2103 - 2107 |
Calculation of lattice heating in SiC RF power devices Bertilsson K, Harris C, Nilsson HE |
2109 - 2114 |
A comprehensive geometrical and biasing analysis for latchup in 0.18-mu m COSi2STI CMOS structure Goh WL, Yeo KS |
2115 - 2124 |
Capacitance analysis of devices with electrically floating regions Yamaguchi K, Horiuchi M |
2125 - 2131 |
A compact deep-submicron MOSFET g(ds) model including hot-electron and thermoelectric effects Zhou X, Chiah SB, Lim KY |
2133 - 2145 |
A sum-over-paths impulse-response moment-extraction algorithm for RC IC-interconnect networks Le Coz YL, Krishna D, Petranovic DM, Loh WM, Bendix P |
2147 - 2151 |
Field emission of vertically-aligned carbon nanotube arrays grown on porous silicon substrate Li JT, Lei W, Zhang XB, Wang BP, Ba L |
2153 - 2157 |
Predictive model of a reduced surface field p-LDMOSFET using neural network Kim B, Kim S, Lee DW, Roh TM, Kim J |
2159 - 2163 |
Impulse responses of submicron GaAs photodetectors Ohno T, Ishibashi K, Aoyagi Y, Aida Y |
2165 - 2173 |
Effects of generation/recombination processes and leakage current through interfacial "punctures" on electrical characterization of unipolar directly bonded semiconductor structures Stuchinsky VA |
2175 - 2179 |
Influence of annealing ambient on GaAs oxide prepared by the liquid phase method Chou DW, Wang LT, Wang HH, Sze PW, Wang YH, Houng MP |
2181 - 2189 |
Dynamic surface temperature measurements in SiC epitaxial power diodes performed under single-pulse self-heating conditions Hillkirk LM |
2191 - 2198 |
Influences of nonuniformity in metal concentration in gate dielectric silicate on CMIS inverters' propagation delay time Ono M, Ino T, Koyama M, Takashima A, Nishiyama A |
2199 - 2206 |
Analytical model for the programming of source side injection SST superflash split-gate cell using two-dimensional analysis Guan HN, Lee D, Li GP |
2207 - 2211 |
Analysis and optimisation of the trench gated emitter switched thyristor Spulber O, Sweet M, Vershinin K, Luther-King N, De Souza MM, Narayanan EMS |
2213 - 2217 |
High resolution transport spectroscopy in ultimate MOSFETs at very low temperature Sanquer M, Jehl X, Specht M, Bertrand G, Guegan G, Deleonibus S |
2219 - 2223 |
Optoelectronic properties of Zn0.52Se0.4/Si Schottky diodes Venkatachalam S, Kumar RTR, Mangalaraj D, Narayandass SK, Kim K, Yi JS |
2225 - 2234 |
Integral function method for determination of nonlinear harmonic distortion Cerdeira A, Aleman MA, Estrada M, Flandre D |
2235 - 2241 |
Electrical properties of high permittivity ZrO2 gate dielectrics on strained-Si Maiti CK, Dalapati GK, Chatterjee S, Samanta SK, Varma S, Patil S |
2243 - 2249 |
Quarter micron BiCMOS technology platform with implanted-base- or SiGe-bipolar transistor for wireless communication ICs Tilke AT, Rothenhausser S, Rochel M, Stahrenberg K, Goller K, Junge A, Pribil A, Foste B, Wiedemann J, Tegeler M, Berkner J, Wagner C, Dahl C |
2251 - 2254 |
100 angstrom-thick tunnel junction by double impurity doping liquid phase epitaxy for V-band TUNNETT oscillation Nishizawa J, Murai A, Makabe H, Ito O, Kimura T, Suto K, Oyama Y |
2255 - 2262 |
Drain current thermal noise modeling for deep submicron n- and p-channel MOSFETs Han K, Shin H, Lee K |
2263 - 2270 |
LDMOS in SOI technology with very-thin silicon film Bawedin M, Renaux C, Flandre D |
2271 - 2275 |
Low-frequency noise in Si0.7Ge0.3 surface channel pMOSFETs with ALD HfO2/Al2O3 gate dielectrics von Haartman M, Wu D, Malm BG, Hellstrom PE, Zhang SL, Ostling M |
2277 - 2280 |
Differential capacitance as a method of determining the presence of a quasi-bidimensional electronic gas Martinez-Orozco JC, Gaggero-Sager LM, Vlaev SJ |
2281 - 2286 |
Complementary tunneling transistor for low power application Wang PF, Hilsenbeck K, Nirschl T, Oswald M, Stepper C, Weis M, Schmitt-Landsiedel D, Hansch W |
2287 - 2291 |
Preparation and electrical properties of SrTiO3 ceramics doped with M2O3-PbO-CuO Zhao JC, Wu XH, Li LT, Li X |
2293 - 2297 |
Promotion of piezoelectric properties of lead zirconate titanate ceramics with (Zr,Ti) partially replaced by Nb2O5 Chen BH, Huang CL, Wu L |
2299 - 2306 |
Hole mobility enhancement and Si cap optimization in nanoscale strained Si1-xGexPMOSFETs Shi ZH, Onsongo D, Rai R, Samavedam SB, Banerjee SK |
2307 - 2313 |
Electrical simulation of the flicker in poly-Si TFT-LCD pixels for the large-area and high-quality TFT-LCD development and manufacturing Son MS, Yoo KH, Jang J |
2315 - 2319 |
Characterization of double gate MOSFETs fabricated by a simple method on a recrystallized silicon film Lin XN, Feng CG, Zhang SD, Ho WH, Chan MS |
2321 - 2327 |
A closed-form expression to analyze electronic properties in delta-doped heterostructures Chen XY, Nabet B |
2329 - 2334 |
Simulation of submicrometer metal-semiconductor-metal ultraviolet photodiodes on gallium nitride Li J, Donaldson WR, Hsiang TY |
2335 - 2338 |
The SILC study by PDO method Wang Z, Zhang HQ, Xu MZ, Tan CH |
2339 - 2342 |
Determining the generation lifetime in a MOS capacitor using linear sweep techniques Tapajna M, Harmatha L |
2343 - 2346 |
Fabrication of ZnO-based metal-insulator-semiconductor diodes by ion implantation Alivov YI, Look DC, Ataev BM, Chukichev MV, Mamedov VV, Zinenko VI, Agafonov YA, Pustovit AN |
2347 - 2349 |
Comment on "Negative Schottky barrier between titanium and n-type Si(001) for low-resistance ohmic contacts Osvald J |
2351 - 2352 |
Response to "Comment on'Negative Schottky barrier between titanium and n-type Si(001) for low-resistance ohmic contacts" [Solid State Electron. 2004;48 : 335-8] Tao M, Zhu J |