Analysis of transit times and minority carrier mobility in n-p-n 4H-SiC bipolar junction transistors

An analysis of the transit times and minority carrier mobility in n-p-n 4H-SiC RF bipolar junction transistors is presented. These parameters were extracted from small signal RF measurements on 4H-SiC RF transistors with three different base thicknesses: 100, 140, and 200 nm. The study shows that the room temperature minority carrier electron mobility is 215 cm/sup 2//V/spl middot/s for a base Al doping of N/sub B/=4/spl times/10/sup 18/ cm/sup -3/. The analysis reveals that the collector charging time /spl tau//sub C/ and the parasitic charging time /spl tau//sub P/ from the capacitance between metal pads and the underlying collector region have a significant effect on the transistors RF performance. The calculated RF gain is in good agreement with the measured results.     

Low-voltage high performance compact all cascode CMOS current mirror

A high performance and compact current mirror with extremely low input and high output resistances (R/sub in//spl sim/0.01/spl Omega/, R/sub out//spl sim/10 G/spl Omega/), high copying accuracy, very low input and output voltage requirements (V/sub in/, V/sub out//spl ges/V/sub DSsat/), high bandwidth (200 MHz using a 0.5 /spl mu/m CMOS technology) and low settling time (25 ns) is proposed. Simulations and experimental results are shown that validate the circuit.     

High-speed silicon electrooptic Modulator design

An electrically driven Mach-Zehnder waveguide modulator based on high-index contrast silicon split-ridge waveguide technology and electronic carrier injection is proposed. The excellent optical and carrier confinement possible in high-index contrast waveguide devices, together with good thermal heat sinking and forward biased operation, enables high-speed modulation with small signal modulation bandwidths beyond 20 GHz, a V/sub /spl pi// times length figure of merit of V/sub /spl pi//L=0.5 V/spl middot/cm and an insertion loss of about 4 dB. The modulator can be fabricated in a complementary metal-oxide-semiconductor compatible way.     

Channel width dependence of NMOSFET hot carrier degradation

The channel width dependence of hot carrier reliability on NMOSFETs from 0.4-/spl mu/m to 0.13-/spl mu/m technology has been studied at both I/sub b,peak/ and V/sub g/ = V/sub d/ conditions. Enhanced degradation on narrow width devices happens on most technologies. The I/sub b//I/sub d/ value and vertical electric field are proposed to be the reasons for enhanced degradation on narrow width NMOSFETs.     

High-performance nonhydrogenated nickel-induced laterally crystallized P-channel poly-Si TFTs

High-performance nickel-induced laterally crystallized (NILC) p-channel poly-Si thin-film transistors (TFTs) have been fabricated without hydrogenation. Two different thickness of Ni seed layers are selected to make high-performance p-type TFTs. A very thin seed layer (e.g., 5 /spl Aring/) leads to marginally better performance in terms of transconductance (Gm) and threshold voltage (V/sub th/) than the case of a 60 /spl Aring/ Ni seed layer. However, the p-type poly-Si TFTs crystallized by the very thin Ni seeding result in more variation in both V/sub th/ and G/sub m/ from transistor to transistor. It is believed that differences in the number of laterally grown polycrystalline grains along the channel cause the variation seen between 5 /spl Aring/ NILC TFTs compared to 60-/spl Aring/ NILC TFTs. The 60 /spl Aring/ NILC nonhydrogenated TFTs show consistent high performance, i.e., typical electrical characteristics have a linear field-effect hole mobility of 156 cm/sup 2//V-S, subthreshold swing of 0.16 V/dec, V/sub th/ of -2.2 V, on-off ratio of >10/sup 8/, and off-current of <1/spl times/10/sup -14/ A//spl mu/m when V/sub d/ equals -0.1 V.     

Highly reliable CVD-WSi metal gate electrode for nMOSFETs

In this paper, we first propose an improved chemical vapor deposition (CVD) WSi/sub x/ metal gate suitable for use in nMOSFETs. We studied the relationship between the Si/W ratio of CVD-WSi/sub x/ film and electrical properties of MOSFETs. As a result, it was found that the Si/W ratio strongly affects carrier mobility and the reliability of gate oxide. In the case of higher Si/W ratio, both electron and hole mobility can be improved. For CVD-WSi/sub 3.9/ electrode, electron mobility and hole mobility at 1.2 V of |V/sub g/-V/sub th/| are 331 and 78 cm/sup 2//V/spl middot/s, respectively. These values are almost the same as those for n/sup +/-poly-Si electrode. The improvement of carrier mobility by controlling the Si/W ratio is due to suppression of fluorine contamination in gate oxide. F contamination at the Si/W ratio of 3.9 is found to be less than that at the Si/W ratio of 2.4 from XPS analysis. Workfunction of CVD-WSi/sub 3.9/ gate estimated from C-V measurements is 4.3 eV. In CVD-WSi/sub 3.9/ gate MOSFETs with gate length of 50 nm, a drive current of 636 /spl mu/A//spl mu/m was achieved for off-state leakage current of 35 nA//spl mu/m at power supply voltage of 1.0 V. By using CVD-WSi/sub 3.9/ gate electrode, highly reliable metal gate nMOSFETs can be realized.     

Electrical characteristics of 8-/spl Aring/ EOT HfO/sub 2//TaN low thermal-budget n-channel FETs with solid-phase epitaxially regrown junctions

The authors demonstrate high-performing n-channel transistors with a HfO/sub 2//TaN gate stack and a low thermal-budget process using solid-phase epitaxial regrowth of the source and drain junctions. The thinnest devices have an equivalent oxide thickness (EOT) of 8 /spl Aring/, a leakage current of 1.5 A/cm/sup 2/ at V/sub G/=1 V, a peak mobility of 190 cm/sup 2//V/spl middot/s, and a drive-current of 815 /spl mu/A//spl mu/m at an off-state current of 0.1 /spl mu/A//spl mu/m for V/sub DD/=1.2 V. Identical gate stacks processed with a 1000-/spl deg/C spike anneal have a higher peak mobility at 275 cm/sup 2//V/spl middot/s, but a 5-/spl Aring/ higher EOT and a reduced drive current at 610 /spl mu/A//spl mu/m. The observed performance improvement for the low thermal-budget devices is shown to be mostly related to the lower EOT. The time-to-breakdown measurements indicate a maximum operating voltage of 1.6 V (1.2 V at 125 /spl deg/C) for a ten-year lifetime, whereas positive-bias temperature-instability measurements indicate a sufficient lifetime for operating voltages below 0.75 V.     

Identifying and locating-dominating codes: NP-completeness results for directed graphs

Let G=(V, A) be a directed, asymmetric graph and C a subset of vertices, and let B/sub r//sup -/(v) denote the set of all vertices x such that there exists a directed path from x to v with at most r arcs. If the sets B/sub r//sup -/(v) /spl cap/ C, v /spl isin/ V (respectively, v /spl isin/ V/spl bsol/C), are all nonempty and different, we call C an r-identifying code (respectively, an r-locating-dominating code) of G. In other words, if C is an r-identifying code, then one can uniquely identify a vertex v /spl isin/ V only by knowing which codewords belong to B/sub r//sup -/(v), and if C is r-locating-dominating, the same is true for the vertices v in V/spl bsol/C. We prove that, given a directed, asymmetric graph G and an integer k, the decision problem of the existence of an r-identifying code, or of an r-locating-dominating code, of size at most k in G, is NP-complete for any r/spl ges/1 and remains so even when restricted to strongly connected, directed, asymmetric, bipartite graphs or to directed, asymmetric, bipartite graphs without directed cycles.     

SODEL FET: novel channel and source/drain profile engineering schemes by selective Si epitaxial growth technology

In this paper, novel channel and source/drain profile engineering schemes are proposed for sub-50-nm bulk CMOS applications. This device, referred to as the silicon-on-depletion layer FET (SODEL FET), has the depletion layer beneath the channel region, which works as an insulator like a buried oxide in a silicon-on-insulator MOSFET. Thanks to this channel structure, junction capacitance (C/sub j/) has been reduced in SODEL FET, i.e., C/sub j/ (area) was /spl sim/0.73 fF//spl mu/m/sup 2/ both in SODEL nFET and pFET at Vbias =0.0 V. The body effect coefficient /spl gamma/ is also reduced to less than 0.02 V/sup 1/2/. Nevertheless, current drives of 886 /spl mu/A//spl mu/m (I/sub off/=15 nA//spl mu/m) in nFET and -320 /spl mu/A//spl mu/m (I/sub off/=10 nA//spl mu/m) in pFET have been achieved in 70-nm gate length SODEL CMOS with |V/sub dd/|=1.2 V. New circuit design schemes are also proposed for high-performance and low-power CMOS applications using the combination of SODEL FETs and bulk FETs on the same chip for 90-nm-node generation and beyond.     

1330 V, 67 m/spl Omega//spl middot/cm/sup 2/ 4H-SiC(0001) RESURF MOSFET

Design and fabrication of 4H-SiC(0001) lateral MOSFETs with a two-zone reduced surface field structure have been investigated. The dose dependencies of experimental breakdown voltage show good agreement with simulation. Through the optimization of implant dose, high-temperature (1700/spl deg/C) annealing after ion implantation, and reduction of channel length, a breakdown voltage of 1330 V and a low on-resistance of 67 m/spl Omega//spl middot/cm/sup 2/ have been obtained. The figure-of-merit (V/sub B//sup 2//R/sub on/) of the present device reaches 26 MW/cm/sup 2/, being the best performance among lateral MOSFETs reported. The temperature dependence of static characteristics is also presented.     

Fully depleted dual-gated thin-film SOI P-MOSFETs fabricated in SOI islands with an isolated buried polysilicon backgate

P-channel dual-gated thin-film silicon-on-insulator (DG-TFSOI) MOSFETs have been fabricated with an isolated buried polysilicon backgate in an SOI island formed by epitaxial lateral overgrowth (ELO) of silicon. This structure allows individual operation of both the top and back gates rather than the conventional common backgate structure. When fully-depleted, the buried gate is used to individually shift the top gate threshold voltage (V/sub T/). A linear shift of /spl Delta/V/sub T,top///spl Delta/V/sub G,back/ of 0.5 V/V was achieved with a thin buried oxide. The effective density of interface traps (D/sub it/) for the backgate polysilicon-oxide SOI interface was measured to be 1.8/spl times/10/sup 11/ #/cm/sup 2//spl middot/eV as compared to the substrate-oxide of 1.1/spl times/10/sup 11/ #/cm/sup 2//spl middot/eV.     

Investigation of breakdown and DC behavior in HBTs with (Al,Ga)As collector layer

We report on the realization of an InGaP-GaAs-based double heterojunction bipolar transistor with high breakdown voltages of up to 85 V using an Al/sub 0.2/Ga/sub 0.8/As collector. These results were achieved with devices with a 2.8 /spl mu/m collector doped to 6/spl times/10/sup 15/ cm/sup -3/ (with an emitter area of 60/spl times/60 /spl mu/m/sup 2/). They agree well with calculated data from a semi-analytical breakdown model. A /spl beta//R/sub SBI/ (intrinsic base sheet resistance) ratio of more than 0.5 by introducing a 150-nm-thick graded Al-content region at the base-collector heterojunction was achieved. This layer is needed to efficiently suppress current blocking, which is otherwise caused by the conduction band offset from GaAs to Al/sub 0.2/Ga/sub 0.8/As. The thickness of this region was determined by two-dimensional numerical device simulations that are in good agreement with the measured device properties.     

A CMOS voltage reference based on weighted /spl Delta/V/sub GS/ for CMOS low-dropout linear regulators

A CMOS voltage reference, which is based on the weighted difference of the gate-source voltages of an NMOST and a PMOST operating in saturation region, is presented. The voltage reference is designed for CMOS low-dropout linear regulators and has been implemented in a standard 0.6-/spl mu/m CMOS technology (V/sub thn//spl ap/|V/sub thp/|/spl ap/0.9 V at 0/spl deg/C). The occupied chip area is 0.055 mm/sup 2/. The minimum supply voltage is 1.4 V, and the maximum supply current is 9.7 /spl mu/A. A typical mean uncalibrated temperature coefficient of 36.9 ppm//spl deg/C is achieved, and the typical mean line regulation is /spl plusmn/0.083%/V. The power-supply rejection ratio without any filtering capacitor at 100 Hz and 10 MHz are -47 and -20 dB, respectively. Moreover, the measured noise density with a 100-nF filtering capacitor at 100 Hz is 152 nV//spl radic/(Hz) and that at 100 kHz is 1.6 nV//spl radic/(Hz).     

InGaAs-InP mesa DHBTs with simultaneously high f/sub /spl tau// and f/sub max/ and low C/sub cb//I/sub c/ ratio

We report an InP-InGaAs-InP double heterojunction bipolar transistor (DHBT), fabricated using a conventional triple mesa structure, exhibiting a 370-GHz f/sub /spl tau// and 459-GHz f/sub max/, which is to our knowledge the highest f/sub /spl tau// reported for a mesa InP DHBT-as well as the highest simultaneous f/sub /spl tau// and f/sub max/ for any mesa HBT. The collector semiconductor was undercut to reduce the base-collector capacitance, producing a C/sub cb//I/sub c/ ratio of 0.28 ps/V at V/sub cb/=0.5 V. The V/sub BR,CEO/ is 5.6 V and the devices fail thermally only at >18 mW//spl mu/m/sup 2/, allowing dc bias from J/sub e/=4.8 mA//spl mu/m/sup 2/ at V/sub ce/=3.9 V to J/sub e/=12.5 mA//spl mu/m/sup 2/ at V/sub ce/=1.5 V. The device employs a 30 nm carbon-doped InGaAs base with graded base doping, and an InGaAs-InAlAs superlattice grade in the base-collector junction that contributes to a total depleted collector thickness of 150 nm.     

Internal efficiency of semiconductor lasers with a quantum-confined active region

We discuss in detail a new mechanism of nonlinearity of the light-current characteristic (LCC) in heterostructure lasers with reduced-dimensionality active regions, such as quantum wells (QWs), quantum wires (QWRs), and quantum dots (QDs). It arises from: 1) noninstantaneous carrier capture into the quantum-confined active region and 2) nonlinear (in the carrier density) recombination rate outside the active region. Because of 1), the carrier density outside the active region rises with injection current, even above threshold, and because of 2), the useful fraction of current (that ends up as output light) decreases. We derive a universal closed-form expression for the internal differential quantum efficiency /spl eta//sub int/ that holds true for QD, QWR, and QW lasers. This expression directly relates the power and threshold characteristics. The key parameter, controlling /spl eta//sub int/ and limiting both the output power and the LCC linearity, is the ratio of the threshold values of the recombination current outside the active region to the carrier capture current into the active region. Analysis of the LCC shape is shown to provide a method for revealing the dominant recombination channel outside the active region. A critical dependence of the power characteristics on the laser structure parameters is revealed. While the new mechanism and our formal expressions describing it are universal, we illustrate it by detailed exemplary calculations specific to QD lasers. These calculations suggest a clear path for improvement of their power characteristics. In properly optimized QD lasers, the LCC is linear and the internal quantum efficiency is close to unity up to very high injection-current densities (15 kA/cm/sup 2/). Output powers in excess of 10 W at /spl eta//sub int/ higher than 95% are shown to be attainable in broad-area devices. Our results indicate that QD lasers may possess an advantage for high-power applications.     

High-temperature thermal stability performance in /spl delta/-doped In/sub 0.425/Al/sub 0.575/As--In/sub 0.65/Ga/sub 0.35/As metamorphic HEMT

We report, to our knowledge, the best high-temperature characteristics and thermal stability of a novel /spl delta/-doped In/sub 0.425/Al/sub 0.575/As--In/sub 0.65/Ga/sub 0.35/As--GaAs metamorphic high-electron mobility transistor. High-temperature device characteristics, including extrinsic transconductance (g/sub m/), drain saturation current density (I/sub DSS/), on/off-state breakdown voltages (BV/sub on//BV/sub GD/), turn-on voltage (V/sub on/), and the gate-voltage swing have been extensively investigated for the gate dimensions of 0.65/spl times/200 /spl mu/m/sup 2/. The cutoff frequency (f/sub T/) and maximum oscillation frequency (f/sub max/), at 300 K, are 55.4 and 77.5 GHz at V/sub DS/=2 V, respectively. Moreover, the distinguished positive thermal threshold coefficient (/spl part/V/sub th///spl part/T) is superiorly as low as to 0.45 mV/K.     

BV/sub CEO/--BV/sub CBO/ separation and sharpness of breakdown in high-speed bipolar transistors

The effect of secondary impact ionization by the noninitiating carrier on the near avalanche behavior of high-speed n-p-n bipolar transistors is studied. We show that secondary collector ionization by generated holes traveling back toward the base layer significantly reduces BV/sub CBO/ if the hole ionization coefficient is higher than that of electrons [/spl beta//sub p/(E)>/spl alpha//sub n/(E)]: positive feedback associated with a strong secondary ionization sharpens the breakdown characteristic by speeding up carrier multiplication and decreases separation between the open-base collector-emitter (BV/sub CEO/) and the open-emitter base-collector (BV/sub CBO/) breakdown voltages. The effect of secondary ionization on the BV/sub CEO/-BV/sub CBO/ separation has not previously been described. Multiplication coefficient comparisons for representative InP, GaAs, and Si collectors indicate all structures can sustain low-current above BV/sub CEO/ operation from a transport (nonthermal) point of view, although the different degrees of secondary ionization in various semiconductors lead to fundamental differences when InP is compared to GaAs and Si since for the latter materials /spl beta//sub p/(E)相似文献   

InGaAs/InP DHBTs with 120-nm collector having simultaneously high f/sub /spl tau//, f/sub max//spl ges/450 GHz

InP/In/sub 0.53/Ga/sub 0.47/As/InP double heterojunction bipolar transistors (DHBT) have been designed for increased bandwidth digital and analog circuits, and fabricated using a conventional mesa structure. These devices exhibit a maximum 450 GHz f/sub /spl tau// and 490 GHz f/sub max/, which is the highest simultaneous f/sub /spl tau// and f/sub max/ for any HBT. The devices have been scaled vertically for reduced electron collector transit time and aggressively scaled laterally to minimize the base-collector capacitance associated with thinner collectors. The dc current gain /spl beta/ is /spl ap/ 40 and V/sub BR,CEO/=3.9 V. The devices operate up to 25 mW//spl mu/m/sup 2/ dissipation (failing at J/sub e/=10 mA//spl mu/m/sup 2/, V/sub ce/=2.5 V, /spl Delta/T/sub failure/=301 K) and there is no evidence of current blocking up to J/sub e//spl ges/12 mA//spl mu/m/sup 2/ at V/sub ce/=2.0 V from the base-collector grade. The devices reported here employ a 30-nm highly doped InGaAs base, and a 120-nm collector containing an InGaAs/InAlAs superlattice grade at the base-collector junction.     

III-nitride-based planar lightwave circuits for long wavelength optical communications

Planar lightwave circuits based on III-nitride wide-bandgap semiconductors are proposed and the feasibility of developing III-nitride-based novel photonic integrated circuits for applications in fiber-optical communications is discussed. III-nitrides have low attenuation in the near-infrared wavelength region because of their wide bandgaps, while as semiconductors their refractive indexes can be modulated by carrier injection. III-nitrides are also well known for their ability to operate at high temperatures, high power levels and in harsh environments. These characteristics make III-nitrides ideal candidates for tunable optical phased-array (PHASAR) devices for optical communications. We have characterized the optical properties of Al/sub x/Ga/sub 1-x/N epilayers in the 1550-nm wavelength region, including the refractive indexes and the impact of Al concentrations. Single-mode ridged optical waveguide devices using GaN-AlGaN heterostructures have been designed, fabricated and characterized for operation in the 1550-nm wavelength window. The birefringence of wurtzite GaN grown on sapphire substrate has been observed. Refractive indexes were found to be different for signal optical field perpendicular and parallel to the crystal c axis (n/sub /spl perp// /spl ne/ n/sub ///). More importantly, we found an approximately 10% change in the index difference /spl Delta/n=n/sub ///-n/sub /spl perp// with varying the waveguide orientation within the c plane, and a 60/spl deg/ periodicity was clearly observed. This is attributed to the hexagonal structure of the nitride materials. Various functional waveguide devices have been realized, including 2/spl times/2 directional couplers and eight-wavelength array-waveguide gratings. Theoretical predictions of temperature sensitivity and the efficiency of carrier-induced refractive change are provided.