Triplet-triplet annihilation

[1] Triplet-triplet annihilation was first discovered in the 1960s to explain the observation of delayed fluorescence in anthracene derivatives.

[9] The sensitizer absorbs the low energy photon and populates its first excited triplet state (T1) through intersystem crossing.

Both the emitter and sensitizer should have long triplet-state lifetimes so that the TTA mechanism has enough time to occur.

[9] In photolysis cancer therapy, light is used to selectively break bonds which releases and activates a target drug molecule.

The drug molecule can be released near or in tumour sites to combat the disease.

A Jablonski diagram describing the mechanism of triplet-triplet annihilation. The energy of the first triplet excited state (T 1 ) is transferred to a second triplet excited state (T 1 ), resulting in (1) the first T 1 returning to the singlet ground state S0 and (2) the second T 1 promoting to the singlet excited state (S 1 ).
A Jablonski diagram describing the sensitization process in triplet-triplet annihilation upconversion. The sensitizer first absorbs light and reaches its first singlet excited state (S 1 ). The sensitizer S 1 state undergoes intersystem crossing (ISC) to the triplet excited state (T 1 ). The sensitizer then transfers energy to the emitter, which returns the sensitizer T 1 to the ground state (S 0 ) and promotes the emitter to its T 1 .