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Probability electronic

An actual molecule is d Tiamic, not static. Electrons move continuously and can be thought of as being spread over the entire molecule. In a covalent bond, nevertheless, the distribution of electrons has the general characteristics shown by the static view in the figure. The most probable electron locations are between the nuclei, where they are best viewed as being shared between the bonded atoms. [Pg.573]

An electron-gain centre of similar geometry and electronic structure is generated (43) by radiolysis of the nitrosocarbonyl Mn(C0)4N0. Spectra associated with the electron-loss centres Mn(C0)nX+ (n=4 or 5) are less well-defined and pose analytical difficulties (41). However, there is little doubt that these are high-spin radicals, probably electronic sextets. [Pg.184]

To describe the d-orbital splitting effect for the octahedral field, one should imagine ligand spheres of electron density approaching along the x, y, and z axes, where the dxi yi and di lobes of electron density point. Figure 1.5 illustrates representations of high-probability electron orbit surfaces for the five d orbitals. [Pg.13]

Radiative transitions may be considered as vertical transitions and may therefore be explained in terms of the Franck-Condon principle. The intensity of any vibrational fine structure associated with such transitions will, therefore, be related to the overlap between the square of the wavefunctions of the vibronic levels of the excited state and ground state. This overlap is maximised for the most probable electronic transition (the most intense band in the fluorescence spectrum). Figure... [Pg.60]

Figure 4.1 Most probable electronic transitions involved in radiative transitions where (a) both electronic states have similar geometries (b) the excited state and ground state have very different geometries... Figure 4.1 Most probable electronic transitions involved in radiative transitions where (a) both electronic states have similar geometries (b) the excited state and ground state have very different geometries...
Fig. 2-36. Electron energy levels in hydrated oxidant Fe and reduc-tantFe AG = energy to organize hydrate structures dGj t = energy required for dehydrated redox ions to donate or accept gaseous electrons ep.2> o = most probable electron donor level of Fe Spe +.A = most probable electron acceptor level of Fe Hj05,2.,p,j = hydrated structures cgn) = standard gaseous electron level (s 0). Fig. 2-36. Electron energy levels in hydrated oxidant Fe and reduc-tantFe AG = energy to organize hydrate structures dGj t = energy required for dehydrated redox ions to donate or accept gaseous electrons ep.2> o = most probable electron donor level of Fe Spe +.A = most probable electron acceptor level of Fe Hj05,2.,p,j = hydrated structures cgn) = standard gaseous electron level (s 0).
The frontier electron level of adsorbed particles splits itself into an occupied level (donor level) in a reduced state (reductant, RED) and a vacant level (acceptor level) in an oxidized state (oxidant, OX), because the reduced and oxidized particles differ from each other both in their respective adsorption energies on the interface of metal electrodes and in their respective interaction energies with molecules of adsorbed water. The most probable electron levels, gred and eqx, of the adsorbed reductant and oxidant particles are separated from each other by a magnitude equivalent to the reorganization energy 2 >. ki in the same way as occurs with hydrated redox particles described in Sec. 2.10. [Pg.165]

As is shown in Eqns. 2-48 and 2-49, the probability density W(e) of electron energy states in the reductant or oxidant particles is represented as a normal distribution function (Gaussian distribution) centered at the most probable electron level (See Fig. 2-39.) as expressed in Eqns. 8-10 and 8-11 ... [Pg.238]

Fig. 8-29. Energy diagram for the most probable electron level, eck, of oxidant particles and the conduction band edge level, Bq, in a cathodic redox electron transfer via the conduction band cathodic current is maximum when cqx equals e. ... Fig. 8-29. Energy diagram for the most probable electron level, eck, of oxidant particles and the conduction band edge level, Bq, in a cathodic redox electron transfer via the conduction band cathodic current is maximum when cqx equals e. ...
Complexation therefore raises the standard Fermi level of redox electrons ep(KEDcs)> provided that the affinity of ligand coordination is greater with the oxidant particle than with the reductant particle (- dGox > - dG c) whereas, the complexation lowers the standard Fermi level of redox electrons Ef(redox)> provided that the affinity of ligand coordination is smaller with the oxidant particle than with the reductant particle (- dGox < - dG o)- With a shift of the standard Fermi level of redox electrons due to complexation, the most probable electron levels esED and cox of the redox particles are also shifted in the same direction. [Pg.275]

As shown in Fig. 8-34, when the most probable electron level of the reductant particle is higher in the ligand-coordinated state cred(chydrated state ereix i). ibe transfer of anodic electrons occurs at higher energy levels (at less anodic potentials) with the ligand-coordinated reductant particle than with the simply hydrated reductant particle. In such a case the complexation of redox particles will accelerate the anodic transfer of redox electrons. [Pg.277]

Pereira et al. (1998) provided biochemical evidence that electron transfer from either iron-only or NiFe-hydrogenases to HmcA is possible, although at a slow rate. The increase in electron-transfer rate by addition of cytochrome C3 indicates that a more probable electron-transport path is from hydrogen through hydrogenase and cytochrome C3 to HmcA. [Pg.103]

The most probable electron transfer term of the excited dye as an acceptor is shifted by Z-reorg into positive directions as explained later (p. 41). With an estimated... [Pg.38]

Photopolymerization of acrylamide by the uranyl ion is said to be induced by electron transfer or energy transfer of the excited uranyl ion with the monomer (37, 38). Uranyl nitrate can photosensitize the polymerization of /S-propiolactone (39) which is polymerized by cationic or anionic mechanism but not by radical. The initiation mechanism is probably electron transfer from /S-propiolactone to the uranyl ion, producing a cation radical which propagates as a cation. Complex formation of uranyl nitrate with the monomer was confirmed by electronic spectroscopy. Polymerization of /J-propiolactone is also photosensitized by sodium chloroaurate (30). Similar to photosensitization by uranyl nitrate, an election transfer process leading to cationic propagation has been suggested. [Pg.338]

BERKELIUM. [CAS 7440-40-6]. Chemical element, symbol Bk, at. no. 97, at wt. 247 (mass number of the most stable isotope), radioactive metal of the Actinide series, also one of the Transuranium elements. All isotopes of berkelium are radioactive all must be produced synthetically. The element was discovered by G.T. Seaborg and associates at the Metallurgical Laboratory of the University of Chicago in 1949. At that time, the dement was produced by bombarding 241 Am with helium ions. 4i Bk is an alpha-emitter and may be obtained by alpha-bombardment of ,4Cm. 245Cm. or 246Ciu. Ollier nuclides include those of mass numbers 243—246 and 248-250. Probable electronic configuration ... [Pg.194]

EINSTENIUM. CAS 7429-92-71. Chemical element symbol Es, at. no. 99. at. wt. 254 (mass number of the most stable isotope), radioactive metal of the Actinide series, also one of the Transuranium elements. Both einsteinium and fermium were formed tit a thermonuclear explosion that occurred in the South Pacific in 1952. The elements were identified by scientists from the University of California s Radiation Laboratory- the Argonnc National Laboratory, and the I. os Alamos Scientific Laboratory. It was observed that very heavy uranium isotopes which resulted from the action of the instantaneous neutron dux on uranium (contained in the explosive device) decayed to form Es and Fm. The probable electronic configuration of Es is... [Pg.538]

The most probable electron configurations for iron atoms in a ligand field formed by amino-acid side chains and sulfur are d5 and d6. The crystal field splitting [A) required to pair spins in iron compounds is... [Pg.27]

Fig. 5.5 Temperature dependencies for Ps formation probability, electron solvation time and positron lifetime in n-propanol. With changing temperature from 150 K to 300 K the electron solvation time in n-propanol varies within 5 orders of magnitude. At the highest studied temperature r approaches 10 ps. At low temperatures it exceeds e+ lifetime T2 more than 1000 times. If e had really contributed to Ps formation, Ps yield would have to decrease. However, it even slightly increases. This fact favors the presolvated electron as the main precursor of Ps formation. Fig. 5.5 Temperature dependencies for Ps formation probability, electron solvation time and positron lifetime in n-propanol. With changing temperature from 150 K to 300 K the electron solvation time in n-propanol varies within 5 orders of magnitude. At the highest studied temperature r approaches 10 ps. At low temperatures it exceeds e+ lifetime T2 more than 1000 times. If e had really contributed to Ps formation, Ps yield would have to decrease. However, it even slightly increases. This fact favors the presolvated electron as the main precursor of Ps formation.
Figure 47. Idealized energy levels and most probable electronic absorptions, ffabs, of one monomeric and two dimeric dye structures. The arrows represent the directions of the localized transition dipole moments. The transition in the face-to-face aggregate is representative of that in an H-aggregate and the transition in the end-to-end structure is representative of that in a J-aggregate. Figure 47. Idealized energy levels and most probable electronic absorptions, ffabs, of one monomeric and two dimeric dye structures. The arrows represent the directions of the localized transition dipole moments. The transition in the face-to-face aggregate is representative of that in an H-aggregate and the transition in the end-to-end structure is representative of that in a J-aggregate.
Methyl cobalamin is usually described as a Co(II) compound, which changes to Co(III) on dissociation of CH3. Describe the probable electronic structure (splitting of d levels and number of unpaired electrons) of the cobalt in both cases. [Pg.636]

In contrast to thermolysis, photolysis leads to an electronically excited state in which the a-nitrogen atom is probably electron-deficient. Clossen and Gray have described the electronic transition normally involved in photolysis (287 nm) as a -> transition [346-> 347] (equation 153). This would leave the py orbital on the... [Pg.305]


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See also in sourсe #XX -- [ Pg.164 ]




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Atomic orbitals electron probability curves

Circular distribution electron probability

Electron correlation excitation probabilities

Electron escape probability

Electron excitation probability

Electron excitation probability approximation

Electron excitation probability atomic orbitals approximation

Electron excitation probability states

Electron probability density function

Electron probability density maps

Electron probability density maxima

Electron probability distribution

Electron probable location

Electron tunneling transmission probability

Electronic excitation probability

Electronic population probability

Electronic transitions, forbidden radiation probability

Electronic wavefunction and probability density function

Electrons probability cloud

Electrons probability maps

Electrons, crystalline solid materials probability, energy

Hydrogen atom electron probability

Hydrogen atom electron probability density

Lewis electron pair model electrons probabilities

Lewis electron pair model probability

Most probable electron level

Probabilities of Electronically Adiabatic Processes

Probabilities of Electronically Non-Adiabatic Processes

Probability density, electronic

Probability density, of electron

Probability distribution, of electrons

Probability electron

Probability electron

Probability electron density

Probability electronic thermodynamic

Probability of electron transfer

Probability of electronic transition

Probability of electronically

Probability of finding an electron

Probability, of finding electrons

The Probability of Electron Tunneling

Transition probabilities electronic

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