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Efficient Signal Alignment Algorithm for Undersampling Digital Predistortion
Chengye JiangWen QiaoGuichen YangFalin Liu
Keywords:Time-domain analysisTime-varying systemsDelay estimationWireless communicationPredistortionCorrelationDiscrete Fourier transformsapproximation theorydata preparationdelayssignal samplingbasis manifold regularizationBMRDPDefficient signal alignment algorithmfractional delay alignmentfractional delay approximation solutionhigh alignment accuracylow complexityTaylor expansion-based methodultralow sampling rateundersampling digital predistortionBasis manifold regularization (BMR)digital predistortion (DPD)power amplifiers (PAs)signal alignmentundersampling
Abstracts:Undersampling is an effective way to reduce the cost of digital predistortion (DPD), but it poses challenges for signal alignment, especially for fractional delay alignment. In this letter, a Taylor expansion-based method for fractional delay approximation solution is proposed. To verify the proposed alignment algorithm, the basis manifold regularization (BMR) is introduced to ensure that the DPD can converge to a satisfactory performance even at an ultralow sampling rate. Simulations and experimental tests demonstrate that the proposed method not only has high alignment accuracy but also low complexity in comparison with traditional methods.
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A Broadband Rectifier With Wide Incident Angle of Incoming Waves Based on Quadrature Coupler for RF Energy Harvesting
Jian LiuMing Hua ZhangShu Ting CaiJia Fan Chen
Keywords:Radio frequencyBroadband communicationBroadband antennasRectennasPower measurementFrequency measurementWireless communicationenergy harvestingmicrowave power transmissionpower combinerspower dividersradiofrequency power transmissionrectifiersrectifying circuits1.6-2.8 GHzBQCbroadband quadrature couplerbroadband rectifierbroadband subrectifiersdc powerdetailed theoretical analysisdirect current power combinerentire Δφ rangeexcellent broadbandfrequency 1.6 GHz to 2.8 GHzfrequency 2.45 GHzhigh-efficiency radio-frequency energy harvesting systemsidentical input powerincoming wavesoutput portsphase differencepower conversion efficiencyrf energy harvestingRF sourcesWIAwide incident anglewide-incident-angle propertyBroadbandquadrature couplerrectifierwide-incident-angle (WIA)
Abstracts:In this letter, a broadband rectifier with a wide-incident-angle (WIA) property is proposed. The circuit is composed of a broadband quadrature coupler (BQC) and two broadband subrectifiers (RectA and RectB). Here, RectA and RectB are connected to the two output ports of the BQC and combined by a direct current (dc) power combiner. Then, the obtained dc power is transmitted to the load resistor. Besides, two RF sources (RF1 and RF2) with identical input power and a phase difference (<inline-formula> <tex-math notation="LaTeX">$Delta varphi$ </tex-math></inline-formula>) are connected to the input and isolated ports of the BQC. A detailed theoretical analysis is carried out. To validate the proposed scheme, we design a broadband (1.6–2.8 GHz) WIA rectifier. Measurement results show that the power conversion efficiency (PCE) exceeded 60% in the frequency range from 1.6 to 2.8 GHz at 13.1 dBm of the input power. Additionally, at 2.45 GHz, the PCE varies in the range of 60.8% and 72.6% within the entire <inline-formula> <tex-math notation="LaTeX">$Delta varphi $ </tex-math></inline-formula> range (0°–360°). Thus, the obtained PCE variation (<inline-formula> <tex-math notation="LaTeX">$Delta eta$ </tex-math></inline-formula>) is 11.8%. Considering its excellent broadband and WIA features, it is very suitable for high-efficiency radio-frequency (RF) energy harvesting (RFEH) systems.
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A Broadband 10–43-GHz High-Gain LNA MMIC Using Coupled-Line Feedback in 0.15-<italic>μ</italic>m GaAs pHEMT Technology
Xu YanPengyu YuJingyuan ZhangSi-Ping GaoYongxin Guo
Keywords:Noise measurementGain measurementPHEMTsWidebandGallium arsenideCouplingsBroadband communicationcircuit tuningcoupled transmission linesfeedback amplifiersfield effect MIMICfield effect MMICgallium arsenideHEMT integrated circuitsIII-V semiconductorsintegrated circuit designlow noise amplifiersmillimetre wave amplifiersMMIC amplifierswideband amplifiers2.4-3.0-dB noise figurearm lengthbandpass characteristicbandwidth 33.0 GHzbroadband high-gain LNA MMICcenter frequencycompensated gain roll-offcoupled-line feedbackcoupling factorCS architecturesE-mode pseudomorphic high electron mobility transistor technologyfrequency 10 GHz to 43 GHzGaAs/intgain 1.0 dBLNA circuitLNA prototypelow-noise amplifier monolithic microwave integrated circuit designnoise figure 2.4 dB to 3.0 dBnovel coupled-line-based positive feedback structurepHEMT technologypower 110.0 mWsize 0.15 mumthree-stage common-source architecturesCoupled-line (CL) feedbackGaAs pseudomorphic high electron mobility transistor (pHEMT)high gainlow-noise amplifier (LNA)wideband
Abstracts:In this letter, a 10–43-GHz low-noise amplifier (LNA) monolithic microwave integrated circuit (MMIC) is designed in a commercial 0.15-<inline-formula> <tex-math notation="LaTeX">$mu text{m}$ </tex-math></inline-formula> GaAs E-mode pseudomorphic high electron mobility transistor (pHEMT) technology. In the proposed LNA circuit, a novel coupled-line (CL)-based positive feedback structure is employed with the bandpass characteristic. By carefully tuning its coupling factor and arm length, the center frequency <inline-formula> <tex-math notation="LaTeX">$f_{c}$ </tex-math></inline-formula> and the intensity of the feedback can be controlled, respectively. Subsequently, targeting <inline-formula> <tex-math notation="LaTeX">$f_{c}$ </tex-math></inline-formula> at the higher cutting edge of the working band leads to compensated gain roll-off and extended bandwidth. Incorporating three-stage common-source (CS) architectures, an LNA prototype is fabricated with a size of 1.05 mm2 including pads. Under 2-V voltage drain drain (VDD), good performance is obtained, including 24.6-dB peak gain with 3-dB bandwidth of 33 GHz, 2.4–3.0-dB noise figure (NF), 54.5 ± 13.8-ps group delay, and 12.3/21.5-dBm best output power at 1 dB gain compression (OP1dB)/output third order intercept point (OIP3). The total dc power is 110 mW.
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A 5.9 mW E-/W-Band SiGe-HBT LNA With 48 GHz 3-dB Bandwidth and 4.5-dB Noise Figure
Eren VardarliPaulius SakalasMichael Schröter
Keywords:Noise measurementGain measurementTransmission line measurementsImpedance matchingFrequency measurementWidebandHeterojunction bipolar transistorsBiCMOS analogue integrated circuitsbipolar MIMICbipolar transistor circuitscarbonGe-Si alloysheterojunction bipolar transistorsimpedance matchingintegrated circuit designlow noise amplifiersmillimetre wave amplifiersmillimetre wave bipolar transistorsQ-factorsemiconductor materialsbase-collector junctionconstant quality factor curvesE-band HBT LNAforward biasingfrequency 62.0 GHz to 110.0 GHzgain 13.5 dBimpedance matching techniquelow-power operationmillimeter-wave two-stage common-emitter low noise amplifiermm-wave radarnoise figure 4.5 dBpower 5.9 mWrelativity flat gainSiGe:C/intsilicon-based E-band LNAssilicon-based W-band LNAssilicon-germanium-carbon bipolar CMOS technologyT-type input matching networktwo-stage broadband noisetwo-stage common-emittervoltage 0.7 VW-band HBT LNAwideband performancewireless communication applications3-dB bandwidthE-bandlow noise amplifier (LNA)low-voltage operationmillimeter-wave (mm-wave) circuit designnoise figure (NF)silicon-germanium (SiGe)-heterojunction bipolar transistor (HBT)W-band
Abstracts:The theory, design, and implementation of a millimeter-wave (mm-wave) two-stage common-emitter (CE) low noise amplifier (LNA) using a 130-nm silicon-germanium (SiGe):C Bipolar CMOS technology is presented. The LNA was optimized for wideband performance from 62 to 110 GHz for both mm-wave radar/sensing and wireless communication applications. A two-stage broadband noise and impedance matching technique is used to obtain a relativity flat gain (13.5 dB) and noise figure (NF) (4.5 dB) across the E-/W-band. Low-voltage <inline-formula> <tex-math notation="LaTeX">$(V_{text {CC}}=0.7,,text {V})$ </tex-math></inline-formula> and low-power (5.9 mW) operation is achieved by forward biasing the base–collector junction, while the wideband capability is further improved by a T-type input matching network utilizing constant quality factor curves. To the best of authors’ knowledge, the presented LNA has the widest 3-dB bandwidth with the lowest power consumption in the literature for silicon-based E-/W-band LNAs.
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A 230-GHz Endfire SIS Mixer With Near Quantum-Limited Performance
John D. GarrettBoon-Kok TanChristine ChaumontFaouzi BoussahaGhassan Yassin
Keywords:MixersOptical waveguidesRadio frequencyOptical receiversJunctionsPerformance evaluationOptical mixingMillimeter wave communicationSuperconductorsTunnelingRadio astronomyaluminium compoundsfocal planesniobiumsuperconductor-insulator-superconductor mixerswaveguide transitionsconventional radial probe mixersendfire SIS mixerendfire superconductor-insulator-superconductorfinline mixerfrequency 210.0 GHz to 260.0 GHzfrequency 230.0 GHzlarge-format focal plane arraysmixer chipNb-AlAlOx-Nb/intquantum limitSIS mixing elementsunilateral finlinewaveguide structurewaveguide-to-planar circuit transitionMillimeter wave devicesradio astronomyreceiverssuperconductive tunneling
Abstracts:In this letter, we report the near quantum-limited performance of a 230 GHz endfire superconductor-insulator-superconductor (SIS) mixer utilizing a Nb/Al-AlOx/Nb trilayer. An important feature of this mixer is its use of a unilateral finline for the waveguide-to-planar circuit transition, which allows for a wide radiofrequency (RF) bandwidth, a simple waveguide structure with easy alignment, and for the mixer chip to be aligned along the optical axis. Each of these factors is beneficial in the construction of large-format focal plane arrays. We tested the new finline mixer from 210 to 260 GHz in a liquid helium cryostat at ~4 K. The best recorded noise temperature was approximately twice the quantum limit, which is comparable to conventional radial probe mixers. This suggests that endfire SIS mixers can be used in large format arrays, comprising 100s or even 1000s of SIS mixing elements, while retaining state-of-the-art quantum mixing performance.
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A Millimeter-Wave Variable-Gain Power Amplifier With P₁ dB Improvement Technique in 65-nm CMOS
Xiongyao LuoWenjie FengHaoshen ZhuLiang WuWenquan CheQuan Xue
Keywords:Gain measurement5G mobile communicationWireless communicationPower generationLogic gatesFrequency measurementTransistorsCMOS analogue integrated circuitsdistortionfield effect MIMICfield effect MMICmillimetre wave power amplifiersMMIC power amplifiersAM-AM distortionamplitude-to-amplitude distortionCMOS processefficiency 29.5 percentefficiency 34 percentfrequency 23.1 GHz to 29.0 GHzgain adjustmenthigh output power compression pointmillimeter-wave variable-gain power amplifierMMW VGPAPDPApeaking-mode gain response shapingpostdistortion power amplifierpostdistortion techniquepower added efficiencysize 65 nmvariable gainCMOSfifth generation (5G)millimeter wave (MMW)postdistortionvariable-gain power amplifier (VGPA)
Abstracts:A millimeter-wave (MMW) variable-gain power amplifier (VGPA) with <inline-formula> <tex-math notation="LaTeX">$P_{mathrm {1,dB}}$ </tex-math></inline-formula> improvement technique is proposed. The proposed VGPA consists of a postdistortion power amplifier (PDPA) and a variable-gain amplifier (VGA), for realizing high output power 1-dB compression point (<inline-formula> <tex-math notation="LaTeX">$P_{mathrm {1,dB}}$ </tex-math></inline-formula>) and variable gain, respectively. To improve the <inline-formula> <tex-math notation="LaTeX">$P_{mathrm {1,dB}}$ </tex-math></inline-formula> performances, a postdistortion technique with peaking-mode gain response shaping is proposed. This new approach has less amplitude-to-amplitude (AM–AM) distortion. Fabricated in 65-nm CMOS process, the proposed VGPA achieves 16-dBm output <inline-formula> <tex-math notation="LaTeX">$P_{mathrm {1,dB}}$ </tex-math></inline-formula> with 29.5% power added efficiency (PAE) and 16.7-dBm saturated output power (<inline-formula> <tex-math notation="LaTeX">$P_{mathrm {sat}}$ </tex-math></inline-formula>) with 34% peak PAE. The maximum gain reaches 33.1 dB with 3-dB bandwidth from 23.1 to 29 GHz and 31.1-dB dynamic range of gain adjustment.
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Miniaturized Dual-Band Filter Using Dual-Mode Dielectric Waveguide Resonator
Zuoyu XuYongle WuQingxiang DongWeimin Wang
Keywords:Dual bandBand-pass filtersCouplingsDielectricsPassbandWireless communicationband-pass filterscoatingsdielectric resonatorsdielectric waveguidessilverwaveguide filtersAg/intcascaded trisection unitcoatingCT unitcylinder dielectric blockcylinder DWRdual-band bandpass filterdual-band BPFdual-mode dielectric waveguide resonatorminiaturized dual-band filterTM010 modesTM011 modestransmission zeroTZBandpass filter (BPF)dielectric waveguide resonator (DWR)dual-banddual-modeminiaturization
Abstracts:This letter presents a novel miniaturized dual-band bandpass filter (BPF) using a dual-mode dielectric waveguide resonator (DWR). The DWR is a cylinder dielectric block with the surface being silver-coated. The two modes are TM010 and TM011 modes, which are used to construct the two passbands. The frequency of them can be adjusted by changing the radius and the height of the cylinder DWR and the frequency space can be controlled independently. The BPF is composed of three cylindrical cavities, which are arranged in an equilateral triangle. The three cavities construct a cascaded trisection (CT) unit, which creates a transmission zero (TZ) at the upper side of the two passbands. Finally, a dual-band BPF using DWR is simulated, manufactured, and measured to exhibit the feasibility of the proposed design. Their results are in good agreement, showing good performance, such as miniaturization, good return loss (RL), and upper stopband selectivity.
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Vertical Waveguide-to-Microstrip Self-Diplexing Transition for Dual-Band Applications
Emilio ArnieriFrancesco GrecoLuigi BocciaGiandomenico Amendola
Keywords:Waveguide transitionsMicrostripDual bandBandwidthLoss measurementInsertion lossSubstratesMillimeter wave communicationmicrostrip transitionsprinted circuit manufactureprinted circuitsrectangular waveguidesdual-band applicationsdual-band self-diplexing operationH-shaped slotsK frequency bandKa frequency bandlower bandsmass productionmetalized via holesparasitic patchespower leakage preventionradiating patchesrectangular waveguideself-diplexing operationstandard printed circuit board manufacturing processingstandard waveguideupper bandsvertical waveguide-to-microstrip self-diplexing transitionDual-bandmicrostrip-to-waveguide transitionmillimeter-wavePCBsubstrate-integrated waveguide (SIW)
Abstracts:This letter presents a novel vertical waveguide-to-microstrip self-diplexing transition for dual-band applications. The transition is realized with standard printed circuit board (PCB) manufacturing processing, making it suitable for mass production and practical applications. A standard waveguide is screwed on the topside of the stack-up. Dual-band self-diplexing operation is achieved by coupling two microstrips (one for each band) to two radiating patches through H-shaped slots. The operating bandwidth has been enhanced by adding two parasitic patches above the radiating ones. Metalized via holes are used to form a cage around the rectangular waveguide and the microstrips to prevent power leakage. A prototype has been fabricated to operate at K/Ka frequency band. The experimental results show a −10 dB matching bandwidth of 20% and 14% for the lower and upper bands, respectively. Within these ranges, the maximum measured insertion loss is about 0.6 and 0.7 dB, respectively.
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A Broadband <italic>Ka</italic>-Band Waveguide Magic-T With Compact Inner Ridge Matching
Song GuoKaijun SongLi QianXinjun Zou
Keywords:Ports (computers)Power dividersBroadband communicationStriplineLoss measurementWireless communicationBandwidthridge waveguidesstrip linesbroadband isolation characteristicsbroadband Ka-band waveguide magic-Tbroadband matchingcollinear portscompact inner ridge matchingcompact sizedeference portsdesign processgrounded suspended striplinehigh-power applicationsinner ridge-matching structurenoise figure 37.5 dBpower capacitywaveguide BJ-320 waveguide operating bandwidthInner ridgemagic-Tsuspended stripline
Abstracts:In this letter, a broadband waveguide magic-T with compact size is presented. A grounded suspended stripline has been used to obtain broadband isolation characteristics and increase power capacity. The inner ridge-matching structure is used to achieve broadband matching. The method and design process of the demonstrated magic-T are described in detail. The measured 15-dB bandwidth is about 30.3%, almost for waveguide BJ-320 waveguide operating bandwidth. The measured isolation between sum and deference ports is above 37.5 dB; 20-dB measured isolation is achieved between collinear ports. The measured and simulated results are in good agreement. It has advantages in high-power applications.
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Current Source Implementations for the HIE-FDTD Methods
Ankit Kumar PandeyAlok Kumar Saxena
Keywords:IndexesTime-domain analysisFinite difference methodsStability criteriaPower system stabilityJammingWireless communicationfinite difference time-domain analysisADI-FDTD methodalternating direction implicit finite-difference time-domain methodcurrent source implementationsfield errorsimplicit-explicit finite-difference time-domainimproved HIE-FDTDleapfrog HIE-FDTD methodstime index parametersCurrent source implementationsfinite-difference time-domain (FDTD) methodhybrid implicit–explicit (HIE) schemeleapfrog algorithm
Abstracts:In this letter, the current source implementations are presented for the hybrid implicit–explicit finite-difference time-domain (HIE-FDTD), the improved HIE-FDTD, and the leapfrog HIE-FDTD methods. The asymmetry and the field errors of these HIE-FDTD methods are investigated for all possible values of the time index parameters. The proposed implementations give very low asymmetry and field errors for all the three HIE–FDTD methods. The field errors given by these HIE-FDTD methods are lower than those given by the alternating direction implicit finite-difference time-domain (ADI-FDTD) method.