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1.
This paper describes a system architecture and CMOS implementation that leverages the inherently high mechanical quality factor (Q) of a MEMS gyroscope to improve performance. The proposed time domain scheme utilizes the often-ignored residual quadrature error in a gyroscope to achieve, and maintain, perfect mode-matching (i.e., $sim$0 Hz split between the high-Q drive and sense mode frequencies), as well as electronically control the sensor bandwidth. A CMOS IC and control algorithm have been interfaced with a 60 $mu{hbox {m}}$ thick silicon mode-matched tuning fork gyroscope $({rm M}^{2}mathchar"707B {rm TFG})$ to implement an angular rate sensing microsystem with a bias drift of 0.16$^{circ}/{hbox{hr}}$. The proposed technique allows microsystem reconfigurability—the sensor can be operated in a conventional low-pass mode for larger bandwidth, or in matched mode for low-noise. The maximum achieved sensor Q is 36,000 and the bandwidth of the microsensor can be varied between 1 to 10 Hz by electronic control of the mechanical frequencies. The maximum scale factor of the gyroscope is 88 ${hbox{mV}}/^{circ}/{hbox{s}}$ . The 3$~$ V IC is fabricated in a standard 0.6 $ mu{hbox {m}}$ CMOS process and consumes 6 mW of power with a die area of 2.25 ${hbox {mm}}^{2}$.   相似文献   

2.
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.   相似文献   

3.
We report the first demonstration of a strained $hbox{In}_{0.53} hbox{Ga}_{0.47}hbox{As}$ channel n-MOSFET featuring in situ doped $hbox{In}_{0.4}hbox{Ga}_{0.6}hbox{As}$ source/drain (S/D) regions. The in situ silicondoped $hbox{In}_{0.4}hbox{Ga}_{0.6}hbox{As}$ S/D was formed by a recess etch and a selective epitaxy of $hbox{In}_{0.4}hbox{Ga}_{0.6}hbox{As}$ in the S/D by metal–organic chemical vapor deposition. A lattice mismatch of $sim$0.9% between $ hbox{In}_{0.53}hbox{Ga}_{0.47}hbox{As}$ and $hbox{In}_{0.4} hbox{Ga}_{0.6}hbox{As}$ S/D gives rise to lateral tensile strain and vertical compressive strain in the $hbox{In}_{0.53}hbox{Ga}_{0.47}hbox{As}$ channel region. In addition, the in situ Si-doping process increases the carrier concentration in the S/D regions for series-resistance reduction. Significant drive-current improvement over the control n-MOSFET with Si-implanted $hbox{In}_{0.53}hbox{Ga}_{0.47}hbox{As}$ S/D regions was achieved. This is attributed to both the strain-induced band-structure modification in the channel that reduces the effective electron mass along the transport direction and the reduction in the S/D series resistance.   相似文献   

4.
New hydrogen-sensing amplifiers are fabricated by integrating a GaAs Schottky-type hydrogen sensor and an InGaP–GaAs heterojunction bipolar transistor. Sensing collector currents ( $I_{rm CN}$ and $I_{rm CH}$) reflecting to $hbox{N}_{2}$ and hydrogen-containing gases are employed as output signals in common-emitter characteristics. Gummel-plot sensing characteristics with testing gases as inputs show a high sensing-collector-current gain $(I_{rm CH}/I_{rm CN})$ of $≫hbox{3000}$. When operating in standby mode for in situ long-term detection, power consumption is smaller than 0.4 $muhbox{W}$. Furthermore, the room-temperature response time is 85 s for the integrated hydrogen-sensing amplifier fabricated with a bipolar-type structure.   相似文献   

5.
Several fully-integrated multi-stage lumped-element quadrature hybrids that enhance bandwidth, amplitude and phase accuracies, and robustness are presented, and a fully-integrated double-quadrature heterodyne receiver front-end that uses two-stage Lange/Lange couplers is described. The Lange/Lange cascade exploits the inherent wide bandwidth characteristic of the Lange hybrid and enables a robust design using a relatively low transformer coupling coefficient. The measured image-rejection ratio is $>$ 55 dB over a 200 MHz bandwidth centered around 5.25 $~$GHz without any tuning, trimming, or calibration; the front-end features 23.5 dB gain, $-$79 dBm sensitivity, 5.6 dB SSB NF, $-$7$~$ dBm IIP3, $-$18 dB $S_{11}$ and a 1 mm $times$ 2 mm die area in 0.18$ mu{hbox {m}}$ CMOS.   相似文献   

6.
This paper discusses the design of a novel photoacoustic microscopy imaging system with promise for studying the structure of tissue microvasculature for applications in visualizing angiogenesis. A new 16 channel analog and digital high-frequency array based photoacoustic microscopy system (PAM) was developed using an Nd:YLF pumped tunable dye laser, a 30 MHz piezo composite linear array transducer, and a custom multichannel receiver electronics system. Using offline delay and sum beamforming and beamsteering, phantom images were obtained from a 6 $mu{hbox {m}}$ carbon fiber in water at a depth of 8 mm. The measured $-6~{rm dB}$ lateral and axial spatial resolution of the system was $100pm 5~mu{hbox {m}}$ and $45pm 5~mu{hbox {m}}$, respectively. The dynamic focusing capability of the system was demonstrated by imaging a composite carbon fiber matrix through a 12.5 mm imaging depth. Next, 2-D in vivo images were formed of vessels around 100 $mu{hbox {m}}$ in diameter in the human hand. Three-dimensional in vivo images were also formed of micro-vessels 3 mm below the surface of the skin in two Sprague Dawley rats.   相似文献   

7.
As the size of CMOS devices is scaled down to nanometers, noise can significantly affect circuit performance. Because noise is random and dynamic in nature, a probabilistic-based approach is better suited to handle these types of errors compared with conventional CMOS designs. In this paper, we propose a cost-effective probabilistic-based noise-tolerant circuit-design methodology. Our cost-effective method is based on master-and-slave Markov random field (MRF) mapping and master-and-slave MRF logic-gate construction. The resulting probabilistic-based MRF circuit trades hardware cost for circuit reliability. To demonstrate a noise-tolerant performance, an 8-bit MRF carry-lookahead adder (MRF_CLA) was implemented using the 0.13-${rm mu}hbox{m}$ CMOS process technology. The chip measurement results show that the proposed master-and-slave MRF_CLA can provide a $7.00times 10^{-5}$ bit-error rate (BER) under 10.6-dB signal-to-noise ratio, while the conventional CMOS_CLA can only provide $8.84times 10^{-3}$ BER. Because of high noise immunity, the master-and-slave MRF_CLA can operate under 0.25 V to tolerate noise interference with only 1.9 ${rm mu}hbox{W/MHz}$ of energy consumption. Moreover, the transistor count can be reduced by 42% as compared with the direct-mapping MRF_CLA design .   相似文献   

8.
A $g_{m}$-boosted resistive feedback low-noise amplifier (LNA) using a series inductor matching network and its application to a 2.4 GHz LNA is presented. While keeping the advantage of easy and reliable input matching of a resistive feedback topology, it takes an extra advantage of $g_{m}$ -boosting as in inductively degenerated topology. The gain of the LNA increases by the $Q$ -factor of the series RLC input network, and its noise figure (NF) is reduced by a similar factor. By exploiting the $g_{m}$-boosting property, the proposed fully integrated LNA achieves a noise figure of 2.0 dB, S21 of 24 dB, and IIP3 of ${- 11}~ hbox{dBm}$ while consuming 2.6 mW from a 1.2 V supply, and occupies 0.6 ${hbox {mm}}^{2}$ in 0.13-$mu{hbox {m}}$ CMOS, which provides the best figure of merit. This paper also includes an LNA of the same topology with an external input matching network which has an NF of 1.2 dB.   相似文献   

9.
This paper investigates the program saturation in aggressively scaled interpoly dielectric (IPD) floating-gate (FG) cells for nand application. To describe the program saturation in IPD stacks containing thick suboxides $(geq hbox{4} hbox{nm})$ , a simple model was developed, directly yielding the maximum reachable programmed threshold voltage level for a given FG cell geometry. The presented model agrees very well to program saturation measurements carried out on a 48 nm FG nand technology with an IPD composed of $hbox{SiO}_{2}$ and $ hbox{Al}_{2}hbox{O}_{3}$. By extending the considerations to an arbitrary IPD, this paper represents the first attempt to quantify the IPD current blocking ability required for future scaled FG memory cells.   相似文献   

10.
In this paper, we will study the exponential sum $sum_{xin {BBF}_q}chi(alpha x^{(p^k+1)/2}+beta x)$ that is related to the generalized Coulter–Matthews function $x^{(p^k+1)/2}$ with $k/{rm gcd}(m,k)$ odd. As applications, we obtain the following: the correlation distribution of a $p$-ary $m$-sequence and a decimated $m$-sequence of degree ${p^k+1 over 2}$;   相似文献   

11.
A high-$T_{c}$ superconducting (HTS) single-flux-quantum (SFQ) logic family including an and gate, an or gate, and an inverter was designed. The circuit parameters were optimized for a Josephson junction's critical current density, which may change due to a temperature change or insufficient run-to-run reproducibility of the fabrication process. New circuit design layout rules were implemented to improve $I_{c}$ uniformity. As a result, all circuits were successfully tested and show at least $pm$40% critical current density operational margins. An effect of the parasitic capacitance formed by a junction electrode and a ground plane on the operating margins of the and gate was investigated by numerical simulation. Test circuits were fabricated using $hbox{YBa}_{2} hbox{Cu}_{3}hbox{O}_{7 - delta}$ ramp-edge junction technology and were operated at temperatures higher than 30 K. Bias current margins were also measured, and they found to be close to the simulated ones.   相似文献   

12.
We have developed ZnO thin-film transistor design and fabrication techniques to demonstrate microwave frequency operation with 2-$muhbox{m}$ gate length devices produced on GaAs substrates. Using $hbox{SiO}_{2}$ gate insulator and pulsed laser deposited ZnO active layers, a drain–current on/off ratio of $hbox{10}^{12}$, a drain–current density of 400 mA/mm, a field-effect mobility of $hbox{110} hbox{cm}^{2}!/ hbox{V}!cdothbox{s}$, and a subthreshold gate voltage swing of 109 mV/dec were achieved. Devices with Ti-gate metal had current and power gain cutoff frequencies of 500 and 400 MHz, respectively.   相似文献   

13.
We report on the fabrication of ZnO-based dual gate (DG) thin-film transistors (TFTs) with 20-nm-thick $hbox{Al}_{2}hbox{O}_{3}$ for both top and bottom dielectrics, which were deposited by atomic layer deposition on glass substrates at 200 $^{ circ}hbox{C}$. As characterized with single gate (SG), DG, and ground plane (GP) modes, our ZnO TFTs are well operated under 5 V. DG-mode TFT showed a field mobility of 0.38 $ hbox{cm}^{2}/hbox{V} cdot hbox{s}$, a high saturation current of 6 $muhbox{A}$, and an on/off current ratio of $sim hbox{10}^{6}$, while SG- and GP-mode TFTs showed a similar value of mobility but with lower current. Using DG and GP modes, nor gate operation was well demonstrated.   相似文献   

14.
Ultrathin-barrier normally off AlN/GaN/AlGaN double-heterostructure field-effect transistors using an in situ SiN cap layer have been fabricated on 100-mm Si substrates for the first time. The high 2DEG density in combination with an extremely thin barrier layer leads to enhancement-mode devices with state-of-the-art combination of specific on-resistance that is as low as 1.25 $hbox{m}Omegacdothbox{cm}^{2}$ and breakdown voltage of 580 V at ${V}_{rm GS} = hbox{0} hbox{V}$ . Despite the 2-$muhbox{m}$ gate length used, the transconductance peaks above 300 mS/mm. Furthermore, pulsed measurements show that the devices are dispersion free up to high drain voltage ${V}_{rm DS} = hbox{50} hbox{V}$. More than 200 devices have been characterized in order to confirm the reproducibility of the results.   相似文献   

15.
Ga-rich GaZnO thin films were prepared by metal–organic chemical vapor deposition. The optical bandgap of GaZnO films can be engineered from 3.3 to 4.9 eV by varying the Ga content. The film is amorphortized and the resistivity increases with an increase of Ga content. The Ga-rich GaZnO alloy with lower resistivity is investigated as a UV transparent conductor, while the semi-insulating Ga-rich GaZnO film with high transparency at 280–900 nm is employed as the channel layer to fabricate deep UV transparent thin-film transistor. The transistor shows a typical n-channel field-effect characteristic with a current on/off ratio of $hbox{10}^{4}$$ hbox{10}^{5}$, a threshold voltage of $sim$42 V, a saturated field-effect mobility of $sim!hbox{0.06} hbox{cm}^{2} cdot hbox{V}^{-1} cdot hbox{s}^{-1}$, and a subthreshold swing of $ sim!hbox{7.7} hbox{V} cdot hbox{decade}^{-1}$.   相似文献   

16.
A 5-GHz dual-path integer-$N$ Type-II phase-locked loop (PLL) uses an LC voltage-controlled oscillator and softly switched varactors in an overlapped digitally controlled integral path to allow a large fine-tuning range of approximately 160 MHz while realizing a low susceptibility to noise and spurs by using a low $K_{rm VCO}$ of 3.2 MHz/V. The reference spur level is less than $-$70 dBc with a 1-MHz reference frequency and a total loop-filter capacitance of 26 pF. The measured phase noise is $-$75 and $-$115 dBc/Hz at 10-kHz and 1-MHz offsets, respectively, using a loop bandwidth of approximately 30 kHz. This 0.25-${hbox{mm}}^{2}$ PLL is fabricated in a 90-nm digital CMOS process and consumes 11 mW from a 1.2-V supply.   相似文献   

17.
A high-voltage lateral double-diffusion MOSFET (LDMOS) with a charge-balanced surface low on-resistance path (CBSLOP) layer is proposed and experimentally demonstrated using a modified CMOS process. The CBSLOP layer can not only provide a low on-resistance path in the on-state but also keep the charge balance between the N and P pillars of a surface low on-resistance path in the off-state, which results in improved breakdown voltage (BV). The experimental results show that the CBSLOP-LDMOS with a drift length of 35 $mu hbox{m}$ exhibits a BV of 500 V and specific on-resistance $(R_{{rm on}, {rm sp}}!)$ of 96 $hbox{m}Omega cdot hbox{cm}^{2}$, yielding to a power figure of merit $(BV^{2}!!/ !R_{{rm on}, {rm sp}})$ of 2.6 $hbox{MW}/hbox{cm}^{2}$ . The excellent device performances, coupled with a CMOS-compatible fabrication process, make the proposed CBSLOP-LDMOS a promising candidate for smart power integrated circuit.   相似文献   

18.
Micro-springs for integrated circuit test and packaging are demonstrated as soldered flip chip interconnects in a direct die to printed circuit board package. The spring interconnects are fabricated with thin film metallization as the last step in a wafer-scale process. The z-compliance of the interconnects can be used to test and/or burn-in parts in wafer form. After the parts are diced from the wafer, the springs then become the first-level (and often the last-level) interconnect between the chip and the board. The xy-compliance of the interconnect enables considerably large die to be soldered to an organic printed circuit board without underfill using a surface mount compatible process. To demonstrate this concept, daisy chain test vehicles were fabricated on die measuring 11.5 mm $times$ 6.5 mm with 48 spring contacts on a 0.8 mm $times$ 0.65 mm grid array, each spring measuring 400 $, mu$m $times$ 100 $mu$m. The parts were placed onto organic boards with screen printed solder paste using a pick and place machine. The parts were reflowed to complete the solder connection to each spring using eutectic and lead-free solder. Assembled parts have undergone ${>}20thinspace 000$ hot plate thermal cycles and ${>}1000$ oven thermal cycles without failure.   相似文献   

19.
We report the charge transport and inferred surface depletion characteristics of silicon nanowires (Si NWs) with diameters of 90–170 nm after boron doping to $hbox{8}times hbox{10}^{17}$ and $hbox{4} times hbox{10}^{19} hbox{cm}^{-3}$ by a proximity diffusion doping technique. Four-probe current–voltage measurements were performed to obtain the NW resistivity, and the electrically active dopant concentration and surface oxide charge density were extracted by varying the NW diameter. The Ti/Au to Si NW contact resistance and specific contact resistivity were also obtained, and specific contact resistivities as low as $hbox{2} times hbox{10}^{-5} Omega cdot hbox{cm}^{2}$ were achieved. The derived parameters for these ex situ boron-doped Si NWs agree reasonably well with the expected characteristics and earlier reported results for in situ boron-doped Si NWs. Interface charge creates a surface depletion region in p-type Si NWs, which decreases the conducting area of the NW. This effect increases the NW resistance and becomes increasingly significant with decreasing dopant concentration and NW diameter. A simple method is presented to estimate the relative influence of surface charge density on electrical transport in NWs for this case.   相似文献   

20.
We have studied a bottom-gate polycrystalline-silicon thin-film transistor (poly-Si TFT) with amorphous-silicon (a-Si) ${rm n}^{+}$ contacts and center-offset gated structure, where intrinsic poly-Si is used in the center-offset region. The fabrication process is compatible with the conventional a-Si TFT with addition of thermal annealing for crystallization of a-Si. The bottom-gate poly-Si TFT with a 5-$muhbox{m}$ offset length exhibited a field-effect mobility of 18.3 $hbox{cm}^{2}/hbox{V} cdot hbox{s}$ and minimum OFF-state current of $hbox{2.79} times hbox{10}^{-12} hbox{A}/muhbox{m}$ at $V_{rm ds} = hbox{5} hbox{V}$. The leakage currents are two orders of magnitude lower than those of a nonoffset TFT with mobility drop from 23.8 to 18.3 $hbox{cm}^{2}/ hbox{V} cdot hbox{s}$.   相似文献   

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