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Furthermore, we analyzed soil solutions sampled with piezometer, porous cups, and at the drain outlet.
This significantly increases the SB width due to increased depletion at the drain end.
Similarly, drain extension also induces the electron plasma at the drain side.
The charge generated by a radiation strike at the drain of the bias current transistor results in voltage change at the drain node, which causes change in the output impedance of the transistor.
The value of ΔV is increased up to ∼116 V at the drain source voltage of 2 V with great stability.
The drain-end carrier velocity is smaller than the ultimate saturation velocity due to the presence of a finite electric field at the drain.
Also, the hot carrier effect minimizes with reduction of the peak of the electric field at the drain side of the HD-CNTFET.
Polarity gate induces p+ region at the source side and n+ region at the drain side, instead of relying on the abrupt doping profile at the junctions.
Output characteristics show that substantial kink effect reduction can be achieved when the sub-TFT placed at the drain end of the device has an L2 ≪ L1.
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For this we investigate the influence of drain-extension and HALO doping gradients at the drain-extension channel junction (DECJ).
But increasing V DS would finally result in tunneling at the drain-channel side.
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