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Energy level diagram model

Use SHMO to obtain the energy spectrum for the models methylenepentadiene. bicyclohexatriene, and styrene. IDraw all three energy level diagrams.. Are there degeneracies for these molecules ... [Pg.225]

Fig. 4. Energy level diagrams showing possible electronic configurations for positively-charged polaron (a) and bipolaron (b) defects and (c) a schematic bipolaron band model. The negatively-charged polaron would carry three electrons and the bipolaron four. Also shown is the neutral polaron-exciton (d) which would decay to restore the chain structure. Fig. 4. Energy level diagrams showing possible electronic configurations for positively-charged polaron (a) and bipolaron (b) defects and (c) a schematic bipolaron band model. The negatively-charged polaron would carry three electrons and the bipolaron four. Also shown is the neutral polaron-exciton (d) which would decay to restore the chain structure.
Fig. 8. Schematic total energy level diagram of the D(H,0) donors in Ge based on the tunneling hydrogen model (Reprinted with permission from the American Physical Society, Jobs, B., Haller, E.E., and Falicov, L.M. (1980). Phys. Rev. B 22, 832.)... Fig. 8. Schematic total energy level diagram of the D(H,0) donors in Ge based on the tunneling hydrogen model (Reprinted with permission from the American Physical Society, Jobs, B., Haller, E.E., and Falicov, L.M. (1980). Phys. Rev. B 22, 832.)...
The four-orbital model implies that the a- and Soret bands are caused by transitions from the two top filled 7r-orbitals (alu, a2u) to the lowest empty 7r -orbitals (eg) of the porphyrin jr-electron system. Fig. 3 shows these four molecular orbitals (49, 65) and Fig. 4 a schematic energy level diagram with the unperturbed porphyrin levels and the energy of the normal a-band on the left (66). If the metal possesses filled d-orbitals, d,-electron donation from the dxz and dyz (d -) orbitals to the empty eg-ir -orbitals of the porphyrin may occur, thus raising the eg-7r -orbitals and lowering the d -orbitals which have now become bonding (Fig. 4). The consequence is the hypsochromic shift of the a-band observed in the d8 metalloporphyrins (Fig. 2 and Table 3). [Pg.93]

Figure 2.5. Energy level diagram (top) and spectra (bottom) illustrating the two-state model of relaxation. The energy of the absorbed quantum is Av , and the energies of the emitted quanta are hvfl (unrelaxed) and hvF (relaxed). The fluorescence spectrum of the unrelaxed state (solid curve) is shifted relative to the absorption spectrum (dotted curve) due to the Stokes shift. The emission intensity from the unrelaxed state decreases and that from the relaxed state (dashed curve) increases as a result of relaxation. Figure 2.5. Energy level diagram (top) and spectra (bottom) illustrating the two-state model of relaxation. The energy of the absorbed quantum is Av , and the energies of the emitted quanta are hvfl (unrelaxed) and hvF (relaxed). The fluorescence spectrum of the unrelaxed state (solid curve) is shifted relative to the absorption spectrum (dotted curve) due to the Stokes shift. The emission intensity from the unrelaxed state decreases and that from the relaxed state (dashed curve) increases as a result of relaxation.
Figure 2.8. Energy level diagram (top) and spectra (bottom) illustrating the site-photoselection model of >... [Pg.92]

The authors discuss Schroeder s paradox, referred to elsewhere in this review, and the fact that liquid water uptake increases but saturated water uptake decreases with temperature. And, at low temperature, the water uptake by membranes in contact with saturated vapor is greater than that by membranes in contact with liquid water, which suggests a fundamental difference in membrane microstructure for the two situations. An energy level diagram of thermodynamic states versus temperature was proposed, based on this Flory—Huggins-based model. [Pg.322]

Figure 1 is an energy level diagram showing a proposed model for the band structure of zinc oxide. The valence band and conduction band are shown separated by a forbidden gap. Two levels which correspond to the trapping of two electrons by the interstitial zinc are indicated in the forbidden gap. Surface levels associated with adsorbed oxygen are shown. [Pg.271]

Energy Configuration Diagram. This model, based on the energy level diagrams of atoms and molecules, is applicable to luminescence processes in which excitation and emission take place at the same luminescence center. [Pg.237]

We can combine this spin concept and our orbital model to build atoms electron by electron. This is done by using what is called an energy-level diagram, shown in Figure 5.22. Each box represents an orbital, each electron is represented by an arrow, and two electrons spinning in opposite directions in the same orbital are shown as two arrows pointing in opposite directions. [Pg.161]

A1 is a nucleus with 13 protons and 13 neutrons. If we fill in the shell model energy level diagram from the bottom, we find the following configurations ... [Pg.149]

Au is a nucleus with 79 protons and 119 neutrons. Filling in the shell model energy level diagram we should find that the highest partially filled orbitals are... [Pg.150]

Figure 1.17 Energy-level diagram for the bonding model of ethylene. The ctch levels are not actually all at the same energy, but are lower than ircc. Figure 1.17 Energy-level diagram for the bonding model of ethylene. The ctch levels are not actually all at the same energy, but are lower than ircc.
Construct a complete orbital model for HN3, showing both a and tt molecular orbitals, and giving an approximate energy-level diagram showing electron occupancy. Compare the MO model with the resonance model. [Pg.41]

Describe the bonding in [Mn(CN)g]3-, using both crystal field theory and valence bond theory. Include the appropriate crystal field d orbital energy-level diagram and the valence bond orbital diagram. Which model allows you to predict the number of unpaired electrons How many do you expect ... [Pg.911]

Figure 1.3 Illustration of the two classes of two-electron processes caused by photoionization using magnesium as an example, using, on the left the model-picture of Fig. 1.1 and on the right an energy-level diagram (not to scale) (a) direct double photoionization in the outer 3s shell (b) 2p inner-shell photoionization with subsequent Auger decay where one 3s electron jumps down to fill the 2p hole and the other 3s electron is ejected into the continuum (Auger electron). The wavy line represents the incident photon (which is often omitted in such representations) electrons and holes are shown as filled and open circles, respectively arrows indicate the movements of electrons continuum electrons are classified according to their kinetic energy e. Figure 1.3 Illustration of the two classes of two-electron processes caused by photoionization using magnesium as an example, using, on the left the model-picture of Fig. 1.1 and on the right an energy-level diagram (not to scale) (a) direct double photoionization in the outer 3s shell (b) 2p inner-shell photoionization with subsequent Auger decay where one 3s electron jumps down to fill the 2p hole and the other 3s electron is ejected into the continuum (Auger electron). The wavy line represents the incident photon (which is often omitted in such representations) electrons and holes are shown as filled and open circles, respectively arrows indicate the movements of electrons continuum electrons are classified according to their kinetic energy e.
Fig. 1. Molecular orbital energy level diagram of the Me4M2( -CH)2 molecules, modeling the (Me,SiCH2)4M2(/j-CSiMe3)2 molecules, employing the method of Fenske and Hall, and showing the orbital population of the HOMO M—C and M—M n, 4b3u for M = Ta M—M a, 6ag for M = W and M—M S, 2a for M = Re. Fig. 1. Molecular orbital energy level diagram of the Me4M2( -CH)2 molecules, modeling the (Me,SiCH2)4M2(/j-CSiMe3)2 molecules, employing the method of Fenske and Hall, and showing the orbital population of the HOMO M—C and M—M n, 4b3u for M = Ta M—M a, 6ag for M = W and M—M S, 2a for M = Re.
Fig. 2. Simple one-dimensional model of quantum tunneling — a schematic illustration of the energy level diagram of two conductors, the sample and tip separated in vacuum by a distance, z with (a) no applied bias and (b) with an applied bias, V. Fig. 2. Simple one-dimensional model of quantum tunneling — a schematic illustration of the energy level diagram of two conductors, the sample and tip separated in vacuum by a distance, z with (a) no applied bias and (b) with an applied bias, V.
Atomic Systems. Many atomic species may be modeled as three-level systems. Figure 2 illustrates the energy level diagram for sodium. Other alkali and alkaline metals behave in a similar manner. [Pg.65]


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