Bulk Mosfet
Bulk buy mosfet online from Chinese suppliers on dhgate.com. Get deals with coupon and discount code! Source high quality products in hundreds of categories wholesale direct from China. . n-channel device (n-MOSFET) on p-substrate – uses electron inversion layer. p-channel device (p-MOSFET) on n-Si substrate – uses hole inversion layer n+ n+ p Bulk or Body Drain Source Gate (a) n-channel MOSFET D− G −I Dp B p+ p+ n Bulk or Body Drain Gate (b) p-channel MOSFET Source + V SG D S− G + + V GS I Dn B V SD 0 V.
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- The bulk MOSFETs have a capacitance equivalent thickness (CET) of 1.8 nm and have been fabricated with identical back-end processes. The gate-to-channel capacitance is 19 fF/.
Универсальный англо-русский словарь. Академик.ру. 2011.
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Mosfet Bulk Effect
- Nanoscale CMOS. Innovative Materials, Modeling and Characterization, Francis Balestra. This book provides a comprehensive review of the state-of-the-art in the development of new and innovative materials, and of advanced modeling and characterization methods for nanoscale CMOS… ПодробнееКупить за 21150.85 рубэлектронная книга
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4 IEEE TRANSACTIONS ON ELECTRON DEVICES
IEEE | ||
Fig. 6. | Proof | |
Comparison of (a) transverse stress profiles and (b) STI stress-induced hole mobility variations for planar versus trigate (WSTRIPE = 20 nm) bulk | ||
MOSFETs using Taurus 3-D [11]. The silicon stripe height is 10 nm for the trigate bulk MOSFETs, which provides for more uniform channel mobility because | ||
of reduced STI-induced channel stress. | ||
Fig. 7. | CESL-induced stress distribution in planar and trigate bulk MOSFETs. The CESL is assumed to be a 30-nm-thick silicon nitride with 2-GPa tensile |
stress. LG = 20 nm, tox = 9 Å, gate electrode thickness (TGATE) = 40 nm, spacer width (LSPACER) = 20 nm, WSTRIPE = 20 nm, WSPACING = 20, and HSTRIPE = 10 nm.
132IV. IMPACT OF RANDOM VARIATIONS
133Here, LERand RDF-induced variations are compared for
134the three MOSFET structures. Gate LER profiles are sampled
135from a scanning electron micrograph of extreme ultraviolet
136resist lines. On average, these lines have an LER (3σ) value
of 4 nm and a line width roughness (LWR) value of 6.4 nm. 137 The distance between the consecutive sampling points of the 138 LER profiles is approximately 0.8 nm. Examples of simulated 139 structures with different gate LER profiles are shown in Fig. 8. 140 The source and drain junction profiles are assumed to have 141
SUN et al.: STUDY OF PLANAR MOSFET, SOI FinFET, AND TRIGATE MOSFET DESIGNS | 5 |
Fig. 10. LERand RDFinduced variations in trigate bulk MOSFET, SOI
Fig. 8. Examples of simulated gate electrodes with different LER profiles. | FinFET, and planar bulk MOSFET. | LG = 20 nm, and tSi = 0.6 LG = |
12 nm. |
IEEE | ||||
Fig. 9. LER-induced variation in trigate bulk MOSFET, SOI FinFET, and | ||||
planar bulk MOSFET. LG = 20 nm, and tSi = 0.6 LG = 12 nm. | ||||
142 the same LER as the gate electrode to simulate the worst case | ||||
143 scenario; thus, Le will have the same roughness profile as | ||||
144 | LG. The RDF profiles are generated using kinetic Monte Carlo | |||
145 simulations [9] on the MOSFET structures with gate LER. | ||||
146 | Three-dimensional device simulations are performed for the | |||
147 optimized nominal designs to investigate the effects of LER | ||||
148 only and also to investigate the effects of LER, together with | ||||
149 | RDF, in the source/drain and channel regions. | |||
150 | Fig. 9 shows the gate LER-induced VT variations (σVT ) | |||
151 for the SOI FinFET, planar bulk MOSFET, and trigate bulk | ||||
152 | MOSFET with tSi = 0.6 LG. The variation is smallest for the | |||
153 trigate bulk MOSFET design due to its superior electrostatic | ||||
154 integrity. The SOI FinFET has VT variation comparable to that | ||||
155 of the planar bulk MOSFET. This is because the two sidewall | ||||
156 gates of the FinFET have discrete different gate lengths due to | Fig. 11. Effect of tSi on LERand RDFinduced variations. LG = 20 nm. | |||
157 | gate LWR, whereas the effects of gate LWR on planar bulk | |||
158 | MOSFETs are somewhat averaged across the channel width. | (a) tSi = 0.6 LG = 12 nm. (b) tSi = 0.8 LG = 16 nm. | ||
159 | VT variations due to the presence of both LER and RDF are | |||
160 shown in Fig. 10. VT lowering (where | VT is equal to the | gradient regions increases with smaller WSTRIPE [12] and 167 | ||
161 | VT value of the nominal design subtracted by the mean VT | also because of larger LER-induced variation, the SOI FinFET 168 | ||
162 value of the MOSFET structures with gate LER and RDF) | does not provide for reduced random variation, as compared 169 | |||
163 is smallest for the trigate bulk MOSFET due to its superior | with the trigate bulk MOSFET design, although there are no 170 | |||
164 electrostatic integrity. Overall, the trigate bulk MOSFET also | channel dopants in the SOI FinFET. Fig. 11 shows the effect 171 | |||
165 shows comparable random VT | variation as the SOI FinFET. | of tSi on the random variation. For the trigate bulk MOSFET, 172 | ||
Download cinterion wireless modules port devices driver. 166 | Because VT variation induced | by RDF | in the source/drain | tSi = 0.6 LG yields the smallest random variation, whereas 173 |
6
174 for the planar bulk MOSFET, tSi = 0.8 LG is beneficial for 175 reduced RDF-induced variability since the average number of 176 channel dopants is smaller.
177 | V. CONCLUSION |
178The impact of process-induced systematic and random vari-
179ations on transistor performance has been investigated for three
Bulk Mosfet Cable
180different transistor structures. As compared with the planar bulk
181MOSFET and SOI FinFET, the trigate bulk MOSFET design
182shows the least variability and the best nominal performance.
183Thus, it is a promising device architecture for transistor scaling
184to the end of the technology roadmap.
IEEE TRANSACTIONS ON ELECTRON DEVICES
[7] X. Sun and T.-J. King Liu, “Scale length assessment of the tri-gate 206 bulk MOSFET design,” IEEE Trans. Electron Devices, vol. 56, no. 11, 207
pp. 2840–2842, Nov. 2009. | 208 |
[8] A. Hokazono, H. Itokawa, N. Kusunoki, I. Mizushima, | S. Inaba, 209 |
S. Kawanaka, and Y. Toyoshima, “Steep channel & halo profiles utilizing 210 boron-diffusion-barrier layers (Si:C) for 32 nm node and beyond,” in VLSI 211
Symp. Tech. Dig., 2008, pp. 112–113. | 212 |
[9] Synopsys, Inc., Mountain View, CA, Sentaurus User’s Manual, 2009.06, 213 2009. 214
[10]G. Scott, J. Lutze, M. Rubin, F. Nouri, and M. Manley, “NMOS drive 215 current reduction caused by transistor layout and trench isolation induced 216
stress,” in IEDM Tech. Dig., 1999, pp. 827–830. | 217 | |
[11] Taurus User’s Manual, Synopsys, Inc., Mountain View, CA. | 218 | AQ1 |
[12]V. Varadarajan, L. Smith, S. Balasubramanian, and T.-J. King Liu, “Multi219 gate FET design for tolerance to statistical dopant fluctuations,” in 220
Proc. IEEE Silicon Nanoelectron. Workshop, 2006, pp. 137–138. | 221 |
185 | REFERENCES | Xin Sun, photograph and biography not available at the time of publication. 222 |
Mosfet Bulk Current
186[1] H. Masuda, S. Ohkawa, A. Kurokawa, and M. Aoki, “Challenge:
187Variability characterization and modeling for 65to 90-nm process,” in
188 | Proc. Custom Integr. Circuits Conf., 2005, pp. 593–599. | Victor Moroz, photograph and biography not available | Capture one 20 free crack for mac. at the time of 223 | ||
189 | [2] | A. Asenov, A. R. Brown, J. H. Davies, S. Kaya, and G. Slavcheva, | |||
publication. | 224 | ||||
190 | IEEE | ||||
“Simulation of intrinsic parameter fluctuations in decananometer and | |||||
191 | nanometer-scale MOSFETs,” IEEE Trans. Electron Devices, vol. 50, | ||||
192 | no. 9, pp. 1837–1852, Sep. 2003. | ||||
193 | [3] R.-H. Yan, A. Ourmazd, and K. F. Lee, “Scaling the Si MOSFET: From | Nattapol Damrongplasit, photograph and biography not available at the time 225 | |||
194 | bulk to SOI to bulk,” IEEE Trans. Electron Devices, vol. 39, no. 7, | of publication. | 226 | ||
195 | pp. 1704–1710, Jul. 1992. | ||||
196 | [4] K. Suzuki, T. Tanaka, Y. Tosaka, H. Horie, and Y. Arimoto, “Scaling | ||||
197 | theory for double-gate SOI MOSFETs,” IEEE Trans. Electron Devices, | ||||
198 | vol. 40, no. 12, pp. 2326–2329, Dec. 1993. | Changhwan Shin, photograph and biography not available at the time of 227 | |||
199 | [5] | D. J. Frank, Y. Taur, and H.-S. P. Wong, “Generalized scale length for | |||
Proof | |||||
200 | two-dimensional effects in MOSFETs,” IEEE Electron Device Lett., | publication. | 228 | ||
201 | vol. 19, no. 10, pp. 385–387, Oct. 1998. | ||||
202 | [6] | X. Sun, Q. Lu, V. Moroz, H. Takeuchi, G. Gebara, J. Wetzel, S. Ikeda, | |||
203 | C. Shin, and T.-J. King Liu, “Tri-gate bulk MOSFET design for CMOS | Tsu-Jae King Liu, photograph and biography not available at the time of 229 | |||
204 | scaling to the end of the roadmap,” IEEE Electron Device Lett., vol. 29, | ||||
205 | no. 5, pp. 491–493, May 2008. | publication. | 230 |
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