high valence state. When illuminated at 30 K the Ni -L state is formed, where the charge density at the Ni-Fe site has greatly increased (see also the shift of the FTIR bands in Fig. 7.6). Upon raising the temperature to 200 K in the dark, the nearby CO now can bind to the electron-rich Ni.The Ni. CO species has been earlier characterized by our group.
CN and CO ligands keeps the Fe in a low-spin state (S = 0) and prevents the detection of hyperfine splitting of Fe in EPR and Fe-ENDOR (Huyett et al. 1997). Also, very good agreement with experimental data was obtained for model clusters of the Ni-A, Ni-C and Ni-L states. [Pg.176]

Figure 3.3. Reactions of CO with hydrogen-reduced A. vinosum hydrogenase (Ffappe et al. 1999). Starting with enzyme plus 0.8mM hydrogen (equivalent to 1 bar Nia-SR state), a transient Nia-C state was detected within 10ms when the solution was mixed with CO-saturated buffer (in the dark). Thereafter, a rapid decline of the Nia-C state was noticed (conversion into Nia-S-CO). The sample obtained at 10 ms could be converted to the Nia-L state by illumination at 30K. Raising the temperature to 200K did not reverse process instead a state was detected in which CO was directly bound to nickel (Nia -CO). Protons are not shown. Figure 3.3. Reactions of CO with hydrogen-reduced A. vinosum hydrogenase (Ffappe et al. 1999). Starting with enzyme plus 0.8mM hydrogen (equivalent to 1 bar Nia-SR state), a transient Nia-C state was detected within 10ms when the solution was mixed with CO-saturated buffer (in the dark). Thereafter, a rapid decline of the Nia-C state was noticed (conversion into Nia-S-CO). The sample obtained at 10 ms could be converted to the Nia-L state by illumination at 30K. Raising the temperature to 200K did not reverse process instead a state was detected in which CO was directly bound to nickel (Nia -CO). Protons are not shown.
Note that the probability of finding state L changes with A, according to Eq. (3.2.14), which is also the mole fraction of the L state as a function of A. We shall denote this function by X (A), which changes from [i.e., (A = 0)], when A = 0 to for the fully occupied system at A Thus,... [Pg.55]

Alaska Aquatic life criterion for total hydrocarbons in marine and surface waters 15-g/L State of Alaska 1989... [Pg.161]

Florida Average or maximum allowable quantity of oil or grease discharged Class V waters (navigation, industrial use) 10 mg/L State of Florida 1992... [Pg.161]

Nebraska Maximum petroleum oil concentration in surface waters 10 mg/L State of Nebraska 1991... [Pg.161]

Energies and Other Properties of Heavy Atoms and Molecules Tables Spectroscopic parameters ofCdH X L state ... [Pg.171]

Copper forms practically aU its stable compounds in -i-l and +2 valence states. The metal oxidizes readily to -i-l state in the presence of various com-plexing or precipitating reactants. However, in aqueous solutions +2 state is more stable than -i-l. Only in the presence of ammonia, cyanide ion, chloride ion, or some other complexing group in aqueous solution, is the +1 valence state (cuprous form) more stable then the +2 (cupric form). Water-soluble copper compounds are, therefore, mostly cupric unless complexing ions or molecules are present in the system. The conversion of cuprous to cupric state and metalhc copper in aqueous media (ionic reaction, 2Cu+ — Cu° -i- Cu2+) has a Kvalue of 1.2x106 at 25°C. [Pg.255]

There are 75 standard tableaux functions in a full valence treatment, but only 36 are H states, half being x-components and half y-components. The variation problem therefore has two 18 x 18 matrices. The principal standard tableaux functions in the wave function are shown in Table 13.2. The predominant term in the wave function clearly involves the C atom in its / (l) state. The calculated dipole... [Pg.178]


See other pages where L State is mentioned: [Pg.533]    [Pg.89]    [Pg.90]    [Pg.25]    [Pg.30]    [Pg.31]    [Pg.31]    [Pg.31]    [Pg.348]    [Pg.172]    [Pg.443]    [Pg.798]    [Pg.588]    [Pg.54]    [Pg.130]    [Pg.87]    [Pg.135]    [Pg.141]    [Pg.159]    [Pg.25]    [Pg.26]    [Pg.101]    [Pg.97]    [Pg.250]    [Pg.99]    [Pg.200]    [Pg.138]    [Pg.141]    [Pg.436]   
See also in sourсe #XX -- [ Pg.611 ]




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