A high quality factor and low power loss micromachined RF bifilar transformer for UWB RFIC applications

In this letter, the authors demonstrate that high quality factor and low power loss transformers can be obtained by using the CMOS process-compatible backside inductively coupled plasma (ICP) deep-trench technology to selectively remove the silicon underneath the transformers. A 62.4% (from 8.99 to 14.6) and a 205.8% (from 8.6 to 26.3) increase in the Q-factor, a 10.3% (from 0.697 to 0.769) and a 30.2% (from 0.652 to 0.849) increase in the maximum available power gain (G/sub Amax/), and a 0.43- (from 1.57 to 1.14 dB) and a 1.15-dB (from 1.86 to 0.71 dB) reduction in the minimum noise figure (NF/sub min/) were achieved at 5.2 and 10 GHz, respectively, for a bifilar transformer with overall dimension of 240/spl times/240 /spl mu/m/sup 2/ after the backside ICP etching. The values of G/sub Amax/ of 0.769 and 0.849 are both state-of-the-art results among all reported on-chip bifilar transformers. These results indicate that the backside ICP deep-trench technology is very promising for high-performance radio frequency integrated circuit applications.     

Wafer-level packaging technology for high-Q on-chip inductors and transmission lines

In the current trend toward portable applications, high-Q integrated inductors have gained considerable importance. Hence, much effort has been spent to increase the performance of on-chip Si inductors. In this paper, wafer-level packaging (WLP) techniques have been used to integrate state-of-the-art high-Q on-chip inductors on top of a five-levels-of-metal Cu damascene back-end of line (BEOL) silicon process using 20-/spl Omega//spl middot/cm Si wafers. The inductors are realized above passivation using thick post-processed low-K dielectric benzocyclobutene (BCB) and Cu layers. For a BCB-Cu thickness of 16 /spl mu/m/10 /spl mu/m, a peak single-ended Q factor of 38 at 4.7 GHz has been measured for a 1-nH inductor with a resonance frequency of 28 GHz. Removing substrate contacts slightly increases the performance, though a more significant improvement has been obtained by combining post-processed passives with patterned ground shields: for a 2.3-nH above integrated-circuit (above-IC) inductor, a 115% increase in Q/sub BW//sup max/ (37.5 versus 17.5) and a 192% increase in resonance frequency (F/sub res/: 12 GHz versus 5 GHz) have been obtained as compared to the equivalent BEOL realization with a patterned ground shield. Next to inductors, high-quality on-chip transmission lines may be realized in the WLP layers. Losses below -0.2 dB/mm at 25 GHz have been measured for 50-/spl Omega/ post-processed coplanar-waveguide lines, above-IC thin-film microstrip lines have measured losses below -0.12 dB/mm at 25 GHz.     

SOI technology for radio-frequency integrated-circuit applications

This paper presents a silicon-on-insulator (SOI) integration technology, including structures and processes of OFF-gate power nMOSFETs, conventional lightly doped drain (LDD) nMOSFETs, and spiral inductors for radio frequency integrated circuit (RFIC) applications. In order to improve the performance of these integrated devices, body contact under the source (to suppress floating-body effects) and salicide (to reduce series resistance) techniques were developed for transistors; additionally, locally thickened oxide (to suppress substrate coupling) and ultra-thick aluminum up to 6 /spl mu/m (to reduce spiral resistance) were also implemented for spiral inductors on high-resistivity SOI substrate. All these approaches are fully compatible with the conventional CMOS processes, demonstrating devices with excellent performance in this paper: 0.25-/spl mu/m gate-length offset-gate power nMOSFET with breakdown voltage (BV/sub DS/) /spl sim/ 22.0 V, cutoff frequency (f/sub T/)/spl sim/15.2 GHz, and maximal oscillation frequency (f/sub max/)/spl sim/8.7 GHz; 0.25-/spl mu/m gate-length LDD nMOSFET with saturation current (I/sub DS/)/spl sim/390 /spl mu/A//spl mu/m, saturation transconductance (g/sub m/)/spl sim/197 /spl mu/S//spl mu/m, cutoff frequency /spl sim/ 25.6 GHz, and maximal oscillation frequency /spl sim/ 31.4 GHz; 2/5/9/10-nH inductors with maximal quality factors (Q/sub max/) 16.3/13.1/8.95/8.59 and self-resonance frequencies (f/sub sr/) 17.2/17.7/6.5/5.8 GHz, respectively. These devices are potentially feasible for RFIC applications.     

CMOS-compatible micromachined edge-suspended spiral inductors with high Q-factors and self-resonance frequencies

This paper reports a new category of high-Q edge-suspended inductors (ESI) that are fabricated using CMOS-compatible micromachining techniques. This structure was designed based on the concept that the current was crowded at the edges of the conducting metal wires at high frequencies due to the proximity effect. The substrate coupling and loss can be effectively suppressed by removing the silicon around and underneath the edges of the signal lines. Different from the conventional air-suspended inductors that have the inductors built on membranes or totally suspended in the air, the edge-suspended structures have the silicon underneath the center of the metal lines as the strong mechanical supports. The ESIs are fabricated using a combination of deep dry etching and anisotropic wet etching techniques that are compatible with CMOS process. For a three-turn 4.5-nH inductor, a 70% increase (from 6.8 to 11.7) in maximum Q-factor and a 57% increase (from 9.1 to 14.3 GHz) in self-resonance frequency were obtained with a 11-/spl mu/m suspended edge in 25-/spl mu/m-wide lines.     

Implementation of perfect-magnetic-coupling ultralow-loss transformer in RFCMOS technology

In this letter, we propose a single-turn multiple-layer interlaced stacked transformer structure with nearly perfect magnetic-coupling factor (k/sub IM//spl sim/1) using standard mixed-signal/RF CMOS (or BiCMOS) technology. A single-turn six-layer interlaced stacked transformer was implemented to demonstrate the proposed structure. Temperature dependence (from -25/spl deg/C to 175/spl deg/C) of the quality-factor (Q-factor), k/sub Im/, resistive-coupling factor (k/sub Re/), maximum available power gain (G/sub Amax/), and minimum noise figure (NF/sub min/) performances of the transformer are reported. State-of-the-art G/sub Amax/ of 0.762 and 0.904 (i.e., NF/sub min/ of 1.181 dB and 0.437 dB) have been achieved at 5.2 and 8 GHz, respectively, at room temperature, mainly due to the perfect magnetic-coupling factor and the high resistive-coupling factor. The present analysis is helpful for RF engineers to design ultralow-voltage high-performance transformer-feedback low-noise amplifiers and voltage-controlled oscillators, and other radio frequency integrated circuits which include transformers.     

Temperature and substrate-impedance dependence of noise figure of monolithic RF inductors on silicon

In this letter, we analyze the effects of temperature (from -50/spl deg/C to 200/spl deg/C) and substrate impedance on the noise figure (NF) and quality factor (Q-factor) performances of monolithic RF inductors on silicon. The results show a 0.75 dB (from 0.98 to 0.23 dB) reduction in minimum NF (NF/sub min/) at 8 GHz, an 86.1% (from 15.1 to 28.1) increase in maximum Q-factor (Q/sub max/), and a 4.8% (from 16.5 to 17.3 GHz) improvement in self-resonant frequency (f/sub SR/) were obtained if post-process of proton implantation had been done. This means the post-process of proton implantation is effective in improving the NF and Q-factor performances of inductors on silicon mainly due to the reduction of eddy current loss in the silicon substrate. In addition, it was found that NF increases with increasing temperature but show a reverse behavior within a higher frequency range. This phenomenon can be explained by the positive temperature coefficients of the series metal resistance (R/sub s/), the parallel substrate resistances (R/sub sub1/ and R/sub sub2/), and the resistance R/sub s1/ of the substrate transformer loop. The present analyzes are helpful for RF designers to design less temperature-sensitive high-performance fully on-chip low-noise-amplifiers (LNAs) and voltage-controlled-oscillators (VCOs) for single-chip receiver front-end applications.     

High Q multilayer spiral inductor on silicon chip for 5/spl sim/6 GHz

High Q-values of spiral inductors at frequency around 5/spl sim/6 GHz have been achieved with a multilayer spiral (MLS) structure on a high loss silicon substrate. Compared to a one-layer spiral (OLS) inductor, the Q-value of a 4-nH inductor has been improved by about 80% at 5.65 GHz. The impact of the structure on Q-value and resonant frequency has been analyzed, which shows that an optimal height for the via of MLS inductors should be considered when inductors are designed. The fabrication process is compatible with Cu/SiO/sub 2/ interconnect technology.     

High-Q factor three-dimensional inductors

In this paper, the great flexibility of three-dimensional (3-D) monolithic-microwave integrated-circuit technology is used to improve the performance of on-chip inductors. A novel topology for high-Q factor spiral inductor that can be implemented in a single or multilevel configuration is proposed. Several inductors were fabricated on either silicon substrate (/spl rho/ = 30 /spl Omega/ /spl middot/ cm) or semi-insulating gallium-arsenide substrate demonstrating, more particularly, for GaAs technology, the interest of the multilevel configuration. A 1.38-nH double-level 3-D inductor formed on an Si substrate exhibits a very high peak Q factor of 52.8 at 13.6 GHz and a self-resonant frequency as high as 24.7 GHz. Our 4.9-nH double-level GaAs 3-D inductor achieves a peak Q factor of 35.9 at 4.7 GHz and a self-resonant frequency of 8 GHz. For each technology, the performance limits of the proposed inductors in terms of quality factor are discussed. Guidelines for the optimum design of 3-D inductors are provided for Si and GaAs technologies.     

DC, RF, and microwave noise performances of AlGaN/GaN HEMTs on sapphire substrates

High-performance AlGaN/GaN high electron-mobility transistors with 0.18-/spl mu/m gate length have been fabricated on a sapphire substrate. The devices exhibited an extrinsic transconductance of 212 mS/mm, a unity current gain cutoff frequency (f/sub T/) of 101 GHz, and a maximum oscillation frequency (f/sub MAX/) of 140 GHz. At V/sub ds/=4 V and I/sub ds/=39.4 mA/mm, the devices exhibited a minimum noise figure (NF/sub min/) of 0.48 dB and an associated gain (Ga) of 11.16 dB at 12 GHz. Also, at a fixed drain bias of 4 V with the drain current swept, the lowest NFmin of 0.48 dB at 12 GHz was obtained at I/sub ds/=40 mA/mm, and a peak G/sub a/ of 11.71 dB at 12 GHz was obtained at I/sub ds/=60 mA/mm. With the drain current held at 40 mA/mm and drain bias swept, the NF/sub min/,, increased almost linearly with the increase of drain bias. Meanwhile, the Ga values decreased linearly with the increase of drain bias. At a fixed bias condition (V/sub ds/=4 V and I/sub ds/=40 mA/mm), the NF/sub min/ values at 12 GHz increased from 0.32 dB at -55/spl deg/C to 2.78 dB at 200/spl deg/C. To our knowledge, these data represent the highest f/sub T/ and f/sub MAX/, and the best microwave noise performance of any GaN-based FETs on sapphire substrates ever reported.     

Micromachined 22 GHz PI filter by CMOS compatible ICP deep trench technology

A K-band second-order bandpass filter with planar inductive pi-network using CMOS technology is demonstrated for the first time. To reduce the substrate loss of the filter, the CMOS process compatible backside inductively-coupled-plasma (ICP) deep trench technology is used to selectively remove the silicon underneath the filter. After the ICP etching, a 55.5-92.2% improvement in quality factor is achieved for the inductors in the filter. In addition, a 1.1 dB improvement in maximum available power gain (G_Amax) in K-band is achieved for the filter after the ICP etching. These results show that the micromachined pi (PI) filter is very promising for microwave/millimetre-wave RFIC applications     

Micromachined V-band CMOS bandpass filter with 2 dB insertion loss

A low-insertion-loss V-band CMOS bandpass filter is demonstrated. The proposed filter architecture has the following features: the low-frequency transmission-zero (vz1) and the high-frequency transmission-zero (vz2) can be tuned by the series-feedback capacitor Cs and the parallelfeedback capacitor Cp, respectively. To reduce the substrate loss, the CMOS process compatible backside inductively-coupled-plasma (ICP) deep trench technology is used to selectively remove the silicon underneath the filter. After the ICP etching, this filter achieved insertion loss (1/S21) lower than 3 dB over the frequency range 52.5?76.8 GHz. The minimum insertion loss was 2 dB at 63.5 GHz, the best results reported for a V-band CMOS bandpass filter in the literature.     

Broadband microwave noise characteristics of high-linearity composite-channel Al/sub 0.3/Ga/sub 0.7/N/Al/sub 0.05/Ga/sub 0.95/N/GaN HEMTs

We report broadband microwave noise characteristics of a high-linearity composite-channel HEMT (CC-HEMT). Owing to the novel composite-channel design, the CC-HEMT exhibits high gain and high linearity such as an output third-order intercept point (OIP3) of 33.2 dBm at 2 GHz. The CC-HEMT also exhibits excellent microwave noise performance. For 1-/spl mu/m gate-length devices, a minimum noise figure (NF/sub min/) of 0.7 dB and an associated gain (G/sub a/) of 19 dB were observed at 1 GHz, and an (NF/sub mi/) of 3.3 dB and a G/sub a/ of 10.8 dB were observed at 10 GHz. The dependence of the noise characteristics on the physical design parameters, such as the gate-source and gate-drain spacing, is also presented.     

Shielded passive devices for silicon-based monolithic microwave and millimeter-wave integrated circuits

This paper introduces floating shields for on-chip transmission lines, inductors, and transformers implemented in production silicon CMOS or BiCMOS technologies. The shield minimizes losses without requiring an explicit on-chip ground connection. Experimental measurements demonstrate Q-factor ranging from 25 to 35 between 15 and 40 GHz for shielded coplanar waveguide fabricated on 10 /spl Omega//spl middot/cm silicon. This is more than a factor of 2 improvement over conventional on-chip transmission lines (e.g., microstrip, CPW). A floating-shielded, differentially driven 7.4-nH inductor demonstrates a peak Q of 32, which is 35% higher than an unshielded example. Similar results are realizable for on-chip transformers. Floating-shielded bond-pads with 15% less parasitic capacitance and over 60% higher shunt equivalent resistance compared to conventional shielded bondpads are also described. Implementation of floating shields is compatible with current and projected design constraints for production deep-submicron silicon technologies without process modifications. Application examples of floating-shielded passives implemented in a 0.18-/spl mu/m SiGe-BiCMOS are presented, including a 21-26-GHz power amplifier with 23-dBm output at 20% PAE (at 22 GHz), and a 17-GHz WLAN image-reject receiver MMIC which dissipates less than 65 mW from a 2-V supply.     

Low noise RF MOSFETs on flexible plastic substrates

We report a low minimum noise figure (NF/sub min/) of 1.1 dB and high associated gain (12 dB at 10 GHz) for 16 gate-finger 0.18-/spl mu/m RF MOSFETs, after thinning down the Si substrate to 30 /spl mu/m and mounting it on plastic. The device performance was improved by flexing the substrate to create stress, which produced a 25% enhancement of the saturation drain current and lowered NF/sub min/ to 0.92 dB at 10 GHz. These excellent results for mechanically strained RF MOSFETs on plastic compare well with 0.13-/spl mu/m node (L/sub g/=80 nm) devices.     

Micromachined high-Q inductors in a 0.18-μm copper interconnectlow-k dielectric CMOS process

On-chip spiral micromachined inductors fabricated in a 0.18-μm digital CMOS process with 6-level copper interconnect and low-K dielectric are described. A post-CMOS maskless micromachining process compatible with the CMOS materials and design rules has been developed to create inductors suspended above the substrate with the inter-turn dielectric removed. Such inductors have higher quality factors as substrate losses are eliminated by silicon removal and increased self-resonant frequency due to reduction of inter-turn and substrate parasitic capacitances. Quality factors up to 12 were obtained for a 3.2-nH micromachined inductor at 7.5 GHz. Improvements of up to 180% in maximum quality factor, along with 40%-70% increase in self-resonant frequency were seen over conventional inductors. The effects of micromachining on inductor performance was modeled using a physics-based model with predictive capability. The model was verified by measurements at various stages of the post-CMOS processing. Micromachined inductor quality factor is limited by series resistance up to a predicted metal thickness of between 6-10 μm     

Microwave noise performance of AlGaN-GaN HEMTs with small DC power dissipation

We report low microwave noise performance of discrete AlGaN-GaN HEMTs at DC power dissipation comparable to that of GaAs-based low-noise FETs. At 1-V source-drain (SD) bias and DC power dissipation of 97 mW/mm, minimum noise figures (NF/sub min/) of 0.75 dB at 10 GHz and 1.5 dB at 20 GHz were achieved, respectively. A device breakdown voltage of 40 V was observed. Both the low microwave noise performance at small DC power level and high breakdown voltage was obtained with a shorter SD spacing of 1.5 /spl mu/m in 0.15-/spl mu/m gate length GaN HEMTs. By comparison, NF/sub min/ with 2 /spl mu/m SD spacing was 0.2 dB greater at 10 GHz.     

Large suspended inductors on silicon and their use in a 2-μmCMOS RF amplifier

Large spiral inductors encased in oxide over silicon are shown to operate beyond the UHF band when the capacitance and loss resistance are greatly reduced by selective removal of the underlying substrate. Using a 100-nH inductor whose self-resonance lies at 3 GHz, a balanced tuned amplifier with a gain of 14 dB centered at 770 MHz has been implemented in a standard digital 2-μm CMOS IC process. The core amplifier noise figure is 6 dB, and the power dissipation is 7 mW for a 3-V supply     

Very low noise RF nMOSFETs on plastic by substrate thinning and wafer transfer

A very low minimum noise figure (NF/sub min/) of 1.2 dB and a high associated gain of 12.8 dB at 10 GHz were measured for six-finger, 0.18-/spl mu/m radio frequency (RF) metal-oxide semiconductor field-effect transistors mounted on insulating plastic following substrate-thinning (/spl sim/30 /spl mu/m) and wafer transfer. Before this process, the devices had a slightly better RF performance of 1.1-dB NF/sub min/ and a 13.7-dB associated gain. The small RF performance degradation of the active transistors transferred to plastic shows the potential of integrating electronics onto plastic.     

Microwave noise characteristics of AlGaN/GaN HEMTs on SiC substrates for broad-band low-noise amplifiers

This letter reports high-performance passivated AlGaN/GaN high electron-mobility transistors (HEMTs) with 0.25-/spl mu/m gate-length for low noise applications. The devices exhibited a minimum noise figure (NF/sub min/) of 0.98 dB and an associated gain (G/sub a/) of 8.97 dB at 18 GHz. The noise resistance (R/sub n/), the measure of noise sensitivity to source mismatch, is 31/spl Omega/ at 18 GHz, which is relatively low and suitable for broad-band low noise amplifiers. The noise modeling analysis shows that the minimum noise figure of the GaN HEMT can be reduced further by reducing noise contributions from parasitics. These results demonstrate the viability of AlGaN/GaN HEMTs for low-noise as well as high power amplifiers.     

On-chip solenoid inductors with high quality factor for high frequency magnetic integrated circuits

On-chip solenoid inductors for high frequency magnetic integrated circuits are proposed. The eddy current loss was reduced by dividing the inductor into three consecutive inductors connected in series. The inductor has an inductance of 1.1nH and the maximum quality factor (Q/sub max/) of 50.5. The self-resonant frequency and the operating frequency at Q/sub max/ are greater than 17.5GHz and 16.7GHz, respectively.