P-4: Electro Static Discharge Effects on Polysilicon TFTs for AMLCD

2002 ◽  
Vol 33 (1) ◽  
pp. 212 ◽  
Author(s):  
Seung-Chul Lee ◽  
Byung-Chul Jeon ◽  
Kook-Chul Moon ◽  
Min-Cheol Lee ◽  
Min-Koo Han
Keyword(s):  
Static Discharge

Effects of immobilizing the cat peroneus longus muscle on the activity of its own spindles

1993 ◽  
Vol 75 (6) ◽  
pp. 2629-2635 ◽  
Author(s):  
M. Gioux ◽  
J. Petit
Keyword(s):  
Short Length ◽  
Full Extension ◽  
Peroneus Longus ◽  
Longus Muscle ◽  
Muscle Compliance ◽  
Muscle Spindle Endings ◽  
Static Discharge ◽  
Distal Tendon ◽  
Stimulation Of

The peroneus longus muscle of 10 cats were immobilized by fixating the distal tendon on the fibula at one of two length: neutral (length for a 90 degrees flexion of the ankle joint; 5 cats) or short (length for a full extension of the joint; 5 cats). Spindle afferent discharges were studied after 2 (4 cats) or 5 wk (6 cats) of immobilization and compared with those of four control animals. In each muscle, the discharges of nearly all primary and one of secondary muscle spindle endings were recorded during 2-mm ramp-and-hold stretches applied at different initial muscle lengths. A very slight increase in both the static discharge and the dynamic index of primary endings was observed in passive spindles. The increase in connective tissue that occurs in immobilized muscle and reduces muscle compliance was likely the sole alteration responsible for this constant effect. The responses to stretches of primary endings during stimulation of static and dynamic gamma-axons were not altered. Muscle immobilization at short length, even if spindle properties are not altered, can be expected to reduce the overall amount of group Ia afferent impulses with possible long-term changes on motoneuron properties.

Research on reducing electro-static discharge of tearing film of EPD

2021 ◽  
Author(s):  
Haowei Zou ◽  
Xin Li ◽  
Yong Song ◽  
Hanqing Liu ◽  
Junru Ma ◽  
...  
Keyword(s):  
Static Discharge

Microstructure and Electrical Properties of AZO Films Prepared by RF Magnetron Sputtering

2011 ◽  
Vol 264-265 ◽  
pp. 754-759 ◽  
Author(s):  
Bakri Jufriadi ◽  
Agus Geter E. Sutjipto ◽  
R. Othman ◽  
R. Muhida
Keyword(s):  
Magnetron Sputtering ◽  
Deposition Time ◽  
Transparent Conducting Oxide ◽  
Rf Magnetron Sputtering ◽  
Flat Panel Displays ◽  
Emi Shielding ◽  
Transparent Conducting ◽  
Deposition Processes ◽  
Electro Magnetic ◽  
Static Discharge

AZO is an ideal replacement transparent conducting oxide (TCO) for ITO to all corresponding applications. The typical applications include: transparent electrodes for solar cells, flat panel displays, LCD electrodes, electro-magnetic compatibility (RF-EMI shielding) coatings, touch panel transparent contacts, static discharge dissipation. The production of useful and commercially attractive thin films using different deposition processes is very important parameter to investigate. A systematic study of the sputtering condition and their influenced on electrical and structural were studied. In this work, AZO films were deposited by RF magnetron sputtering at 200 °C. The result shows that the deposited time has influenced the characteristic of deposited AZO films. For a longer deposition time, thin film shows a uniform grain growth. The resistivity found minimum at the deposition time of 45 minutes. It can be considered that by reducing of the grain boundaries which enable the electron carries to conduct smoothly.

Device Design Issues for Electro-static Discharge Suppression Based on the Monitoring of the Lattice Temperature

2005 ◽  
Author(s):  
Gwang-hyeon Lim ◽  
Kwang-dong Yoo ◽  
Joo-hyun Jin ◽  
Sun-kwon Lim ◽  
Kyu-hyun Choi
Keyword(s):  
Lattice Temperature ◽  
Device Design ◽  
Design Issues ◽  
Static Discharge ◽  
Discharge Suppression

Electro-static discharge ignition of monolayers of nanocomposite thermite powders prepared by Arrested Reactive Milling

2015 ◽  
Vol 1758 ◽  
Author(s):  
Ian Monk ◽  
Rayon Williams ◽  
Xinhang Liu ◽  
Edward L. Dreizin
Keyword(s):  
Particle Surface ◽  
Combustion Products ◽  
Reaction Rates ◽  
Interference Filter ◽  
Gas Combustion ◽  
Reactive Milling ◽  
Discharge Ignition ◽  
Reactive Interface ◽  
Arrested Reactive Milling ◽  
Static Discharge

AbstractReactive nanocomposite powders with compositions 2Al∙3CuO, 2.35Al∙Bi2O3, 2Al∙Fe2O3, and 2Al∙MoO3 were prepared by arrested reactive milling, placed in monolayers on a conductive substrate and ignited by an electro-static discharge (ESD) or spark in air, argon, and vacuum. The ESD was produced by discharging a 2000 pF capacitor charged to a voltage varied from 5 to 20 kV. Emission from ignited particles was monitored using a photomultiplier equipped with an interference filter. Experimental variables included particle sizes, milling time used to prepare composite particles, surrounding environment, and starting ESD voltage. All materials ignited in all environments, producing individual burning particles that were ejected from the substrate. The spark duration varied from 1 to 5 µs; the duration of the produced emission pulse was in the range of 80 – 250 µs for all materials studied. The longest emission duration was observed for the nanocomposite thermite using MoO3 as an oxidizer. The reaction rates of the ESD-initiated powders were defined primarily by the scale of mixing of and reactive interface area between the fuel and oxidizer in composite materials rather than by the external particle surface or particle dimensions. In vacuum, particles were heated by ESD while remaining on the substrate until they began generating gas combustion products. In air and argon, particles initially pre-heated by ESD were lifted and accelerated to ca. 100 m/s by the generated shock wave; the airborne particles continued self-heating due to heterogeneous redox reactions.

Accurate Modeling Methodology of Laterally Diffused Metal-Oxide Semiconductor Leakage Current for Electro-Static Discharge Protection Circuit Design

2021 ◽  
Vol 21 (8) ◽  
pp. 4230-4234
Author(s):  
Jun Hyeok Kim ◽  
Su Min Lee ◽  
Chan Ho Park
Keyword(s):  
Metal Oxide ◽  
Leakage Current ◽  
Measurement Data ◽  
Metal Oxide Semiconductor ◽  
Oxide Semiconductor ◽  
Modeling Methodology ◽  
Trap Assisted Tunneling ◽  
Protection Circuit ◽  
Current Characteristics ◽  
Static Discharge

A modeling method using juncap2 physical compact model with SRH (Shockley-Read-Hall), TAT (Trap-Assisted-Tunneling), BBT (Band-to-Band Tunneling) effects is presented for the leakage current in a laterally diffused metal-oxide semiconductor (LDMOS). The juncap2 model is successfully combined with BSIM4 model and it is validated with measurement data. The model accurately predicts the leakage current characteristics for the entire bias region and temperature.

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