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Antibonding state

Chemical reactions of aimnonia with the silicon surface have also been clearly observed using STS [21], where the disappearance of the it and it states characteristic of the clean surface coincides with the fomiation of Si-H antibonding states corresponding to the dissociation of the ammonia on the Si surface. [Pg.1681]

A theoretical interpretation relating the valence electron concentration and the structure was put forward by H. Jones. If we start from copper and add more and more zinc, the valence electron concentration increases. The added electrons have to occupy higher energy levels, i.e. the energy of the Fermi limit is raised and comes closer to the limits of the first Brillouin zone. This is approached at about VEC = 1.36. Higher values of the VEC require the occupation of antibonding states now the body-centered cubic lattice becomes more favorable as it allows a higher VEC within the first Brillouin zone, up to approximately VEC = 1.48. [Pg.162]

Fig. 19 Mn K-edge XANES spectra for a Mn0.95V0.05P and b Co0.10Mn0.90P, normalized relative to MnP. Assignments for peaks are (A) Mn Is —> 3d and Is — 4p (B) Mn Is —> P 3p antibonding states (C) Mn Is — 4p. Reprinted with permission from [60]. Copyright Elsevier... Fig. 19 Mn K-edge XANES spectra for a Mn0.95V0.05P and b Co0.10Mn0.90P, normalized relative to MnP. Assignments for peaks are (A) Mn Is —> 3d and Is — 4p (B) Mn Is —> P 3p antibonding states (C) Mn Is — 4p. Reprinted with permission from [60]. Copyright Elsevier...
The two bonding 7r orbitals represented by these wave functions are degenerate. The wave functions for the antibonding states are identical in form except that negative signs are used in the combination of atomic wave functions and in the normalization constants. [Pg.77]

The adsorptions of H, O, and S04 on Pt/C electrocatalyst electrodes have been further investigated by O Grady and Ramaker by comparing the XANES data at the Pt L2 and L3 absorption edges. In their analysis, the difference spectrum, which they term AS for antibonding state, is obtained as follows ... [Pg.386]

Fig. 31. Schematic potential energy diagram for interaction between absorbate A and a surface M. G is the ground state of the molecular complex, M" + A is an ionic state, (M + A) is an antibonding state, M + A is a state where the adsorbate is excited and the substrate is in its ground state, M + A is a state where the substrate is excited and the adsorbate is in its ground state. Possible electronic transitions from the ground state G to the various excited states are indicated by the shaded Franck-Condon region. Electron bombardment can presumably excite any of these states. (From Ref. )... Fig. 31. Schematic potential energy diagram for interaction between absorbate A and a surface M. G is the ground state of the molecular complex, M" + A is an ionic state, (M + A) is an antibonding state, M + A is a state where the adsorbate is excited and the substrate is in its ground state, M + A is a state where the substrate is excited and the adsorbate is in its ground state. Possible electronic transitions from the ground state G to the various excited states are indicated by the shaded Franck-Condon region. Electron bombardment can presumably excite any of these states. (From Ref. )...
The claim of direct observation is used occasionally as the ultimate panacea and to support claims of validity and authenticity. Direct observation means nothing more than that some property of an intermediate is measured during its lifetime, that is, the lifetime of the species exceeds the characteristic time scale of the method of observation. The simplest direct observable is absorption or emission of light, transitions to non- or antibonding states and radiative return to the ground state, which have little or no structural information. Problems inherent in relying on direct observation are evident in medieval accounts of unicorns or mermaids or... [Pg.213]

Fig. 3.2 The bonding and antibonding states for (a) the homonuclear and (b) the heteronuclear diatomic molecule. The shift in the energy levels due to overlap repulsion has not been shown. Fig. 3.2 The bonding and antibonding states for (a) the homonuclear and (b) the heteronuclear diatomic molecule. The shift in the energy levels due to overlap repulsion has not been shown.
Therefore, as illustrated by the left-hand panels of Fig. 3.2, s-valent diatomic molecules are characterized by bonding and antibonding states that are separated in energy by the amount wAB, such that... [Pg.54]

Thus, we recover the expected result that the free atomic s and p levels split independently of each other into bonding and antibonding states, with energies Es + ssother hand, we have... [Pg.70]

This behaviour is illustrated schematically by the left-hand panel of Fig. 3.13. We see that for large intemuclear separations the a states go over to bonding and antibonding states around the free atomic energy levels Es... [Pg.70]

Note that because of the symmetry of the % orbitals, which are displayed in Fig. 3.10(b), the bonding state is odd under inversion about the molecular centre, the antibonding state even. Hence, they are labelled and 7ig respectively. [Pg.71]


See other pages where Antibonding state is mentioned: [Pg.344]    [Pg.220]    [Pg.232]    [Pg.241]    [Pg.46]    [Pg.92]    [Pg.95]    [Pg.102]    [Pg.270]    [Pg.71]    [Pg.376]    [Pg.102]    [Pg.616]    [Pg.14]    [Pg.27]    [Pg.199]    [Pg.160]    [Pg.189]    [Pg.46]    [Pg.387]    [Pg.1]    [Pg.12]    [Pg.13]    [Pg.175]    [Pg.186]    [Pg.188]    [Pg.344]    [Pg.290]    [Pg.315]    [Pg.55]    [Pg.57]    [Pg.66]    [Pg.70]    [Pg.72]   
See also in sourсe #XX -- [ Pg.12 ]

See also in sourсe #XX -- [ Pg.12 ]

See also in sourсe #XX -- [ Pg.130 ]

See also in sourсe #XX -- [ Pg.46 , Pg.64 , Pg.68 , Pg.69 , Pg.70 , Pg.91 ]




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