tesi R. Miscioscia.pdf - EleA@UniSA
tesi R. Miscioscia.pdf - EleA@UniSA
tesi R. Miscioscia.pdf - EleA@UniSA
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Chapter 4 135<br />
μ (cm 2 V -1 s -1 )<br />
1.0<br />
0.8<br />
0.6<br />
0.4<br />
0.2<br />
0.0<br />
-0.2<br />
μ(W g ) = - 0.27 + 0.87 W g<br />
After Esseni's I ch extraction<br />
0.2 0.4 0.6 0.8 1.0 1.2 1.4<br />
Lateral grain size (μm)<br />
figure 19: extrapolation of a linear trend from the field-effect mobilities versus mean pentacene<br />
grain dimensions for polymeric dielectrics-based OTFTs (black symbols). Red squares are<br />
PFTEOS:TEOS samples mobilities.<br />
As we can observe in figure 19, the mobility trend in samples<br />
having polymeric dielectric is strongly dependent from channel’s<br />
morphology but also the anomaly of PFTEOS:TEOS samples is still<br />
evident if we remind figure 13.<br />
By interpolating all the symbols but the red ones (the first on<br />
the left and the last on the right in the plot), we obtained an estimation<br />
line for transistor’s performances as the channel film morphology<br />
changes.<br />
The major differences introduced by Ich estimation are, instead,<br />
evident in thermal analyses that allow now to distinguish some<br />
important features of PFTEOS:TEOS samples in comparison with<br />
PMMA samples.<br />
Looking at figure 20, we see that the activation energy curves<br />
are now more separated and denote the dependence of the thermal<br />
activation from thickness and nature of gate dielectric in OTFTs. They<br />
still keep the usual decreasing behavior with the gate field intensity