Profiling interface traps in MOS transistors by the DC current-voltage method

1996 ◽  
Vol 17 (2) ◽  
pp. 72-74 ◽  
Author(s):  
Chih-Tang Sah ◽  
A. Neugroschel ◽  
K.M. Han ◽  
J.T. Kavalieros
2013 ◽  
Vol 740-742 ◽  
pp. 533-536 ◽  
Author(s):  
Viktoryia Uhnevionak ◽  
Christian Strenger ◽  
Alex Burenkov ◽  
Vincent Mortet ◽  
Elena Bedel-Pereira ◽  
...  

4H-SiC n-channel lateral MOSFETs were manufactured and characterized electrically by current-voltage measurements and by numerical simulation. To describe the observed electrical characteristics of the SiC MOSFETs, Near-Interface Traps (NIT) and mobility degradation models were included in the simulation. The main finding of the simulation is that two models for the NIT states in the upper part of the SiC bandgap are able to describe the electrical data equally well. In one of them, acceptor-like traps and fixed charge are considered while in a newly developed one, donor-like traps are taken into account also.


2014 ◽  
Vol 778-780 ◽  
pp. 710-713 ◽  
Author(s):  
Hamid Amini Moghadam ◽  
Sima Dimitrijev ◽  
Ji Sheng Han

This paper presents a physical model based on interface traps to explain both the larger barrier heights of practical Schottky diodes in comparison to the theoretically expected values and the appearance of a knee in the log I–V characteristics. According to this model, acceptor-type interface traps near the valance band increase the Schottky barrier height, which shifts the log I–V characteristic to higher forward-bias voltages. In addition to the acceptor traps, donor-type interface traps can appear near the conduction band, and when they do, they cause the knee in the log I–V characteristics as their energy level falls below the Fermi level and the charge associated with these traps changes from positive to neutral.


2011 ◽  
Vol 25 (30) ◽  
pp. 2323-2333
Author(s):  
ADITI SARKAR ◽  
ARNAB GANGOPADHYAY ◽  
A. SARKAR

In this work, meta-material like behavior of natural Mica are studied. This work makes an attempt to analyze the left-handed Maxwellian (LHM) properties of Mica. The investigations carried out on natural Mica specimen are optical reflectance, optical absorbance and DC current–voltage-characteristics (CVC). Optical reflectance of Mica sheet with plane polarized monochromatic light shows distinct difference with conventional theoretical results. The DC CVC also measured with complete electromagnetic shielding. There exists a clear difference in DC characteristic for presence and absence of stray electromagnetic fields. The X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FTIR) and ultraviolet-visible spectroscopy (UV-VIS) analysis are also carried out for further analysis. The results obtained from the optical reflectance characteristics using polarized light indicate LHM behavior as may be found in a meta-material. Micro-structural and electrical analysis shows that it is a nano-structured layered material.


2011 ◽  
Vol 2011 (1) ◽  
pp. 000747-000752 ◽  
Author(s):  
Jack Murray ◽  
Wayne Huebner ◽  
Matthew J. O’Keefe ◽  
Kristina Wilder ◽  
Ryan Eatinger ◽  
...  

Thin film capacitors for RF bypass and filtering applications were sputter deposited onto low temperature co-fired ceramic (LTCC) substrates. The capacitors were configured in a metal-insulator-metal (MIM) design featuring 200 nm thick Al electrodes and a 300 nm thick Al2O3 dielectric layer, with dimensions varied between ∼150×150 μm and ∼750×750 μm. DC current-voltage measurements (E ≤ 5 MV/cm) coupled with impedance analysis (≤15 MHz) was used to characterize the resulting devices. More than 90% of the devices functioned as capacitors with high DC resistance (>20 MΩ) and low loss (tan δ <0.1). A second set of capacitors were made under the same experimental conditions with device geometries optimized for high frequency (≥200 MHz) applications. These capacitors featured temperature coefficient of capacitance (TCC) values between 500 and 1000 ppm/°C as well as low loss and high self-resonant frequency performance (ESR <0.6 Ohms at self-resonance of 5.7 GHz for 82 pF). Capacitance and loss values were comparable between the capacitor structures of similar areas at the different frequency regimes.


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