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Because the carriers are mainly confined at the interface between the pentacene and insulator, and the electric-field profile Ex is almost invariable along the depth of the OFET, we only focused on the carrier density and electric field at the interface in this work.
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Because the carriers are mainly confined at the interface between the pentacene and insulator, and the electric-field profile Ex is almost invariable along the depth of the OFET, we only focused on the carrier density and electric field at the interface in this work.
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18
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52949091103
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If the source could not provide enough injection carriers to compensate the loss of the carriers under the edge of the source, the migration of Ex would be completely different from what we discussed here. We have observed this phenomenon in the TRM-SHG experiment.
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If the source could not provide enough injection carriers to compensate the loss of the carriers under the edge of the source, the migration of Ex would be completely different from what we discussed here. We have observed this phenomenon in the TRM-SHG experiment.
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52949120245
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The approximation of the electric field is crucial to the accuracy of Eq. 3. The simulation showed that it would be good at a relatively large time after a switching of the gate and drain voltages.
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The approximation of the electric field is crucial to the accuracy of Eq. 3. The simulation showed that it would be good at a relatively large time after a switching of the gate and drain voltages.
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20
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52949102867
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In our previous paper (Ref.), the carrier motion was analyzed in accordance with standard time-of-flight approach, where linear carrier motion with time was assumed.
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In our previous paper (Ref.), the carrier motion was analyzed in accordance with standard time-of-flight approach, where linear carrier motion with time was assumed.
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22
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0043190025
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