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44734-AC1
Polyphospholes and Hetero Analogs

Francois Mathey, University of California Riverside

Progress report

The essence of our project is to use our original phosphole functionalization technique as depicted in scheme (1)1 to prepare new families of phosphole-heterole oligomers for optoelectronic applications. After several attempts, we were able to devise an access to

original phosphole-silylene-thiophene chains. These results have been described in our previous report. For practical applications, this synthesis proved to be somewhat difficult to upscale. We thus decided to look for other types of conjugated phosphole oligomers both original and accessible via our functionalization technique. We have found such a family of products and started to investigate its optoelectronic properties in collaboration with our UCR colleague, professor Christopher J. Bardeen.

Synthetic results

Three groups have definitively established the fact that conjugated thiophene-phosphole oligomers display an impressive potential for the manufacture of organic light emitting diodes (OLED's). A typical product developed by the group of Rau is phosphole gold complex (1).2 Dithienophosphole (2) is representative of the work of Baumgartner.3 Finally, Matano has recently developed another type of thieno-annellated phosphole represented by (3).4

These results have served as a basis for our new work.

We first synthesized several polythienyl-substituted phospholes as shown in scheme (2).

Then, we investigated the thermal behavior of (5a-5c) in the presence of KOtBu. The choice of the solvent proved to be critical. At 150oC in diglyme, a clean reaction takes place to give the expected phospholides (6a-6c) (Scheme 3).

The phospholides were characterized as their 1-methylphosphole borane complexes. Compound (7b) was also characterized by X-ray crystal structure analysis (fig. 1). The most characteristic features of the structure are the perfect coplanarity of the three rings, the high dissymmetry of the phosphole ring (P1-C1 1.762(3) vs P1-C4 1.810(3) ) and the short bridge bonds between the rings (C4-C5 1.443(4) and C8-C9 1.452(4) ).

Figure 1: X-ray crystal structure analysis of (7b).

Optical properties

Table (1) summarizes the quantum yield and lifetime measurements for compounds 7b and 7c as well as those of terthiophene and quaterthiophene.

TABLE 1

labs(nm)

lfl(nm)

tfl (ns)

Ffl

Dm

7b

384.3, 382.6

469.5,476.4

0.100

0.016

3.8

7c

410.7, 409.1

502.0, 511.0

1.22

0.178

4.4

terthiophene

354.5, 354.3

421.6, 420.5

0.188

0.060

0.4

quaterthiophene

392

478

0.49

0.18

-

Table 1.  Spectroscopic parameters for oligothiophenes and phosphole analogs made in this work.  For the peak absorption and fluorescence wavelengths labs and lfl, the first value is in toluene and second is in CH2Cl2.

An important difference between the thiophene and phosphole compounds is the fact that the absorption and emission are shifted to longer wavelengths in the phosphole compounds. The shift in wavelength, along with differences in the fluorescence lifetimes, suggest that the excited states in 7b and 7c have different electronic characteristics from those of pure oligothiophenes.  To further probe the nature of the excited states, we varied the polarity of the solvent.  Excited states with more charge transfer character should show fluorescence spectra that shift to lower energies in more polar solvents.  That is exactly what we see in the phosphole analog 7c (Figure 2).

Figure 2:  Black = 7c absorption in 100% toluene.  The absorption in 100% CH2Cl2 is the same.  Purple = fluorescence in 100% toluene; blue = fluorescence in 75% toluene:25% CH2Cl2; green = fluorescence in 50% toluene:50% CH2Cl2; orange fluorescence in 25% toluene:75% CH2Cl2; red = fluorescence in 100% CH2Cl2.  Note that terthiophene shows at most a 1 nm shift under the same conditions. 

From these data, using the Lippert-Mataga formula, we can extract the change in dipole moment upon photon absorption (Dm), which gives an indication of the charge transfer nature of the excited state.5 For terthiophene, the change in dipole is only 0.6 Debye, while for 7b  and 7c, the changes are 3.8 and 4.4 Debye respectively, with about 10% error in all values.  The larger values for Dm confirm that the phosphole analogs have excited states with greater charge transfer character than the oligothiophenes.

<>Future work

Contrary to the other phosphole-thiophene conjugated oligomers (1)-(3), our compounds display a highly dissymmetrical structure and a huge charge transfer in the excited state. We can modulate this transfer by replacing the terthiophene by a longer oligothiophene, changing the substitution at phosphorus and grafting a functional substituent at the a' position of the phosphole ring using the chemistry of scheme (1).

References

1)    Holand, S.; Jeanjean, M.; Mathey, F. Angew. Chem. Int. Ed. Engl. 1997, 36, 98.

2)    Su, H.-C.; Fahdel, O.; Yang, C.-J.; Cho, T.-Y.; Fave, C.; Hissler, M.; Wu, C.-C.; Rau, R. J. Am. Chem. Soc, 2006, 128, 983.

3)    Dienes, Y.; Durben, S.; Krpti, T.; Neumann, T.; Englert, U.; Nyulaszi, L.; Baumgartner, T. Chem. Eur. J. 2007, 13, 7487.

4)    Miyajima, T.; Matano, Y.; Imahori, H. Eur. J. Org. Chem. 2008, 255.

5)    Hirata, Y.; Mataga, N. J. Phys. Chem. 1984, 88, 3091.


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