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
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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
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3
Q

When is Russell-Sunders coupling appropriate

A
  • when spin orbit coupling is weak in comparison to electron-electron repulsion
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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
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5
Q

What do term symbols assume?

A
  • only the Ground state is populated

- true for Ln3+ ions

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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
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7
Q

UV-Vis spectra of Ln

A
  • intense absorptions

- due to allowed 4f to 5d transitions

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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

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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
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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
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