Comment on “Channel Length and Threshold Voltage Dependence of a Transistor Mismatch in a 32-nm HKMG Technology”

2011 ◽  
Vol 58 (4) ◽  
pp. 1255-1256 ◽  
Author(s):  
Terence B. Hook ◽  
Jeffrey B. Johnson ◽  
Augustin Cathignol ◽  
Antoine Cros ◽  
Gérard Ghibaudo
2010 ◽  
Vol 57 (10) ◽  
pp. 2440-2447 ◽  
Author(s):  
Terence B Hook ◽  
Jeffrey B Johnson ◽  
Jin-Ping Han ◽  
Andrew Pond ◽  
Takashi Shimizu ◽  
...  

Electronics ◽  
2019 ◽  
Vol 8 (6) ◽  
pp. 611 ◽  
Author(s):  
Ik Joon Chang ◽  
Yesung Kang ◽  
Youngmin Kim

Reducing a supply voltage in order to minimize power consumption in memory is a major design consideration in this field of study. In static random access memory (SRAM), optimum energy can be achieved by reducing the voltage near the threshold voltage level for near threshold voltage computing (NTC). However, lowering the operational voltage drastically degrades the stability of SRAM. Thus, in conventional 6T SRAM, it is almost impossible to read exact data, even when a small process variation occurs. To address this problem, an 8T SRAM structure is proposed which can be widely used for improving the read stability at lower voltage operation. In this paper, we investigate the channel length biasing effect on the read access transistor of the 8T SRAM in NTC and compare this with 6T SRAM. Read stability can be improved by suppressing the leakage current due to the longer channel length. Simulation results show that, in NTC, up to a 12× read-error reduction can be achieved by the 20 nm channel length biasing in the 8T SRAM compared to 6T SRAM.


2001 ◽  
Vol 686 ◽  
Author(s):  
Michele L. Ostraat ◽  
Jan W. De Blauwe

AbstractA great deal of research interest is being invested in the fabrication and characterization of nanocrystal structures as charge storage memory devices. In these flash memory devices, it is possible to measure threshold voltage shifts due to charge storage of only a few electrons per nanocrystal at room temperature. Although a variety of methods exist to fabricate nanocrystals and to incorporate them into device layers, control over the critical nanocrystal dimensions, tunnel oxide thickness, and interparticle separation and isolation remains difficult to achieve. This control is vital to produce reliable and consistent devices over large wafer areas. To address these control issues, we have developed a novel two-stage ultra clean reactor in which the Si nanocrystals are generated as single crystal, nonagglomerated, spherical aerosol particles from silane decomposition at 950°C at concentrations exceeding 108 cm−3 at sizes below 10 nm. Using existing aerosol instrumentation, it is possible to control the particle size to approximately 10% on diameter. In the second reactor, particles are passivated with a high quality oxide layer with shell thickness controllable from 0.7 to 2.0 nm. The two-stage aerosol reactor is integrated to a 200 mm wafer deposition chamber such that controlled particle densities can be deposited thermophoretically. With nanocrystal deposits of 1013 cm−2, contamination of transition metals and other elements can be controlled to less than 1010 atoms cm−2.We have fabricated 0.2 μm channel length aerosol nanocrystal floating gate memory devices using conventional MOS ULSI processing on 200 mm wafers. The aerosol nanocrystal memory devices exhibit normal transistor characteristics with drive current 30 μA/μm, subthreshold slope 200 mV/dec, and drain induced barrier lowering 100 mV/V, typical values for thick gate dielectric high substrate doped nonvolatile memory devices. Uniform Fowler-Nordheim tunneling is used to program and erase these memory devices. Despite 5 nm tunnel oxides, threshold voltage shifts > 2 V have been achieved with microsecond program and millisecond erase times at moderate operating voltages. The aerosol devices also exhibit excellent endurance cyclability with no window closure observed after 105 cycles. Furthermore, reasonable disturb times and long nonvolatility are obtained, illustrating the inherent advantage of discrete nanocrystal charge storage. No drain disturb was detected even at drain biases of 4V, indicating that little or no charge conduction occurs in the nanocrystal layer. We have demonstrated promise for aerosol nanocrystal memory devices. However, numerous issues exist for the future of nanocrystal devices. These technology issues and challenges will be discussed as directions for future work.


2010 ◽  
Vol 645-648 ◽  
pp. 961-964 ◽  
Author(s):  
Jang Kwon Lim ◽  
Mietek Bakowski ◽  
Hans Peter Nee

The 1.2 kV 4H-SiC buried-grid vertical JFET structures with Normally-on (N-on) and Normally-off (N-off) design were investigated by simulations. The conduction and switching properties were determined in the temperature range from -50°C to 250°C. In this paper, the characteristics of the N-on designs with threshold voltage (Vth) of -50 V and -10 V are compared with the N-off design (Vth=0). The presented data are for devices with the same channel length at 250°C. The results show that the on-resistance (Ron) decreases with increasing channel doping concentration and decreasing channel width. The presented turn-on, Eon, and turn-off, Eoff, energies per pulse are calculated under the switching conditions 100 A/cm2 and 600 V with a gate resistance of Rg=1 . For the two N-on designs the total switching losses, Esw=Eon+Eoff, differ less than 30% with Wch 0.7 m. With Wch=0.5 m the switching losses of N-off design are almost one order of magnitude higher than those of the N-on design with Vth = -50 V.


Sign in / Sign up

Export Citation Format

Share Document