Radiation Effects on Proton Particles in Bipolar Memory Devices

Author(s):  
Young Lho ◽  
Ki Kim
2014 ◽  
Vol 615 ◽  
pp. 566-568 ◽  
Author(s):  
Xinman Chen ◽  
Wei Hu ◽  
Shuxiang Wu ◽  
Dinghua Bao

2016 ◽  
Vol 39 ◽  
pp. 134-150
Author(s):  
Valerii Ievtukh ◽  
A. Nazarov

In this work, nanocrystal nonvolatile memory devices comprising of silicon nanocrystals located in gate oxide of MOS structure, were comprehensively studied on specialized modular data acquisition setup developed for capacitance-voltage measurements. The memory window formation, memory window retention and charge relaxation experimental methods were used to study the trapping/emission processes inside the dielectric layer of MOS capacitor memory. The trapping/emission processes were studied in standard bipolar memory mode and in new unipolar memory mode, which is specific for nanocrystalline nonvolatile memory. The analysis of experimental results shown that unipolar programming mode is more favourable for nanocrystalline memory operation due to lower wearing out and higher breakdown immunity of the MOS device’s oxide. The study was performed for two types of nanocrystalline memory devices: with one and two silicon nanocrystalline 2D layers in oxide of MOS structure correspondingly. The electrostatic modelling was presented to explain the experimental results.


ETRI Journal ◽  
2007 ◽  
Vol 29 (1) ◽  
pp. 124-126 ◽  
Author(s):  
Young Hwan Lho ◽  
Ki Yup Kim

2019 ◽  
Vol 66 (12) ◽  
pp. 2398-2407
Author(s):  
Joshua S. Holt ◽  
Zahiruddin Alamgir ◽  
Karsten Beckmann ◽  
Nadia Suguitan ◽  
Sierra Russell ◽  
...  

Author(s):  
F. Louchet ◽  
L.P. Kubin

Investigation of frictional forces -Experimental techniques and working conditions in the high voltage electron microscope have already been described (1). Care has been taken in order to minimize both surface and radiation effects under deformation conditions.Dislocation densities and velocities are measured on the records of the deformation. It can be noticed that mobile dislocation densities can be far below the total dislocation density in the operative system. The local strain-rate can be deduced from these measurements. The local flow stresses are deduced from the curvature radii of the dislocations when the local strain-rate reaches the values of ∿ 10-4 s-1.For a straight screw segment of length L moving by double-kink nucleation between two pinning points, the velocity is :where ΔG(τ) is the activation energy and lc the critical length for double-kink nucleation. The term L/lc takes into account the number of simultaneous attempts for double-kink nucleation on the dislocation line.


Author(s):  
G.D. Danilatos

The advent of the environmental SEM (ESEM) has made possible the examination of uncoated and untreated specimen surfaces in the presence of a gaseous or liquid environment. However, the question arises as to what degree the examined surface remains unaffected by the action of the electron beam. It is reasonable to assume that the beam invariably affects all specimens but the type and degree of effect may be totally unimportant for one class of applications and totally unacceptable for another; yet, for a third class, it is imperative to know how our observations are modified by the presence of the beam. The aim of this report is to create an awareness of the need to initiate research work in various fields in order to determine the guiding rules of the limitations (or even advantages) due to irradiation.


Author(s):  
S. G. Ghonge ◽  
E. Goo ◽  
R. Ramesh ◽  
R. Haakenaasen ◽  
D. K. Fork

Microstructure of epitaxial ferroelectric/conductive oxide heterostructures on LaAIO3(LAO) and Si substrates have been studied by conventional and high resolution transmission electron microscopy. The epitaxial films have a wide range of potential applications in areas such as non-volatile memory devices, electro-optic devices and pyroelectric detectors. For applications such as electro-optic devices the films must be single crystal and for applications such as nonvolatile memory devices and pyroelectric devices single crystal films will enhance the performance of the devices. The ferroelectric films studied are Pb(Zr0.2Ti0.8)O3(PLZT), PbTiO3(PT), BiTiO3(BT) and Pb0.9La0.1(Zr0.2Ti0.8)0.975O3(PLZT).Electrical contact to ferroelectric films is commonly made with metals such as Pt. Metals generally have a large difference in work function compared to the work function of the ferroelectric oxides. This results in a Schottky barrier at the interface and the interfacial space charge is believed to responsible for domain pinning and degradation in the ferroelectric properties resulting in phenomenon such as fatigue.


2010 ◽  
Vol 49 (S 01) ◽  
pp. S53-S58 ◽  
Author(s):  
W. Dörr

SummaryThe curative effectivity of external or internal radiotherapy necessitates exposure of normal tissues with significant radiation doses, and hence must be associated with an accepted rate of side effects. These complications can not a priori be considered as an indication of a too aggressive therapy. Based on the time of first diagnosis, early (acute) and late (chronic) radiation sequelae in normal tissues can be distinguished. Early reactions per definition occur within 90 days after onset of the radiation exposure. They are based on impairment of cell production in turnover tissues, which in face of ongoing cell loss results in hypoplasia and eventually a complete loss of functional cells. The latent time is largely independent of dose and is defined by tissue biology (turnover time). Usually, complete healing of early reactions is observed. Late radiation effects can occur after symptom-free latent times of months to many years, with an inverse dependence of latency on dose. Late normal tissue changes are progressive and usually irreversible. They are based on a complex interaction of damage to various cell populations (organ parenchyma, connective tissue, capillaries), with a contribution from macrophages. Late effects are sensitive for a reduction in dose rate (recovery effects).A number of biologically based strategies for protection of normal tissues or for amelioration of radiation effects was and still is tested in experimental systems, yet, only a small fraction of these approaches has so far been introduced into clinical studies. One advantage of most of the methods is that they may be effective even if the treatment starts way after the end of radiation exposure. For a clinical exploitation, hence, the availability of early indicators for the progression of subclinical damage in the individual patient would be desirable. Moreover, there is need to further investigate the molecular pathogenesis of normal tissue effects in more detail, in order to optimise biology based preventive strategies, as well as to identify the precise mechanisms of already tested approaches (e. g. stem cells).


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