DC Exploration of Oxide Trap Charge Effects on Electrically Doped Nano Ribbon FET

Author(s):  
Annada Shankar Lenka ◽  
Prasanna Kumar Sahu ◽  
Sayan Bagchi
2021 ◽  
Vol 21 (8) ◽  
pp. 4252-4257
Author(s):  
Tae Jun Ahn ◽  
Yun Seop Yu

We investigated the effect of the interface trap charge in a monolithic three-dimensional inverter structure composing of JLFETs (M3DINV-JLFET), using the interface trap charge distribution extracted in the previous study. The effect of interface trap charge was compared with a conventional M3DINV composing of MOSFETs (M3DINV-MOSFETs) by technology computer-aided design simulation. When the interface trap charges in both M3DINV-JLFET and M3DINV-MOSFET are added, the threshold voltages, on-current levels, and subthreshold swings of both JLFETs and MOSFETs increase, decrease, and increase, respectively, and switching voltages and propagation delays of M3DINV are shifted and increased, respectively. However, since JLFET and MOSFET have different current paths of bulk and interface in channel, respectively, MOSFET is more affected by the interface trap, and M3DINV-JLFET has almost less effect of interface trap at different thickness of interlayer dielectric, compared to M3DINV-MOSFET.


2016 ◽  
Vol 63 (4) ◽  
pp. 1478-1485 ◽  
Author(s):  
Binit Syamal ◽  
Xing Zhou ◽  
Siau Ben Chiah ◽  
Anand M. Jesudas ◽  
Subramaniam Arulkumaran ◽  
...  

2015 ◽  
Vol 55 (5) ◽  
pp. 789-794 ◽  
Author(s):  
Syed Mukulika Dinara ◽  
Saptarsi Ghosh ◽  
Nripendra N. Halder ◽  
Ankush Bag ◽  
Sekhar Bhattacharya ◽  
...  

Electronics ◽  
2019 ◽  
Vol 8 (6) ◽  
pp. 657 ◽  
Author(s):  
Mohan Liu ◽  
Wu Lu ◽  
Xin Yu ◽  
Xin Wang ◽  
Xiaolong Li ◽  
...  

The latent enhanced low dose rate sensitivity (ELDRS) effect is observed in the double-polysilicon self-aligned (DPSA) technology PNP bipolar junction transistor (BJT) irradiated with a high and low dose rate gamma ray, which is discussed from the perspective of the three-stage degradation rate of the excess base current. The great degradation rate as a result of the high dose irradiation of the first stage is dominantly ascribed to the positive oxide trap charges accumulated during a short irradiation, and then due to the competition between the recombination of electrons and capture of the hole by the traps. It declined sharply into a degradation rate saturated region of the second stage. However, for the low dose rate, the small increase in the degradation rate in the first stage is caused by the holes escaping from the initial recombination and being transported to the interface to form the interface states. Then, the competition between the steadily increasing interfacial trap charge and the continuously annealed shallow level oxide trap charge leads to the stable increase of degradation under low dose irradiation. Finally, in stage three, the increases of the degradation rates for high and low dose irradiation result from the different amounts of the hydrogen molecules generated by the hole reactive with depassiviated Si suspended bonds, which can interact with the deep level defects and release protons, causing an increase of interfacial trap charges with prolonged irradiation.


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