rejection ratio
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Electronics ◽  
2021 ◽  
Vol 10 (14) ◽  
pp. 1613
Author(s):  
Waldemar Jendernalik ◽  
Jacek Jakusz ◽  
Robert Piotrowski ◽  
Grzegorz Blakiewicz ◽  
Stanisław Szczepański

A voltage unity-gain zero-offset CMOS amplifier with reduced gain error and increased PSRR (power supply rejection ratio) is proposed. The amplifier uses two feed mechanisms, negative feedback and supporting positive feedforward, to achieve low deviation from unit gain over the entire input range. The circuit, designed in a standard 180-nanometer 1.8-voltage CMOS process, is compared with two known buffers of similar topology, also designed in the same process. Simulations show that, with the same supply (1.8 V), power (1.2 mW), load (12 pF), bandwidth (50 MHz), and similar area (600 µm2), the proposed buffer achieves the lowest gain error (0.3%) and the highest PSRR (72 dB).


2021 ◽  
Author(s):  
Prateek Jain ◽  
Shambhu Dayal Sharma ◽  
Amit M. Joshi

Abstract In this paper, CMOS based optimized two stage differential amplifier circuit for convenient biomedical signal conditioning system is presented. A low-power, low noise & high CMRR differential amplifier is designed for portable ECG signal conditioning using MOS based low pass filter with stacked transistors. The stack transistors with MOS which is connected at output terminal optimize the design for ECG signal conditioning and other biomedical device signal conditioning. The presented amplifier is designed with standard 45nm CMOS process technology at a 0.85 V supply voltage. The simulation results are derived using Cadence Analog Virtuoso Spectre Simulator. The simulation results show that the presented differential amplifier has a common-mode rejection ratio (CMRR) of 178dB at 100Hz, power supply rejection ratio (PSRR) of 68 dB and power dissipation of 1.5μW. The input referred (IR) noise is 3.83μV/√f and slew rate is 11volt/μsec. These obtained performance parameters is better and efficient compared to conventional differential amplifier. The noise performance is improved using proposed design compared to previous designed differential amplifier.


Membranes ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 304
Author(s):  
Qingxiu Miao ◽  
Yaoling Zhang ◽  
Shuo Cong ◽  
Fei Guo

Membrane distillation (MD) processes need a relatively mild temperature gradient as the driving force for desalination. In the field, it is reasonable to utilize solar energy as the heat source for the feed, and seawater as the infinite cold source for condensation. Solar-driven MD provides a route for the practical application of seawater desalination at a small scale. In this work, we focus on floating MD modules with a solar heating bag as the power source, and perform proof-of-principle experiments on the MD performance under various conditioning parameters, including feed flow rate, feed temperature, salinity, air gap, and sea waves. The results indicate that floating solar-driven MD modules are feasible in terms of permeate flux and salt rejection ratio, and the upward evaporation MD configuration leads to a better performance in terms of permeate flux. The simulation and experiments also show that the natural sea waves disturb the heating bag and the MD module floating on the surface of seawater, and effectively enhance the feed circulation and transport in the system.


Sensors ◽  
2021 ◽  
Vol 21 (8) ◽  
pp. 2711
Author(s):  
Shilpa Mehta ◽  
Xue-Jun Li ◽  
Massimo Donelli

A reconfigurable gm-boosted, image-rejected downconversion mixer is presented in this paper using the SiGe 8 HP technology. The proposed mixer operates within 0.9–13.5 GHz that is suitable for software-defined radio applications. The conversion mixer comprises of resistive biased radio frequency (RF) section, double balanced Gilbert cell mixer core sections divided as per I and Q stages for image-rejection purpose, inductively peaked gm-boosting section and tunable filter section, respectively. In comparison to previous works in the scientific literature, the design shows enhanced conversion gain (CG), noise figure (NF), and image-rejection ratio (IRR). For the entire band of operation, the mixer attains a good return loss |S11| of <−10 dB. Additionally, the design accomplishes an excellent CG of 22 dB, NF of 2.5 dB, and an image-rejection ratio of 30.2 dB at maximum frequency. Finally, a third-order intercept point (IP3) of −3.28 dBm and 1 dB compression point (CP1) of −13 dBm, respectively, shows moderate linearity performance.


2021 ◽  
Vol 2021 ◽  
pp. 1-6
Author(s):  
Kin-Tak Lam ◽  
Sheng-Joue Young ◽  
Yen-Lin Chu ◽  
Chi-Nan Tsai ◽  
Tung-Te Chu ◽  
...  

In this study, metal–semiconductor–metal-structured ultraviolet (UV) photodetectors (PDs) based on pure zinc oxide (ZnO) and amorphous indium gallium zinc oxide (a-IGZO) thin films were fabricated and characterized. The ZnO seed layers were deposited on Corning glass substrates via a radio frequency (RF) magnetron sputtering technique. Results showed that under a 5 V applied bias; the dark currents of the pure ZnO and a-IGZO thin films were 0.112 pA and 2.85 nA, respectively. Meanwhile, the UV-to-visible rejection ratio of the pure ZnO and a-IGZO thin films were 14.33 and 256, respectively. Lastly, the PDs of thea-IGZO thin films had a lower leakage current and higher rejection ratio than that of the pure ZnO thin films from the UV to visible light region.


Electronics ◽  
2021 ◽  
Vol 10 (5) ◽  
pp. 631
Author(s):  
Wei-Lun Huang ◽  
Sheng-Po Chang ◽  
Cheng-Hao Li ◽  
Shoou-Jinn Chang

In this thesis, Aluminum-Gallium-Zinc oxide (AGZO) photo thin film transistors (PTFTs) fabricated by the co-sputtered method are investigated. The transmittance and absorption show that AGZO is highly transparent across the visible light region, and the bandgap of AGZO can be tuned by varying the co-sputtering power. The AGZO TFT demonstrates high performance with a threshold voltage (VT) of 0.96 V, on/off current ratio of 1.01 × 107, and subthreshold swing (SS) of 0.33 V/dec. Besides, AGZO has potential for solar-blind applications because of its wide bandgap. The AGZO PTFT of this research can achieve a rejection ratio of 4.31 × 104 with proper sputtering power and a rising and falling time of 35.5 s and 51.5 s.


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