Generally what you are looking for is generation of singlet (
1Δ
g) oxygen. The ground electronic state of oxygen (dioxygen) is a singlet state (
3Σ
g-). You cannot photogenerate singlet oxygen directly because the transition is forbidden by symmetry and by spin (and by parity – three strikes against it!). But you can photogenerate it indirectly by an energy transfer reaction from a photogenerated triplet state in a photosensitizer.
Here's a quick lesson in photophysics you may find useful.
If S is our photosensitizer, in the absence of oxygen (* = excited state):
1)
1S + hν
1 1S* (photoexcitation)
One of three things happens now:
2)
1S*
1S + heat (internal conversion)
3)
1S*
1S + hν
2 (fluorescence)
4)
1S*
3S* + heat (intersystem crossing)
If (4), then one of two things generally happen:
5)
3S*
1S + hν
3 (phosphorescence)
6)
3S*
1S + heat (intersystem crossing)
Each process has an associated rate constant that is determined by a lot of molecular structural parameters and quantum phenomena. What's important to know is that anything that when it comes to direct transitions involving light, anything with a singlet to singlet conversion is USUALLY fast and anything with a singlet to triplet (or vice-versa) conversion is USUALLY slow. Typically heat-producting relaxations have fast rates, so phosphorescence and fluorescence (particularly the former) are usually minor processes EXCEPT in more rigid molecules and molecules with larger HOMO-LUMO gaps, which have slower rates of internal conversion for various reasons that you probably don't care about.
Anyway, in molecules that have efficient intersystem crossing - including porphyrins with closed-shell metals - pathway 4 becomes competitive and a large population of long lived excited triplet states can be generated. If this happens, and oxygen is present, the following photochemical conversion can take place:
7)
3S* +
3Σ
g- O
2 1S +
1Δ
g O
2*
It may not be immediately apparent that spin is conserved here but it is. The sensitizer goes from an excited triplet to a ground singlet and oxygen goes from a ground triplet to an excited triplet. So the total change in spin is conserved, so the reaction is fast. This can only happen if the sensitizer is a triplet. It can also only happen obviously if the sensitizer triplet state is higher energy than the oxygen singlet state, which is approximately 95 kJ/mol. That’s pretty low and most conjugated chromophores have lowest lying electronic states well above that, which means most chromophores COULD sensitize singlet oxygen. The limiting factor really is efficient intersystem crossing in the excited chromophore, which (thankfully for us, as it turns out, because if we had singlet oxygen being generated everywhere, it’d tear us all to shreds), most aren’t.
Oh and if you’re wondering why singlet oxygen is such a powerful oxidizing agent, it’s because, unlike ground-state (triplet) oxygen, its reactions with organic substrates (mostly ground state singlets) are not (again) spin forbidden. Most reactions between ground state triplet oxygen and organic substrates are thermodynamically favorable but kinetically slow because spin isn’t conserved when these reactions take place. Singlet oxygen on the other hand has loads of energy to spare and it’s kinetically fast because there’s no spin-associated kinetic barrier.