Growth and physical properties of crystalline rubrene - BOA Bicocca ...
Growth and physical properties of crystalline rubrene - BOA Bicocca ...
Growth and physical properties of crystalline rubrene - BOA Bicocca ...
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2.6 Oxidation <strong>of</strong> <strong>crystalline</strong> <strong>rubrene</strong> 21<br />
Figure 2.9: Depth pr<strong>of</strong>iles <strong>of</strong> <strong>rubrene</strong> peroxide concentration in <strong>rubrene</strong> thin films<br />
with different degrees <strong>of</strong> crystallinity as determined by mass spectrometry. From<br />
[19].<br />
<strong>crystalline</strong> <strong>rubrene</strong> there is less room for the molecular conformational change<br />
upon <strong>rubrene</strong> peroxide formation. Nonetheless this result demonstrate the<br />
presence <strong>of</strong> a non negligible amount <strong>of</strong> <strong>rubrene</strong> peroxide even in the first few<br />
layers <strong>of</strong> <strong>rubrene</strong> crystals exposed to air. This has also been confirmed by<br />
Mitr<strong>of</strong>anov et al., comparing the PL spectra <strong>of</strong> pristine <strong>rubrene</strong> single crys-<br />
tals with those <strong>of</strong> <strong>rubrene</strong> single crystals oxidized on purpose by exposing<br />
them to a pure oxygen atmosphere for several hours[69]. The PL spectra<br />
collected at various temperatures, reported in figure 2.10a <strong>and</strong> referring to<br />
pristine (left) <strong>and</strong> oxidized (right) samples, show a clear change <strong>of</strong> the PL<br />
b<strong>and</strong>s upon oxidation, in particular with the appearance <strong>of</strong> a b<strong>and</strong> around<br />
650 nm, attributed to the electronic transitions from a b<strong>and</strong>gap state in-<br />
duced by <strong>rubrene</strong> peroxide. By two-photon spectroscopy the authors have<br />
also been able to measure the PL spectra <strong>of</strong> the oxidized samples as a func-<br />
tion <strong>of</strong> depth in the crystal. The results, reported in figure 2.10b, show that<br />
the <strong>rubrene</strong> peroxide PL b<strong>and</strong> is present only in the spectra collected from<br />
the sample surface, while the spectra collected from the bulk resemble those<br />
<strong>of</strong> pristine <strong>rubrene</strong> crystals, in agreement with the mass spectrometry data<br />
previously discussed.<br />
The actual origin <strong>of</strong> the 650 nm PL b<strong>and</strong>, which is <strong>of</strong>ten related to oxy-<br />
gen induced b<strong>and</strong>gap states, is however still unclear. Recently Chen et al.<br />
have carried out a systematic study on this particular b<strong>and</strong> <strong>and</strong> their find-<br />
ings suggest that it actually originates from amorphous inclusions in <strong>rubrene</strong>