High-Performance 0.1-$muhbox{m}$ Gate AlGaN/GaN HEMTs on Silicon With Low-Noise Figure at 20 GHz

The realization of high-performance 0.1-$muhbox{m}$ gate AlGaN/GaN high-electron mobility transistors (HEMTs) grown on high-resistivity silicon substrates is reported. Our devices feature cutoff frequencies as high as $f_{T} = hbox{75} hbox{GHz}$ and $f_{rm MAX} = hbox{125} hbox{GHz}$, the highest values reported so far for AlGaN/GaN HEMTs on silicon. The microwave noise performance is competitive with results achieved on other substrate types, such as sapphire and silicon carbide, with a noise figure $F = hbox{1.2}{-}hbox{1.3} hbox{dB}$ and an associated gain $G_{rm ass} = hbox{8.0}{-}hbox{9.5} hbox{dB}$ at 20 GHz. This performance demonstrates that GaN-on-silicon technology is a viable alternative for low-cost millimeter-wave applications.      

High Microwave-Noise Performance of AlGaN/GaN MISHEMTs on Silicon With Gate Insulator Grown by ALD

High microwave-noise performance is realized in AlGaN/GaN metal–insulator semiconductor high-electron mobility transistors (MISHEMTs) on high-resistivity silicon substrate using atomic-layer-deposited (ALD) $hbox{Al}_{2}hbox{O}_{3}$ as gate insulator. The ALD $hbox{Al}_{2}hbox{O}_{3}/hbox{AlGaN/GaN}$ MISHEMT with a 0.25- $muhbox{m}$ gate length shows excellent microwave small signal and noise performance. A high current-gain cutoff frequency $f_{T}$ of 40 GHz and maximum oscillation frequency $f_{max}$ of 76 GHz were achieved. At 10 GHz, the device exhibits low minimum-noise figure $(hbox{NF}_{min})$ of 1.0 dB together with high associate gain $(G_{a})$ of 10.5 dB and low equivalent noise resistance $(R_{n})$ of 29.2 $Omega$. This is believed to be the first report of a 0.25-$muhbox{m}$ gate-length GaN MISHEMT on silicon with such microwave-noise performance. These results indicate that the AlGaN/GaN MISHEMT with ALD $hbox{Al}_{2}hbox{O}_{3}$ gate insulator on high-resistivity Si substrate is suitable for microwave low-noise applications.      

AlGaN/GaN HEMTs With Low Leakage Current and High On/Off Current Ratio

In this letter, we propose using an oxide-filled isolation structure followed by $hbox{N}_{2}/hbox{H}_{2}$ postgate annealing to reduce the leakage current in AlGaN/GaN HEMTs. An off-state drain leakage current that is smaller than $hbox{10}^{-9} hbox{A/mm}$ (minimum $hbox{5.1} times hbox{10}^{-10} hbox{A/mm}$) can be achieved, and a gate leakage current in the range of $hbox{7.8} times hbox{10}^{-10}$ to $hbox{9.2} times hbox{10}^{-11} hbox{A/mm}$ ($V_{rm GS}$ from $-$10 to 0 V and $V_{rm DS} = hbox{10} hbox{V}$) is obtained. The substantially reduced leakage current results in an excellent on/off current ratio that is up to $hbox{1.5} times hbox{10}^{8}$. An improved flicker noise characteristic is also observed in the oxide-filled devices compared with that in the traditional mesa-isolated GaN HEMTs.      

Operation of Pt/AlGaN/GaN-Heterojunction Field-Effect-Transistor Hydrogen Sensors With Low Detection Limit and High Sensitivity

To enhance the device sensitivity and detection limit, a gate bias is applied to the catalytic metal of AlGaN/GaN-heterojunction field-effect-transistor (HFET) hydrogen sensors to control the carrier concentration in the channel at operation. The sensors exhibit a good sensitivity at temperatures up to 800 $^{circ}hbox{C}$ and a detection limit of 10-ppb $ hbox{H}_{2}$ in $hbox{N}_{2}$. The dependence of the device sensitivity on gate and drain biases has been investigated. The sensitivity peaks at the gate bias of threshold voltage and the drain bias of knee voltage in sensing gas. At high temperatures and $hbox{H}_{2}$ concentrations, specifically from 300 $^{circ}hbox{C}$ and 1000-ppm $hbox{H}_{2}/hbox{N}_{2}$, respectively, the sensitivity of HFETs at $V_{rm gs} = -hbox{3.5} hbox{V}$ and $V_{rm ds} = hbox{1} hbox{V}$ is more than three orders higher than their sensitivity at $V_{rm gs} = hbox{0} hbox{V}$ and the sensitivity of Schottky diodes.      

AlN/GaN Insulated-Gate HEMTs With 2.3 A/mm Output Current and 480 mS/mm Transconductance

High-electron mobility transistors (HEMTs) based on ultrathin AlN/GaN heterostructures with a 3.5-nm AlN barrier and a 3-nm $hbox{Al}_{2}hbox{O}_{3}$ gate dielectric have been investigated. Owing to the optimized AlN/GaN interface, very high carrier mobility $(sim!!hbox{1400} hbox{cm}^{2}/hbox{V}cdothbox{s})$ and high 2-D electron-gas density $(sim!!kern1pthbox{2.7} times hbox{10}^{13} /hbox{cm}^{2})$ resulted in a record low sheet resistance $(sim !!hbox{165} Omega/hbox{sq})$. The resultant HEMTs showed a maximum dc output current density of $simkern1pt$2.3 A/mm and a peak extrinsic transconductance $g_{m,{rm ext}} sim hbox{480} hbox{mS/mm}$ (corresponding to $g_{m,{rm int}} sim hbox{1} hbox{S/mm}$). An $f_{T}/f_{max}$ of 52/60 GHz was measured on $hbox{0.25} times hbox{60} muhbox{m}^{2}$ gate HEMTs. With further improvements of the ohmic contacts, the gate dielectric, and the lowering of the buffer leakage, the presented results suggest that, by using AlN/GaN heterojunctions, it may be possible to push the performance of nitride HEMTs to current, power, and speed levels that are currently unachievable in AlGaN/GaN technology.      

Breakdown Enhancement of AlGaN/GaN HEMTs on 4-in Silicon by Improving the GaN Quality on Thick Buffer Layers

We have achieved a 9- $muhbox{m}$-thick AlGaN/GaN high-electron mobility transistor (HEMT) epilayer on silicon using thick buffer layers with reduced dislocation density $(D_{D})$. The crack-free 9- $muhbox{m}$-thick epilayer included 2- $muhbox{m}$ i-GaN and 7- $ muhbox{m}$ buffer. The HEMTs fabricated on these devices showed a maximum drain–current density of 625 mA/mm, transconductance of 190 mS/mm, and a high three-terminal OFF breakdown of 403 V for device dimensions of $L_{g}/W_{g}/L_{rm gd} = hbox{1.5/15/3} muhbox{m}$ . Without using a gate field plate, this is the highest $BV$ reported on an AlGaN/GaN HEMT on silicon for a short $L_{rm gd}$ of 3 $muhbox{m}$. A very high $BV$ of 1813 V across 10- $mu hbox{m}$ ohmic gap was achieved for i-GaN grown on thick buffers. As the thickness of buffer layers increased, the decreased $D_{D}$ of GaN and increased resistance between surface electrode and substrate yielded a high breakdown.      

N-Face GaN/AlGaN HEMTs Fabricated Through Layer Transfer Technology

We present a new method to fabricate N-face GaN/AlGaN high electron mobility transistors (HEMTs). These devices are extremely promising for ultrahigh frequency applications where low contact resistances and excellent carrier confinement are needed. In this letter, the N-face of a Ga-face AlGaN/GaN epilayer grown on Si(111) is exposed by removing the Si substrate. To provide mechanical support, prior to the substrate removal, the Ga-face of the wafer is bonded to a Si(100) carrier wafer. The resultant N-face GaN/AlGaN heterostructures exhibited record transport properties ($mu_{e} !=! hbox{1670} hbox{cm}^{2}/hbox{V}cdot hbox{s}$, $n_{s} !=! hbox{1.6} !times! hbox{10}^{13}/ hbox{cm}^{2}$, and $R_{rm sh} = hbox{240} Omega/hbox{sq}$ ). These excellent transport properties rendered N-face HEMTs with 30% higher maximum drain current than Ga-face HEMTs and good RF characteristics ($f_{T} = hbox{10.7} hbox{GHz} cdot muhbox{m}$ and $f_{max} = hbox{21.5} hbox{GHz}cdot muhbox{m}$), comparable to state-of-the-art Ga-face devices.      

Impacts of $hbox{N}_{2}$ and $hbox{NH}_{3}$ Plasma Surface Treatments on High-Performance LTPS-TFT With High-$kappa$ Gate Dielectric

Low-temperature polycrystalline-silicon thin-film transistors (LTPS-TFTs) with high- $kappa$ gate dielectrics and plasma surface treatments are demonstrated for the first time. Significant field-effect mobility $mu_{rm FE}$ improvements of $sim$86.0% and 112.5% are observed for LTPS-TFTs with $hbox{HfO}_{2}$ gate dielectric after $hbox{N}_{2}$ and $ hbox{NH}_{3}$ plasma surface treatments, respectively. In addition, the $hbox{N}_{2}$ and $ hbox{NH}_{3}$ plasma surface treatments can also reduce surface roughness scattering to enhance the field-effect mobility $mu_{rm FE}$ at high gate bias voltage $V_{G}$, resulting in 217.0% and 219.6% improvements in driving current, respectively. As a result, high-performance LTPS-TFT with low threshold voltage $V_{rm TH} sim hbox{0.33} hbox{V}$, excellent subthreshold swing S.S. $sim$0.156 V/decade, and high field-effect mobility $mu_{rm FE} sim hbox{62.02} hbox{cm}^{2}/hbox{V} cdot hbox{s}$ would be suitable for the application of system-on-panel.      

An Analytical Method to Extract the Physical Parameters of a Solar Cell From Four Points on the Illuminated $J{-}V$ Curve

For a variety of solar cells, it is shown that the single exponential $J{-}V$ model parameters, namely—ideality factor $eta$ , parasitic series resistance $R_{s}$, parasitic shunt resistance $R_{rm sh}$, dark current $J_{0}$, and photogenerated current $J_{rm ph}$ can be extracted simultaneously from just four simple measurements of the bias points corresponding to $V_{rm oc}$, $sim!hbox{0.6}V_{rm oc}$, $J_{rm sc}$, and $sim! hbox{0.6}J_{rm sc}$ on the illuminated $J{-}V$ curve, using closed-form expressions. The extraction method avoids the measurements of the peak power point and any $dJ/dV$ (i.e., slope). The method is based on the power law $J{-}V$ model proposed recently by us.      

High-Performance Metal/High-$k$ n- and p-MOSFETs With Top-Cut Dual Stress Liners Using Gate-Last Damascene Process on (100) Substrates

Newly proposed mobility-booster technologies are demonstrated for metal/high- $k$ gate-stack n- and pMOSFETs. The process combination of top-cut SiN dual stress liners and damascene gates remarkably enhances local channel stress particularly for shorter gate lengths in comparison with a conventional gate-first process. Dummy gate removal in the damascene gate process induces high channel stress, because of the elimination of reaction force from the dummy gate. PFETs with top-cut compressive stress liners and embedded SiGe source/drains are performed by using atomic layer deposition TiN/$ hbox{HfO}_{2}$ gate stacks with $T_{rm inv} = hbox{1.4} hbox{nm}$ on (100) substrates. On the other hand, nFETs with top-cut tensile stress liners are obtained by using $hbox{HfSi}_{x}/hbox{HfO}_{2}$ gate stacks with $T_{rm inv} = hbox{1.4} hbox{nm}$. High-performance n- and pFETs are achieved with $I_{rm on} = hbox{1300}$ and 1000 $muhbox{A}/muhbox{m} hbox{at} I_{rm off} = hbox{100} hbox{nA}/mu hbox{m}$, $V_{rm dd} = hbox{1.0} hbox{V}$, and a gate length of 40 nm, respectively.      

A $Q$ -Band Four-Element Phased-Array Front-End Receiver With Integrated Wilkinson Power Combiners in 0.18-$mu{{hbox{m}}}$ SiGe BiCMOS Technology

A four-element phased-array front-end receiver based on 4-bit RF phase shifters is demonstrated in a standard 0.18- $mu{{hbox{m}}}$ SiGe BiCMOS technology for $Q$-band (30–50 GHz) satellite communications and radar applications. The phased-array receiver uses a corporate-feed approach with on-chip Wilkinson power combiners, and shows a power gain of 10.4 dB with an ${rm IIP}_{3}$ of $-$13.8 dBm per element at 38.5 GHz and a 3-dB gain bandwidth of 32.8–44 GHz. The rms gain and phase errors are $leq$1.2 dB and $leq {hbox{8.7}}^{circ}$ for all 4-bit phase states at 30–50 GHz. The beamformer also results in $leq$ 0.4 dB of rms gain mismatch and $leq {hbox{2}}^{circ}$ of rms phase mismatch between the four channels. The channel-to-channel isolation is better than $-$35 dB at 30–50 GHz. The chip consumes 118 mA from a 5-V supply voltage and overall chip size is ${hbox{1.4}}times {hbox{1.7}} {{hbox{mm}}}^{2}$ including all pads and CMOS control electronics.      

Improved Microwave Noise Performance by SiN Passivation in AlGaN/GaN HEMTs on Si

Effects of silicon nitride (SiN) surface passivation by plasma enhanced chemical vapor deposition (PECVD) on microwave noise characteristics of AlGaN/GaN HEMTs on high-resistivity silicon (HR-Si) substrate have been investigated. About 25% improvement in the minimum noise figure $(NF_{min})$ (0.52 dB, from 2.03 dB to 1.51 dB) and 10% in the associate gain $(G_{rm a})$ (1.0 dB, from 10.3 dB to 11.3 dB) were observed after passivation. The equivalent circuit parameters and noise source parameters (including channel noise coefficient $(P)$, gate noise coefficient $(R)$, and their correlation coefficient $(C)$ ) were extracted. $P$ , $R$ and $C$ all increased after passivation and the increase of C contributes to the decrease of the noise figure. It was found that the improved microwave small signal and noise performance is mainly due to the increase of the intrinsic transconductance $(g_{{rm m}0})$ and the decrease of the extrinsic source resistance $(R_{rm s})$.      

Positive Bias Temperature Instability (PBTI) Characteristics of Contact-Etch-Stop-Layer-Induced Local-Tensile-Strained $hbox{HfO}_{2}$ nMOSFET

The positive bias temperature instability (PBTI) characteristics of contact-etch-stop-layer (CESL)-strained $hbox{HfO}_{2}$ nMOSFET are thoroughly investigated. For the first time, the effects of CESL on an $hbox{HfO}_{2}$ dielectric are investigated for PBTI characteristics. A roughly 50% reduction of $V_{rm TH}$ shift can be achieved for the 300-nm CESL $hbox{HfO}_{2}$ nMOSFET after 1000-s PBTI stressing without obvious $ hbox{HfO}_{2}/hbox{Si}$ interface degradation, as demonstrated by the negligible charge pumping current increase ($≪$ 4%). In addition, the $hbox{HfO}_{2}$ film of CESL devices has a deeper trapping level (0.83 eV), indicating that most of the shallow traps (0.75 eV) in as-deposited $ hbox{HfO}_{2}$ film can be eliminated for CESL devices.      

Performance Improvement of N-Type $hbox{TiO}_{x}$ Active-Channel TFTs Grown by Low-Temperature Plasma-Enhanced ALD

We report on performance improvement of $n$-type oxide–semiconductor thin-film transistors (TFTs) based on $hbox{TiO}_{x}$ active channels grown at 250 $^{circ}hbox{C}$ by plasma-enhanced atomic layer deposition. TFTs with as-grown $hbox{TiO}_{x}$ films exhibited the saturation mobility $(mu_{rm sat})$ as high as 3.2 $hbox{cm}^{2}/hbox{V}cdothbox{s}$ but suffered from the low on–off ratio $(I_{rm ON}/I_{rm OFF})$ of $hbox{2.0} times hbox{10}^{2}$. $hbox{N}_{2}hbox{O}$ plasma treatment was then attempted to improve $I_{rm ON}/I_{rm OFF}$. Upon treatment, the $hbox{TiO}_{x}$ TFTs exhibited $I_{rm ON}/I_{rm OFF}$ of $hbox{4.7} times hbox{10}^{5}$ and $mu_{rm sat}$ of 1.64 $hbox{cm}^{2}/hbox{V}cdothbox{s}$, showing a much improved performance balance and, thus, demonstrating their potentials for a wide variety of applications such as backplane technology in active-matrix displays and radio-frequency identification tags.      

Anomalous Kink Effect in GaN High Electron Mobility Transistors

An anomalous kink effect has been observed in the room-temperature drain current $I_{D}$ versus drain voltage $V_{rm DS}$ characteristics of GaN high electron mobility transistors. The kink is originated by a buildup (at low $V_{rm DS}$) and subsequent release (at high $V_{rm DS}$) of negative charge, resulting in a shift of pinch-off voltage $V_{P}$ toward more negative voltages and in a sudden increase in $I_{D}$. The kink is characterized by extremely long negative charge buildup times and by a nonmonotonic behavior as a function of photon energy under illumination. The presence of traps in the GaN buffer may explain both spectrally resolved photostimulation data and the slow negative charge buildup.      

Strain Enhanced nMOS Using In Situ Doped Embedded $hbox{Si}_{1 - x}hbox{C}_{x}$ S/D Stressors With up to 1.5% Substitutional Carbon Content Grown Using a Novel Deposition Process

This letter reports on the implementation of high carbon content and high phosphorous content $hbox{Si}_{1 - x}hbox{C}_{x}$ layers in the source and drain regions of n-type MOSFET in a 65-nm-node integration scheme. The layers were grown using a novel epitaxial process. It is shown that by implementing stressors with $x approx hbox{0.01}$ , nMOSFET device performance is enhanced by up to 10%, driving 880 $mu hbox{A}/muhbox{m}$ at 1-V $V_{rm DD}$. It is also demonstrated that the successful implementation of $hbox{Si}_{1 - x} hbox{C}_{x}$ relies on the careful choice of integration and epitaxial layer parameters. There is a clear impact of the postepitaxial implantation and thermal treatment on the retained substitutional C content $([C_{rm sub}])$. Furthermore, adding a Si capping layer on top of the $hbox{Si}_{1 - x}hbox{C}_{x}$, greatly improves upon the stressors' stability during the downstream processing and the silicide sheet resistance.      

Investigation of Al-Doped Emitter on N-Type Rear Junction Solar Cells

This brief models the junction discontinuities of a rear Al-doped $ hbox{p}^{+}$ emitter $(hbox{np}^{+})$ formed by screen printing and firing. Theoretical fitting of the suns–$V_{rm oc}$ data to the circuit model shows that not only do the junction discontinuities deteriorate cell $V_{rm oc}$, for the case of p-type cells, but they also reduce cell fill factor on n-type cells through increased junction recombination and nonlinear shunts.      

A 10-kV Monolithic Darlington Transistor With $beta_{ rm forced}$ of 336 in 4H-SiC

4H-SiC bipolar Darlington transistors with a record-high current gain have been demonstrated. The dc forced current gain was measured up to 336 at 200 $hbox{W/cm}^{2}$ ( $J_{C} = hbox{35} hbox{A/cm}^{2}$ at $V_{rm CE} = hbox{5.7} hbox{V}$) at room temperature. The current gain exhibits a negative temperature coefficient and remains as high as 135 at 200 $^{circ}hbox{C}$. The specific on-resistance is 140 $hbox{m}Omegacdothbox{cm}^{2}$ at room temperature and increases at elevated temperatures. An open-emitter breakdown voltage $(BV_{rm CBO})$ of 10 kV was achieved at a leakage current density of $≪hbox{1} hbox{mA/cm}^{2}$. The device exhibits an open-base breakdown voltage $(BV_{rm CEO})$ of 9.5 kV. The high current gain of SiC Darlington transistors can significantly reduce the gate-drive power consumption with the same forward-voltage drop as that of 10-kV SiC bipolar junction transistors, thus making the device attractive for high-power high-temperature applications.      

55% PAE and High Power Ka-Band GaN HEMTs With Linearized Transconductance via $hbox{n}+$ GaN Source Contact Ledge

We report small- and large-signal performances of 140-nm gatelength field-plated GaN HEMTs at Ka-band frequencies, in which the GaN HEMTs were fabricated with $hbox{n}+$ source contact ledge. The parasitic channel resistance is reduced by $ sim$50%, whereas the peak extrinsic transconductance is improved by 20% from 370 to 445 mS/mm. The GaN HEMTs with $hbox{n}+$ source ledge exhibit improvement of maximum stable gain by at least 0.7 dB over reference devices without $hbox{n}+$ ledge. At 30 GHz, CW output power density of 10 W/mm is measured with peak PAE of 40% and associated gain of 8.4 dB at $hbox{Vds} = hbox{42} hbox{V}$. At $hbox{Vds} = hbox{30} hbox{V}$, the output power density is measured as 7.3 W/mm with peak PAE of 50%, peak DE of 58%, and associated gain of 8.5 dB. The best PAE was measured as 55% at 5 W/mm at 30, 33, and 36 GHz, where the associated gains were 7.9, 7.6, and 8.2 dB, respectively.      

Gate-First AlGaN/GaN HEMT Technology for High-Frequency Applications

This letter describes a gate-first AlGaN/GaN high-electron mobility transistor (HEMT) with a W/high- $k$ dielectric gate stack. In this new fabrication technology, the gate stack is deposited before the ohmic contacts, and it is optimized to stand the 870 $^{circ}hbox{C}$ ohmic contact annealing. The deposition of the W/high-$k$ dielectric protects the intrinsic transistor early in the fabrication process. Three different gate stacks were studied: $hbox{W}/ hbox{HfO}_{2}$, $hbox{W}/hbox{Al}_{2}hbox{O}_{3}$ , and $hbox{W}/hbox{HfO}_{2}/hbox{Ga}_{2}hbox{O}_{3}$ . DC characterization showed transconductances of up to 215 mS/mm, maximum drain current densities of up to 960 mA/mm, and more than five orders of magnitude lower gate leakage current than in the conventional gate-last Ni/Au/Ni gate HEMTs. Capacitance–voltage measurements and pulsed-$IV$ characterization show no hysteresis for the $hbox{W}/hbox{HfO}_{2}/ hbox{Ga}_{2}hbox{O}_{3}$ capacitors and low interface traps. These W/high- $k$ dielectric gates are an enabling technology for self-aligned AlGaN/GaN HEMTs, where the gate contact acts as a hard mask to the ohmic deposition.