• Journal of the Korean Institute of Telematics and Electronics A
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• v.29A no.7
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• pp.82-88
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• 1992

This paper presents one of the first comprehensive studies of how hot electron degradation impacts the input offset voltage of a CMOS differential amplifiers. This study utilizes the concept of a virtual source-coupled MOSFET pair in order to evaluate offset voltaged egradation directly from individual device measurement. Next, analytical models are developed to describe the offset voltage degradation. These models are used to examine how hot electron induced offset voltage is affected with the device parameters.

• Journal of the Korean Institute of Telematics and Electronics A
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• v.31A no.1
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• pp.77-83
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• 1994

Characteristics of hot-electron-induced degradation by AC, DC was investigated for p-MOSFET's(W/L=25/l$\mu$m) with sub-10nm RTP-CVD gate oxides. It was confirmed that the surface channel p-MOSFET of a thinner gate oxide shows less degradation. Mechanisms for this effect were analyzed using a simple MOS Device degradation model. It was found that the number of generated electron traps(fixed charge) is determined by the amount of peak gate current, dependent of the gate oxide thickness, and the major cause of the smaller degradation in the thinner gate oxide devices is the lower hot electron trapping carriers.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.41 no.7
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• pp.21-29
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• 2004

Hot carrier degradation characteristics of Nano-scale CMOSFETs with dual gate oxide have been analyzed in depth. It is shown that, PMOSFET lifetime dominate the device lifetime than NMOSFET In Nano-scale CMOSFETs, that is, PMOSFET lifetime under CHC (Channel Hot Carrier) stress is much lower than NMOSFET lifetime under DAHC (Dram Avalanche Hot Carrier) stress. (In case of thin MOSFET, CHC stress showed severe degradation than DAHC for PMOSFET and DAHC than CHC for NMOSFET as well known.) Therefore, the interface trap generation due to enhanced hot hole injection will become a dominant degradation factor in upcoming Nano-scale CMOSFET technology. In case of PMOSFETs, CHC shows enhanced degradation than DAHC regardless of thin and thick PMOSFETs. However, what is important is that hot hole injection rather than hot electron injection play a important role in PMOSFET degradation i.e. threshold voltage increases and saturation drain current decreases due to the hot carrier stresses for both thin and thick PMOSFET. In case of thick MOSFET, the degradation by hot carrier is confirmed using charge pumping current method. Therefore, suppression of PMOSFET hot carrier degradation or hot hole injection is highly necessary to enhance overall device lifetime or circuit lifetime in Nano-scale CMOSFET technology

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.40 no.10
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• pp.32-38
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• 2003

This works reports the measurement and analysis results on the hot electron induced device degradation in Gate-All-Around SOI MOSFET's, which were fabricated using commercially available SIMOX material. It is observed that the worst-case condition of the device degradation in nMOSFETs is $V_{GS}$ = $V_{TH}$ due to the higher impact ionization rate when the parasitic bipolar transistor action is activated. It is confirmed that the device degradation is caused by the interface state generation from the extracted degradation rate and the dynamic transconductance measurement. The drain current degradation with the stress gate voltages shows that the device degradation of pMOSFETs is dominantly governed by the trapping of hot electrons, which are generated in drain avalanche hot carrier phenomena.r phenomena.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.35D no.11
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• pp.62-69
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• 1998

The general degradation model has been applied to analyze the hot carrier induced degradation of the DC and RF characteristics of RF-nMOSFET. The degradation of cut-off frequency has been severer than the degradation of bulk MOSFET drain current. The value of the degradation rate n and the degradation parameter m for RF-nMOSFET has been equal to those for bulk MOSFET. The decrease of device degradation with the increase of fingers could be explained by the large source/drain parasitic resistance and drain saturation voltage. It has been also found that the RF performance degradation could be explained by the decrease of $g_{m}$ and $C_{gd}$ and the increase of $g_{ds}$ after stress. The degradation of the DC and RF characteristics of RF-nMOSFET could be predicted by the measurement of the substrate current.t.

• Journal of the Korean Institute of Telematics and Electronics A
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• v.30A no.9
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• pp.38-45
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• 1993

In this study, the degradation characteristics of drain output resis-tance was described due to hot electron effects. An semi-empirical model for the degraded drain output resistance was derived from the measured device characteristics. The suggested model was verified from the measured data and the device parameter dependence was also analyzed. The degradation of drain output resistance was increased with stress time and had linear relationship with the degradation of drain current. The device lifetime which was defined by failure criteria of drain output resistance (such as $\Delta$ro/roo=5%) was equivalent to that of failure criteria of drain current (such as $\Delta$ID/ID=5%)

• Journal of the Korean Institute of Telematics and Electronics
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• v.25 no.7
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• pp.780-790
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• 1988

We have studied the hot-carrier-induced degradation caused by the high channel electric field due to the decrease of the gate length of MOSFET used in VLSI. Under DC stress, the condition in which maximum substrate current occures gave the worst degradation. Under AC dynamic stress, other conditions, the pulse shape and the falling rate, gave enormous effects on the degradation phenomena, especially at 77K. Threshold voltage, transconductance, channel conductance and gate current were measured and compared under various stress conditions. The threshold voltage was almost completely recovered by hot-injection stress as a reverse-stress. But, the transconductance was rapidly degraded under hot-hole injection and recovered by sequential hot-electron stress. The Si-SiO2 interface state density was analyzed by a charge pumping technique and the charge pumping current showed the same trend as the threshold voltage shift in degradation process.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.40 no.9
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• pp.638-643
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• 2003

Channel width dependence of hot-carrier effect in nMOSFET with shallow trench isolation is analyzed. $I_{sub}$- $V_{G}$ and $\Delta$ $I_{ㅇ}$ measurement data show that MOSFETs with narrow channel-width are more susceptible to the hot-carrier degradation than MOSFETs with wide channel-width. By analysing $I_{sub}$/ $I_{D}$, linear $I_{D}$- $V_{G}$ characteristics, thicker oxide-thickness at the STI edge is identified as the reason for the channel-width dependent hot-carrier degradation. Using the charge-pumping method, $N_{it}$ generation due to the drain avalanche hot-carrier (DAHC) and channel hot-electron (CHE) stress are compared. are compared.

• Journal of the Korean Institute of Telematics and Electronics A
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• v.33A no.4
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• pp.129-135
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• 1996

In this paper, the hot carrier effect and device degradation of deep submicrometer SC-PMOSFETs have been measured and characterized. It has been shown that the substrate current of a 0.15$\mu$m PMOSFET increases with increasing of impact ionization rate, and the impact ionization rate is a function of the gate length and gate bias voltage. Correlation between gate current and substrate current is investigated within the general framework of the lucky-electron. It is found that the impact ionization rate increases, but the device degradation is not serious with decreasing effective channel length. SCIHE is suggested as the possible phusical mechanism for enhanced impact ionization rate and gate current reduction. Considering the hot carrier induced device degradation, it has been found that the maximum supply voltage is about -2.6V for 0.15$\mu$m PMOSFET.

• Journal of the Korean Institute of Telematics and Electronics A
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• v.31A no.8
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• pp.72-79
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• 1994

In this paper semi empirical models are presented for the hot electron induced threshold voltage shift(${\Delta}V_{t}$) and effective channel shortening length (${\Delta}L_{H}$) in degraded PMOSFET. Trapped electron charges in gate oxide are calculated from the well known gate current model and ΔLS1HT is calculated by using trapped electron charges. (${\Delta}L_{H}$) is a function of gate stress voltage such as threshold voltage shift and degradation of drain current. From the correlation between (${\Delta}L_{H}$) has a logarithmic function of stress time. From the measured results, (${\Delta}V_{t}$) and (${\Delta}L_{H}$) are function of initial gate current and device channel length.