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the source <strong>of</strong> the light emitted by the device.<br />

When the electron recombines with the hole, it is<br />

simply returning to its ground state. In doing so,<br />

it releases energy in the form <strong>of</strong> a photon. The<br />

higher the electron’s excited state, the shorter the<br />

wavelength <strong>of</strong> the photon it emits when it<br />

decays. This difference in energy between the<br />

excited state and the ground state is a material’s<br />

“bandgap”. The bandgap essentially determines<br />

the frequency <strong>of</strong> a photon that a material will<br />

emit. To create blue emitting materials, for<br />

example, the bandgap must be quite large,<br />

around 3.0eV.<br />

There are two particular ways in which an<br />

exciton decays. These processes are called<br />

fluorescence and phosphorescence, and they<br />

depend on the type <strong>of</strong> the exciton. The spins <strong>of</strong><br />

the ground state and excited state electrons<br />

determine its type. The two states are referred to<br />

as “singlet” and “triplet”. The relationship<br />

between the spins <strong>of</strong> the electron in the excited<br />

state and the electron in the ground state defines<br />

whether an exciton is a triplet or a singlet. As<br />

shown in Figure 2, if the spin <strong>of</strong> the excited<br />

electron is symmetrical to that <strong>of</strong> the ground<br />

state, the exciton is referred to as a triplet. If their<br />

spins are out <strong>of</strong> phase, the electrons form a<br />

singlet exciton. Triplet excitons are actually<br />

much more abundant than singlets, typically<br />

existing in a 3:1 ratio. This unequal formation<br />

occurs because the wave function <strong>of</strong> a triplet is<br />

lower in energy than a singlet, thus making<br />

triplets more energetically favorable.<br />

Fluorescence and phosphorescence are<br />

reliant upon whether a singlet or triplet decays.<br />

Fluorescence is the decay <strong>of</strong> singlet excitons,<br />

occurs instantaneously, and ceases when the<br />

source <strong>of</strong> excitation is removed.<br />

Phosphorescence is the decay <strong>of</strong> triplet excitons<br />

and occurs slowly over time- continuing after the<br />

source <strong>of</strong> excitation has been removed.<br />

Fluorescence is the preferred source for light<br />

emission because the decay <strong>of</strong> a singlet is an<br />

allowed process, but it has a problem. Since only<br />

25% <strong>of</strong> the excitons are formed as singlets at<br />

most, the device efficiency is limited.<br />

Unfortunately, the amount <strong>of</strong> singlets created<br />

cannot be controlled at this time. Emission from<br />

fluorescent materials alone simply lacks the<br />

efficiency to be used in devices that could<br />

compete in today’s world market.<br />

Phosphorescence also has a problem. It was<br />

reported that “Triplet states in organic materials<br />

were considered useless, since the energy <strong>of</strong><br />

triplets was believed to dissipate non-radiatively,<br />

as heat” (OIDA, 2002). The decay <strong>of</strong> a triplet is<br />

referred to as a “spin-forbidden” process. This<br />

spin-forbidden aspect <strong>of</strong> phosphorescent<br />

emission keeps fluorescent materials from being<br />

efficient in OLEDs.<br />

How can an OLED work if fluorescence by<br />

itself does not measure up to efficiency<br />

<strong>CMDITR</strong> <strong>Review</strong> <strong>of</strong> <strong>Undergraduate</strong> <strong>Research</strong> Vol. 1 No. 1 Summer 2004 51

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