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Unravelling the role of [Ru(bpy)2(OH2)2]2+ complexes in photo-activated chemotherapy.
The Photochemistry of Ru(bpy)32+
CHEM 6420
Primary Reference
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Photochemistry of Metal Complexes
• For metal complexes, the construction of Jablonski diagrams via electronic
configurations from the MO description follows the same general lines
described in Chapter 1 of this course for organic molecules
• A schematic MO diagram for an octahedral transition metal complex is
shown below:
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Photochemistry of Metal Complexes
• The various MOs can be conveniently classified according to their
predominant atomic orbital contributions as:
1) Strongly bonding, predominantly ligand-centered sL orbitals
2) Bonding, predominantly ligand-centered pL orbitals
3) Essentially nonbonding, metal-centered pM orbitals of t2g symmetry
4) Antibonding, predominantly metal-centered s*M orbitals of eg symmetry
5) Antibonding, predominantly ligand-centered p*L orbitals
6) Strongly antibonding, predominantly metal-centered s*M orbitals
• In the ground electronic configuration of an octahedral complex of a dn
metal ion, orbitals of type 1 and 2 are filled, while n electrons reside in the
orbitals of types 3 and 4
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Recap: Octahedral Metal Complexes
• The d orbital splitting is defined as the pattern of energies of the d orbitals,
and it results from the geometry of the complex
• You might recall from inorganic chemistry that crystal field theory predicts
the splitting
• A general rule for predicting splitting is that d orbitals that lie along the
bonds to the ligands are raised in energy, and the d orbitals that do not lie
along the bond axes are relatively unperturbed in energy
• For an octahedral complex (6 ligands around a metal ion), the d orbitals
are split into two sets, where the 𝑑𝑥𝑦 , 𝑑𝑥𝑧 , and 𝑑𝑦𝑧 orbitals are lower in
energy and the 𝑑𝑧 2 and 𝑑𝑥2 −𝑦2 orbitals are higher in energy
• The three lower-energy orbitals are collectively referred to as t2g, and the
two higher-energy orbitals as eg
eg
t2g
Image source: Wikipedia
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Photochemistry of Metal Complexes
• For metal complexes, one expects to find transitions of the following types:
1) Metal-centered (MC) transitions of type 3 → 4
2) Ligand-centered (LC) transitions of type 2 → 5
3) Ligand-to-metal charge-transfer (LMCT) transitions, e.g., type 2 → 4
4) Metal-to-ligand charge-transfer (MLCT) transitions, e.g., type 3 → 5
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Photochemistry of Metal Complexes
The relative energy ordering depends on the nature of the metal and ligands
• Low-energy MC transitions are expected for first-row transition-metals
• Low-energy LMCT transitions are expected when at least one of the
ligands is easy to oxidize and the metal is easy to reduce
• Low-energy MLCT transitions are expected when the metal is easy to
oxidize and a ligand is easy to reduce
• Low-energy LC transitions are expected for aromatic ligands with extended
p and p* orbitals
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Photochemistry of Metal Complexes
• For octahedral complexes of Ru(II), and the other d6 metal ions, the sL and
pL orbitals are fully occupied and the ground-state configuration is closedshell since the HOMO, pM(t2g)6, is also completely occupied
• The ground state is therefore a singlet, and the excited states are either
singlet or triplet in nature, similar to the organic molecules we’ve previously
studied
• In the case of [Ru(bpy)3]2+, since Ru(II) is easy to oxidize and the 2,2’bipyridine ligands are easy to reduce, the lowest triplet and singlet excited
states are MLCT character
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Bimolecular Processes
• In fluid solution, when the excited state is sufficiently long, an excited
molecule *R may have a chance to encounter another molecule, M
• In such a case, some specific interaction can occur leading to the
deactivation of *R by second-order kinetic processes
• The most important types of interactions in an encounter are those leading
to electron- or energy-transfer
*R + M → R•+ + M•−
Oxidative electron-transfer
*R + M → R•− + M•+
Reductive electron-transfer
*R + M → R + *M
Energy transfer
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Bimolecular Processes
• Reminder: an excited state is both a stronger reductant and stronger
oxidant than the corresponding ground state (Chapter 7)
• The redox potentials of the excited state may be calculated from the
ground state oxidation and reduction potentials and the one-electron
potential corresponding to the zero–zero excited state energy, E0−0, as
shown by eq 1 and 2:
E(R•+/*R) ≈ E(R•+/R) − E0−0
(1)
E(*R/R•−) ≈ E(R/R•−) + E0−0
(2)
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Structure, Bonding, and Excited States of Ru(II)L6 Complexes
• Ru2+ is a d6 system and the polypyridine ligands are usually colorless
molecules possessing s donor orbitals localized on the nitrogen atoms and
p donor and p* acceptor orbitals delocalized on aromatic rings
• The figure below is a simplified MO diagram of Ru(II) polypyridine
complexes showing the possible electronic transitions
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Structure, Bonding, and Excited States of Ru(II)L6 Complexes
• Ru(bpy)32+, as well as most of the Ru(LL)32+ complexes (LL = bidendate
polypyridine ligand), exhibits a D3 symmetry
• A more detailed picture of the MO diagram is shown below
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Structure, Bonding, and Excited States of Ru(II)L6 Complexes
• For most Ru(II) polypyridine complexes, the lowest excited state is a
3MLCT state which undergoes relatively slow radiationless transitions and
thus exhibits relatively a long lifetime and intense luminescence emission
• Such a state is obtained from promoting an electron from a metal pM orbital
to a ligand p*L orbital
• The same p*L orbital is usually involved in one-electron reduction
processes
• It has long been discussed whether in homoleptic complexes the emitting
3MLCT state is best described with a multi-chelate ring-delocalized orbital
(a) or a single chelate ring-delocalized orbital (b), but there is compelling
evidence of “spatially isolated” redox orbitals (b)
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Ru(bpy)32+: Absorption Spectrum
• The absorption spectrum of Ru(bpy)32+ is shown below along with the
proposed assignments
• The bands at 185 nm (not shown) and 285 nm have been assigned as
spin-allowed LC p → p* transitions by comparison with the spectrum of
protonated bipyridine
• The two remaining intense bands at 240 and 450 nm have been assigned
to spin-allowed MLCT d → p* transitions
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Ru(bpy)32+: Emission Properties
• Excitation of Ru(bpy)32+ in any of its absorption bands leads to a
luminescence emission whose intensity, lifetime, and energy position are
more or less temperature dependent
• Detailed studies on the temperature dependence showed that
luminescence originates from three closely spaced levels in thermal
equilibrium
• This cluster of luminescent, closely spaced excited states will be indicated
in the following by *Ru(bpy)32+ or as the 3MLCT state
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Ru(bpy)32+: Emission Properties
• In rigid glass at 77 K the emission lifetime of *Ru(bpy)32+ is ~ 5 ms and the
emission quantum yield is ~ 0.4
• Taken together with the unitary intersystem crossing efficiency, these
figures yield a value of ~ 13 ms for the radiative lifetime
• Values of this order of magnitude have been found for MLCT states of
other transition metal complexes
• LC excited states of transition metal complexes usually exhibit radiative
lifetimes in the millisecond range
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Ru(bpy)32+: Emission Properties
• In the 77 K emission spectrum of Ru(bpy)32+, there is some vibrational
structure
• This structure has been assigned to the C–N and C–C stretching of the
aromatic rings
• This provides an indication of the dominant modes for deactivation of the
3MLCT state
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Quenching of the 3MLCT Excited State
• The lowest 3MLCT excited state of Ru(bpy)32+ lives long enough to
encounter other solute molecules (even when present at relatively low
concentrations) and possesses suitable properties to play the role of
energy donor, electron donor, or electron acceptor
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Quenching of the 3MLCT Excited State
• The energy available to *Ru(bpy)32+ for energy transfer processes is 2.12
eV, or 49 kcal mol−1
• The reduction and oxidation potentials are + 0.84 and -0.86 V (aqueous
solution, vs. SCE)
*RuII(bpy)32+ + Q → RuII(bpy)32+ + *Q
*RuII(bpy)32+ + Q → RuIII(bpy)33+ + Q⦁−
*RuII(bpy)32+ + Q → RuII(bpy)2(bpy⦁−)+ + Q⦁+
energy transfer
oxidative quenching
reductive quenching
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