Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Crystal field theory
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
==Stabilization energy== The crystal field stabilization energy (CFSE) is the stability that results from placing a transition metal ion in the crystal field generated by a set of ligands. It arises due to the fact that when the [[Atomic orbital|''d''-orbitals]] are split in a ligand field (as described above), some of them become lower in energy than before with respect to a spherical field known as the barycenter in which all five ''d''-orbitals are degenerate. For example, in an octahedral case, the ''t<sub>2g</sub>'' set becomes lower in energy than the orbitals in the barycenter. As a result of this, if there are any electrons occupying these orbitals, the metal ion is more stable in the ligand field relative to the barycenter by an amount known as the CFSE. Conversely, the ''e<sub>g</sub>'' orbitals (in the octahedral case) are higher in energy than in the barycenter, so putting electrons in these reduces the amount of CFSE. [[File:Octahedral cfse.svg|thumb|right|500px|Octahedral crystal field stabilization energy. Degenerate atomic ''d''-orbitals of a free metal ion (left), destabilization of ''d''-orbitals within a spherical negative electric field (center), and loss of degeneracy relative to the spherical field when ligands are treated as point charges in an octahedral geometry.]] If the splitting of the ''d''-orbitals in an octahedral field is Δ<sub>oct</sub>, the three ''t<sub>2g</sub>'' orbitals are stabilized relative to the barycenter by <sup>2</sup>/<sub>5</sub> Δ<sub>oct</sub>, and the ''e<sub>g</sub>'' orbitals are destabilized by <sup>3</sup>/<sub>5</sub> Δ<sub>oct</sub>. As examples, consider the two ''d''<sup>5</sup> configurations shown further up the page. The low-spin (top) example has five electrons in the ''t<sub>2g</sub>'' orbitals, so the total CFSE is 5 x <sup>2</sup>/<sub>5</sub> Δ<sub>oct</sub> = 2Δ<sub>oct</sub>. In the high-spin (lower) example, the CFSE is (3 x <sup>2</sup>/<sub>5</sub> Δ<sub>oct</sub>) - (2 x <sup>3</sup>/<sub>5</sub> Δ<sub>oct</sub>) = 0 - in this case, the stabilization generated by the electrons in the lower orbitals is canceled out by the destabilizing effect of the electrons in the upper orbitals. ===Optical properties=== The optical properties (details of absorption and emission spectra) of many [[coordination complex]]es can be explained by Crystal Field Theory. Often, however, the deeper colors of metal complexes arise from more intense [[Charge-transfer complex|charge-transfer excitations]].<ref name=MTarr2nd>G. L. Miessler and D. A. Tarr “Inorganic Chemistry” 2nd Ed. (Prentice Hall 1999), p.379 {{ISBN|0-13-841891-8}}.</ref>
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)