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Level Diagrams

Fig. V-14. Energy level diagram and energy scales for an n-type semiconductor pho-toelectrochemical cell Eg, band gap E, electron affinity work function Vb, band bending Vh, Helmholtz layer potential drop 0ei. electrolyte work function U/b, flat-band potential. (See Section V-9 for discussion of some of these quantities. (From Ref. 181.)... Fig. V-14. Energy level diagram and energy scales for an n-type semiconductor pho-toelectrochemical cell Eg, band gap E, electron affinity work function Vb, band bending Vh, Helmholtz layer potential drop 0ei. electrolyte work function U/b, flat-band potential. (See Section V-9 for discussion of some of these quantities. (From Ref. 181.)...
Figure A3.13.1. Schematic energy level diagram and relationship between mtemiolecular (collisional or radiative) and intramolecular energy transfer between states of isolated molecules. The fat horizontal bars indicate diin energy shells of nearly degenerate states. Figure A3.13.1. Schematic energy level diagram and relationship between mtemiolecular (collisional or radiative) and intramolecular energy transfer between states of isolated molecules. The fat horizontal bars indicate diin energy shells of nearly degenerate states.
Figure Bl.12.1. (a) Energy level diagram for an/= nueleus showing the effeets of the Zeeman interaetion and first- and seeond-order quadnipolar effeet. The resulting speetra show statie powder speetra for (b) first-order perturbation for all transitions and (e) seeond-order broadening of the eentral transition, (d) The MAS speetnim for the eentral transition. ... Figure Bl.12.1. (a) Energy level diagram for an/= nueleus showing the effeets of the Zeeman interaetion and first- and seeond-order quadnipolar effeet. The resulting speetra show statie powder speetra for (b) first-order perturbation for all transitions and (e) seeond-order broadening of the eentral transition, (d) The MAS speetnim for the eentral transition. ...
Phenomenologically, the FNDOR experiment can be described as the creation of alternative relaxation paths for the electron spins, which are excited with microwaves. In the four-level diagram of the system... [Pg.1570]

With help of the four-level diagram of the =I= system (see figure BL15.8 two conniion ways for recording ELDOR spectra will be illnstrated. In freqnency-swept ELDOR the magnetic field is set at a value that satisfies the resonance condition for one of the two EPR transitions, e.g. 4<- 2, at the fixed observe klystron frequency, The pump klystron is then turned on and its frequency, is swept. When the pump... [Pg.1571]

Figure Bl.15.12. ESEEM spectroscopy. (A) Top energy level diagram and the corresponding stick spectrum for the two allowed (a) and two forbidden (f) transitions. Bottom time behaviour of the magnetization of an allowed (a) spin packet and a forbidden (f) spin packet during a two-pulse ESE sequence (see figure Bl.15.11 (A)). (B) The HYSCORE pulse sequence. Figure Bl.15.12. ESEEM spectroscopy. (A) Top energy level diagram and the corresponding stick spectrum for the two allowed (a) and two forbidden (f) transitions. Bottom time behaviour of the magnetization of an allowed (a) spin packet and a forbidden (f) spin packet during a two-pulse ESE sequence (see figure Bl.15.11 (A)). (B) The HYSCORE pulse sequence.
Figure Bl.15.13. Pulsed ENDOR spectroscopy. (A) Top energy level diagram of an. S-/=i spin system (see also figure Bl,15,8(A)). The size of the filled circles represents the relative population of the four levels at different times during the (3+1) Davies ENDOR sequence (bottom). (B) The Mims ENDOR sequence. Figure Bl.15.13. Pulsed ENDOR spectroscopy. (A) Top energy level diagram of an. S-/=i spin system (see also figure Bl,15,8(A)). The size of the filled circles represents the relative population of the four levels at different times during the (3+1) Davies ENDOR sequence (bottom). (B) The Mims ENDOR sequence.
Figure Bl.16.17. Level diagram showing tire origin of SCRP polarization. Figure Bl.16.17. Level diagram showing tire origin of SCRP polarization.
The most widely used of these tecluiiques is resonance-enlianced multiphoton ionization (REMPI) [ ]. A schematic energy-level diagram of the most conunonly employed variant (2 + 1) of this detection scheme is illustrated in the... [Pg.2082]

Figure C 1.4.8. (a) An energy level diagram showing the shift of Zeeman levels as the atom moves away from the z = 0 axis. The atom encounters a restoring force in either direction from counteriDropagating light beams, (b) A typical optical arrangement for implementation of a magneto-optical trap. Figure C 1.4.8. (a) An energy level diagram showing the shift of Zeeman levels as the atom moves away from the z = 0 axis. The atom encounters a restoring force in either direction from counteriDropagating light beams, (b) A typical optical arrangement for implementation of a magneto-optical trap.
Figure C2.15.4. (a) A tliree-level laser energy level diagram and (b) tlie mby system. Figure C2.15.4. (a) A tliree-level laser energy level diagram and (b) tlie mby system.
Its level diagram is shown in figure C2.15.6. Here a DC or RF discharge is used to excite the He ions, which in turn... [Pg.2860]

Figure C3.3.10. A schematic energy-level diagram for a molecule capable of undergoing unimolecular reaction above tlie energy depicted as tlie reaction barrier. Arrows to tlie right indicate reaction (collision-free) at a rate kg tliat depends on tlie energy E. Down arrows represent collisional redistribution of tlie hot molecules botli above and below tlie reaction barrier. Figure C3.3.10. A schematic energy-level diagram for a molecule capable of undergoing unimolecular reaction above tlie energy depicted as tlie reaction barrier. Arrows to tlie right indicate reaction (collision-free) at a rate kg tliat depends on tlie energy E. Down arrows represent collisional redistribution of tlie hot molecules botli above and below tlie reaction barrier.
I he Koothaan equations just described are strictly the equations fora closed-shell Restricted Hartrce-Fock fRHK) description only, as illustrated by the orbital energy level diagram shown earlier. To be more specific ... [Pg.226]

Draw an enthalpy level diagram showing how Kistiakowsky was able to... [Pg.168]

These absorptions are ascribed to n-n transitions, that is, transitions of an electron from the highest occupied n molecular orbital (HOMO) to the lowest unoccupied n molecular orbital (LUMO). One can decide which orbitals are the HOMO and LUMO by filling electrons into the molecular energy level diagram from the bottom up, two electrons to each molecular orbital. The number of electrons is the number of sp carbon atoms contributing to the n system of a neuhal polyalkene, two for each double bond. In ethylene, there is only one occupied MO and one unoccupied MO. The occupied orbital in ethylene is p below the energy level represented by ot, and the unoccupied orbital is p above it. The separation between the only possibilities for the HOMO and LUMO is 2.00p. [Pg.197]

Compute the eigenvalues and draw the energy level diagram for methylene-cyclopropene. [Pg.199]

Compute the IIMO eigenvalues for benzene and draw its energy level diagram. 16. Draw the energy level diagram for pyrrole. [Pg.199]

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]

Drawing an energy level diagram using these SALC-AOs would result in the following ... [Pg.228]

Show how you could adapt Frosts circle to generate the ] oribital energy level diagram shown in Figure 11 14 for cycloheptatrienyl cation j... [Pg.456]

Once you have calculated an ab initio or a semi-empirical wave function via a single point calculation, geometry optimization, molecular dynamics or vibrations, you can plot the electrostatic potential surrounding the molecule, the total electronic density, the spin density, one or more molecular orbitals /i, and the electron densities of individual orbitals You can examine orbital energies and select orbitals for plotting from an orbital energy level diagram. [Pg.124]

Simplified energy level diagram showing absorption of a photon. [Pg.372]

We can use the energy level diagram in Figure 10.14 to explain an absorbance spectrum. The thick lines labeled Eq and Ei represent the analyte s ground (lowest) electronic state and its first electronic excited state. Superimposed on each electronic energy level is a series of lines representing vibrational energy levels. [Pg.381]

Energy level diagram showing difference between the absorption of Infrared radiation (left) and ultravlolet-visible radiation (right). [Pg.381]

The atomic absorption spectrum for Na is shown in Figure 10.19 and is typical of that found for most atoms. The most obvious feature of this spectrum is that it consists of a few, discrete absorption lines corresponding to transitions between the ground state (the 3s atomic orbital) and the 3p and 4p atomic orbitals. Absorption from excited states, such as that from the 3p atomic orbital to the 4s or 3d atomic orbital, which are included in the energy level diagram in Figure 10.18, are too weak to detect. Since the... [Pg.383]

Energy level diagram for a molecule showing pathways for deactivation of an excited state vr Is vibrational relaxation Ic Is Internal conversion ec Is external conversion, and Isc Is Intersystem crossing. The lowest vibrational energy level for each electronic state Is Indicated by the thicker line. [Pg.425]


See other pages where Level Diagrams is mentioned: [Pg.158]    [Pg.1567]    [Pg.1598]    [Pg.1609]    [Pg.1611]    [Pg.2078]    [Pg.2084]    [Pg.2465]    [Pg.2858]    [Pg.2860]    [Pg.2881]    [Pg.2998]    [Pg.3010]    [Pg.124]    [Pg.147]    [Pg.458]    [Pg.383]    [Pg.427]    [Pg.434]   


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