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tesi R. Miscioscia.pdf - EleA@UniSA

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92 Chapter 3<br />

figure 7: Output characteristics of PI device after thermal annealing (dotted: experimental; line:<br />

model fitting simulations with MOS ideal model).<br />

For PS and PR samples, the same characterization steps before and<br />

after annealing have been carried-out. For PS, the fitting results have<br />

shown in both conditions (see figure 8 and figure 9) the presence of a<br />

contact barrier voltage (VC), as also reported in [11]. In this case, the<br />

undesired current affects the characteristics at low VDS and the fittings<br />

show a dependence from the only VGS bias, which can be modeled by<br />

IG~VGS 4 (as in eq. 2) due to Trap-Charge-Limited Space-Charge-<br />

Limited-Current (TCL SCLC). In this case, we detected the presence<br />

of a Source-Drain contact barrier, modeled in eq. 2 through the VC<br />

voltage shift of the VDS as suggested by Horowitz [11].<br />

2 4<br />

[ ] − V<br />

eq. 2 = −K<br />

( V −V<br />

)( V −V<br />

) − ( V −V<br />

)<br />

I S 2 GS T DS C DS C α SG<br />

Here, the baking treatment decreases the non-ideality factor α but<br />

keeps the same power law exponent, as appears from fittings shown in<br />

figure 9 with the eq. 2 model.

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