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High frequency resistive switching behavior of amorphous TiO₂ and NiO

Senad Bulja, Rose Kopf, Al Tate, Mark Cappuzzo, Dmitry Kozlov, Holger Claussen, Dirk Wiegner, Wolfgang Templ, Dariush Mirshekar-Syahkal

Sci Rep. 2022; 12: 13804. Published online 2022 Aug 13. doi: 10.1038/s41598-022-16907-8

PMCID:: PMC9376065

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Exploitation of response surface method for the optimization of RF-MEMS reconfigurable devices in view of future beyond-5G, 6G and super-IoT applications

Jacopo Iannacci, Girolamo Tagliapietra, Alessio Bucciarelli

Sci Rep. 2022; 12: 3543. Published online 2022 Mar 3. doi: 10.1038/s41598-022-07643-0

PMCID:: PMC8894374

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Dynamic-quenching of a single-photon avalanche photodetector using an adaptive resistive switch

Jiyuan Zheng, Xingjun Xue, Cheng Ji, Yuan Yuan, Keye Sun, Daniel Rosenmann, Lai Wang, Jiamin Wu, Joe C. Campbell, Supratik Guha

Nat Commun. 2022; 13: 1517. Published online 2022 Mar 21. doi: 10.1038/s41467-022-29195-7

PMCID:: PMC8938474

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An X-band Bi-Directional Transmit/Receive Module for a Phased Array System in 65-nm CMOS

Van-Viet Nguyen, Hyohyun Nam, Young Joe Choe, Bok-Hyung Lee, Jung-Dong Park

Sensors (Basel) 2018 Aug; 18(8): 2569. Published online 2018 Aug 6. doi: 10.3390/s18082569

PMCID:: PMC6112044

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Flexible Thermo-Optic Variable Attenuator based on Long-Range Surface Plasmon-Polariton Waveguides

Jie Tang, Yi-Ran Liu, Li-Jiang Zhang, Xing-Chang Fu, Xiao-Mei Xue, Guang Qian, Ning Zhao, Tong Zhang

Micromachines (Basel) 2018 Aug; 9(8): 369. Published online 2018 Jul 26. doi: 10.3390/mi9080369

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Nanosecond resistive switching in Ag/AgI/PtIr nanojunctions

Botond Sánta, Dániel Molnár, Patrick Haiber, Agnes Gubicza, Edit Szilágyi, Zsolt Zolnai, András Halbritter, Miklós Csontos

Beilstein J Nanotechnol. 2020; 11: 92–100. Published online 2020 Jan 8. doi: 10.3762/bjnano.11.9

PMCID:: PMC6964644

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Augmented reality with image registration, vision correction and sunlight readability via liquid crystal devices

Yu-Jen Wang, Po-Ju Chen, Xiao Liang, Yi-Hsin Lin

Sci Rep. 2017; 7: 433. Published online 2017 Mar 27. doi: 10.1038/s41598-017-00492-2

PMCID:: PMC5428510

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Amplitude-Phase Variation in a Graphene-Based Microstrip Line

Muhammad Yasir, Sergej Fatikow, Olaf C. Haenssler

Micromachines (Basel) 2022 Jul; 13(7): 1039. Published online 2022 Jun 30. doi: 10.3390/mi13071039

PMCID:: PMC9322433

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A CMOS–memristor hybrid system for implementing stochastic binary spike timing-dependent plasticity

Javad Ahmadi-Farsani, Saverio Ricci, Shahin Hashemkhani, Daniele Ielmini, Bernabé Linares-Barranco, Teresa Serrano-Gotarredona

Philos Trans A Math Phys Eng Sci. July 25, 2022; 380(2228): 20210018. Published online June 6, 2022. doi: 10.1098/rsta.2021.0018

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Discussion and Demonstration of RF-MEMS Attenuators Design Concepts and Modules for Advanced Beamforming in the Beyond-5G and 6G Scenario—Part 1

Girolamo Tagliapietra, Flavio Giacomozzi, Massimiliano Michelini, Romolo Marcelli, Giovanni Maria Sardi, Jacopo Iannacci

Sensors (Basel) 2024 Apr; 24(7): 2308. Published online 2024 Apr 5. doi: 10.3390/s24072308

PMCID:: PMC11014151

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A Multimode 28 GHz CMOS Fully Differential Beamforming IC for Phased Array Transceivers

Ayush Bhatta, Jeongsoo Park, Donghyun Baek, Jeong-Geun Kim

Sensors (Basel) 2023 Jul; 23(13): 6124. Published online 2023 Jul 3. doi: 10.3390/s23136124

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Bridging the Gap Between Nanowires and Josephson Junctions: A Superconducting Device Based on Controlled Fluxon Transfer

E. Toomey, M. Onen, M. Colangelo, B. A. Butters, A. N. McCaughan, K. K. Berggren

Phys Rev Appl. Author manuscript; available in PMC 2020 Mar 12.

Published in final edited form as: Phys Rev Appl. 2019; 11(3): 10.1103/physrevapplied.11.034006. doi: 10.1103/physrevapplied.11.034006

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Comparative High Voltage Impulse Measurement

Gerald J. FitzPatrick, Edward F. Kelley

J Res Natl Inst Stand Technol. 1996 Sep-Oct; 101(5): 639–658. doi: 10.6028/jres.101.063

PMCID:: PMC4907613

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A Subnanosecond Electric Pulse Exposure System for Biological Cells

Shu Xiao, Iurii Semenov, Ross Petrella, Andrei G. Pakhomov, Karl H. Schoenbach

Med Biol Eng Comput. Author manuscript; available in PMC 2018 Jul 1.

Published in final edited form as: Med Biol Eng Comput. 2017 Jul; 55(7): 1063–1072. Published online 2016 May 13. doi: 10.1007/s11517-016-1516-7

PMCID:: PMC5884115

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Approaching microwave photon sensitivity with Al Josephson junctions

Andrey L Pankratov, Anna V Gordeeva, Leonid S Revin, Dmitry A Ladeynov, Anton A Yablokov, Leonid S Kuzmin

Beilstein J Nanotechnol. 2022; 13: 582–589. Published online 2022 Jul 4. doi: 10.3762/bjnano.13.50

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Inductive Coupling of Bipolar Signals with a Conjugate Coil Pair for an Analog Passive ECG Sensor Using a PPy-Coated pvCNT Dry Electrodes

Mohammad Abu-Saude, Bashir I. Morshed

Sensors (Basel) 2023 Jun; 23(11): 5283. Published online 2023 Jun 2. doi: 10.3390/s23115283

PMCID:: PMC10256043

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Middle ear function and cochlear input impedance in chinchilla

Michaël C. C. Slama, Michael E. Ravicz, John J. Rosowski

J Acoust Soc Am. 2010 Mar; 127(3): 1397–1410. doi: 10.1121/1.3279830

PMCID:: PMC2856507

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Analysis of exosome purification methods using a model liposome system and tunable-resistive pulse sensing

Rebecca E. Lane, Darren Korbie, Will Anderson, Ramanathan Vaidyanathan, Matt Trau

Sci Rep. 2015; 5: 7639. Published online 2015 Jan 6. doi: 10.1038/srep07639

PMCID:: PMC4648344

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Artificial optoelectronic spiking neuron based on a resonant tunnelling diode coupled to a vertical cavity surface emitting laser

Matěj Hejda, Ekaterina Malysheva, Dafydd Owen-Newns, Qusay Raghib Ali Al-Taai, Weikang Zhang, Ignacio Ortega-Piwonka, Julien Javaloyes, Edward Wasige, Victor Dolores-Calzadilla, José M. L. Figueiredo, Bruno Romeira, Antonio Hurtado

Nanophotonics. 2023 Mar; 12(5): 857–867. Published online 2022 Nov 15. doi: 10.1515/nanoph-2022-0362

PMCID:: PMC9995654

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Fast Negative Feedback Enables Mammalian Auditory Nerve Fibers to Encode a Wide Dynamic Range of Sound Intensities

Mark Ospeck

PLoS One. 2012; 7(3): e32384. Published online 2012 Mar 8. doi: 10.1371/journal.pone.0032384

PMCID:: PMC3297600

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PMC Images search for resistive attenuator

Figure 3

Comparison of the measured and simulated S-parameters characteristics of the 1-bit series (a,b) and shunt (c,d) RF-MEMS attenuators from 1 to 30 GHz. S21 (a) and VSWR (b) of the series attenuator, when the resistive load is inserted (switch OFF) and shorted (switch ON). S21 (c) and VSWR (d) of the shunt attenuator, when the resistive load is inserted (switch ON) and not inserted (switch OFF). Images created with Microsoft Office 365 Excel (www.office.com).

Exploitation of response surface method for the optimization of RF-MEMS reconfigurable devices in view of future beyond-5G, 6G and super-IoT applications

Sci Rep. 2022;12:3543.
Figure 10

A schematic of the Pi-type resistive attenuator cell (a) and simplified models of it in the OFF (b) and ON (c) states.

An X-band Bi-Directional Transmit/Receive Module for a Phased Array System in 65-nm CMOS

Sensors (Basel). 2018 Aug;18(8):2569.
Figure 21

Reflective-type variable attenuator (RTVA) based on TiO₂.

High frequency resistive switching behavior of amorphous TiO2 and NiO

Sci Rep. 2022;12:13804.
Figure 2

Simplified circuit diagram that shows the main components for down-conversion and digitization of the sensed RF signal. The sensed signal is connected to the RF mixer (AD8605) through a lattice balun (L_bC_b network) followed by a Wilkinson power splitter (L_sC_s network) and a resistive tee attenuator (R_A1i network). The power splitter fed part of the signal back to the envelope detector (ADL5511) for current source operation. The differential mixer output is connected to a single-ended input of the ADC (AD7277) through an active balun that consisted of an op-amp stage (AD8605), which was also an effective low-pass filter for the sum frequency (594.2 MHz). The digitized down converted RF was sent to the fiber optical transmitter (AFBR-1624Z).

Optically Controlled On-Coil Amplifier with RF Monitoring Feedback

Magn Reson Med. ;79(5):2833-2841.