Lecture 3 Flashcards
1
Q
Why can’t we just consider spin momenta for lanthanides?
A
- 4f orbitals are core like and shielded from 5s and 5p electrons
- can no longer assume that angular momentum is quenched
2
Q
What scheme is used and how is it defined?
A
- Russel Saunders coupling
- S = total spin
- L= total orbital
- J = L+S,…L-S
3
Q
When is Russell-Sunders coupling appropriate
A
- when spin orbit coupling is weak in comparison to electron-electron repulsion
4
Q
What is used when spin orbit coupling is large in comparison to ligand field effects?
A
- Term symbols
- S is maximised
- The highest value of L is the lowest in energy
- For a shell that is less than half-filled J is as low as possible
- For a shell that is more than half-filled J is as high as possible
5
Q
What do term symbols assume?
A
- only the Ground state is populated
- true for Ln3+ ions
6
Q
What do Ln electronic spectra look like?
A
- all similar and independent of ion environment
- spin rules are not relaxed as in TM due to contracted 4f orbitals not interacting with ligands
- Sharp transitions
- less intense colours
7
Q
UV-Vis spectra of Ln
A
- intense absorptions
- due to allowed 4f to 5d transitions
8
Q
Ln Fluorescence
A
- F-F relaxation
- particularly favoured by Eu 3+ and Tb 3+ as their excited states are below the typical triplet states of ligands
9
Q
Magnetic properties of Actinides
A
- complex
- large spin orbit coupling but ligand effects are comparable due to extended 5f orbitals
- J values are split by the ligand field
- Ueff varies with temp
10
Q
Electronic spectra of actinides
A
- increased vibronic coupling
- broader and more intense peaks
- more intense colours
- later actinides represent Ln3+ more
- colours become paler across the series