scholarly journals Improved memory characteristics by NH3-nitrided GdO as charge storage layer for nonvolatile memory applications

2012 ◽  
Vol 101 (3) ◽  
pp. 033501 ◽  
Author(s):  
L. Liu ◽  
J. P. Xu ◽  
F. Ji ◽  
J. X. Chen ◽  
P. T. Lai
2008 ◽  
Vol 1071 ◽  
Author(s):  
Chia-Han Yang ◽  
Yue Kuo ◽  
Chen-Han Lin ◽  
Rui Wan ◽  
Way Kuo

AbstractSemiconducting or metallic nanocrystals embedded high-k films have been investigated. They showed promising nonvolatile memory characteristics, such as low leakage currents, large charge storage capacities, and long retention times. Reliability of four different kinds of nanocrystals, i.e., nc- Ru, -ITO, -Si and -ZnO, embedded Zr-doped HfO2 high-k dielectrics have been studied. All of them have higher relaxation currents than the non-embedded high-k film has. The decay rate of the relaxation current is in the order of nc-ZnO > nc-ITO > nc-Si > nc-Ru. When the relaxation currents of the nanocrystals embedded samples were fitted to the Curie-von Schweidler law, the n values were between 0.54 and 0.77, which are much lower than that of the non embedded high-k sample. The nanocrystals retain charges in two different states, i.e., deeply and loosely trapped. The ratio of these two types of charges was estimated. The charge storage capacity and holding strength are strongly influenced by the type of material of the embedded nanocrystals. The nc-ZnO embedded film holds trapped charges longer than other embedded films do. The ramp-relax result indicates that the breakdown of the embedded film came from the breakdown of the bulk high-k film. The type of nanocrystal material influences the breakdown strength.


2011 ◽  
Vol 422 ◽  
pp. 139-145
Author(s):  
Wan Yi Huang ◽  
Hong Bing Chen ◽  
Sun Chen ◽  
Shi Jin Ding ◽  
David Wei Zhang

Pd nanocrystals embedded in TiO2film are formed in a self-assembly manner by rapid thermal annealing (RTA) of reactively co-sputtered TiPdO films. The cross-section transmission-electron microscopy (TEM) image and X-ray photoelectron spectra (XPS) reveal that the RTA at 800°C for 15 s results in the formation of Pd nanocrystals with an average size of around 10 nm. Further, the metal-oxide-semiconductor (MOS) capacitor with Pd-nanocrystals-embedded TiO2film sandwiched between Al2O3layers has been fabricated and characterized electrically in comparison with the counterpart without Pd nanocrystals, indicating that the formed Pd nanocrystals are dominant charge storage nodes. The fabricated MOS capacitor with Pd nanocrystals exhibits obvious memory characteristics, demonstrating a C-V hysteresis window of about 8.2 V at the sweeping voltage rang of +/-9 V, a flatband voltage shift of ~2V under a constant voltage stress of +9V for 10ns corresponding to a charge injection speed of 6×1012cm-2μs-1. The underlying mechanisms of the memory characteristics under different C-V sweeps have also been discussed.


2008 ◽  
Vol 85 (12) ◽  
pp. 2366-2369 ◽  
Author(s):  
Eunkyeom Kim ◽  
Kyoungmin Kim ◽  
Daeho Son ◽  
Jeongho Kim ◽  
Kyungsu Lee ◽  
...  

Author(s):  
V. Saikumar ◽  
H. M. Chan ◽  
M. P. Harmer

In recent years, there has been a growing interest in the application of ferroelectric thin films for nonvolatile memory applications and as a gate insulator in DRAM structures. In addition, bulk ferroelectric materials are also widely used as components in electronic circuits and find numerous applications in sensors and actuators. To a large extent, the performance of ferroelectric materials are governed by the ferroelectric domains (with dimensions in the micron to sub-micron range) and the switching of domains in the presence of an applied field. Conventional TEM studies of ferroelectric domains structures, in conjunction with in-situ studies of the domain interactions can aid in explaining the behavior of ferroelectric materials, while providing some answers to the mechanisms and processes that influence the performance of ferroelectric materials. A few examples from bulk and thin film ferroelectric materials studied using the TEM are discussed below.Figure 1 shows micrographs of ferroelectric domains obtained from undoped and Fe-doped BaTiO3 single crystals. The domain boundaries have been identified as 90° domains with the boundaries parallel to <011>.


2012 ◽  
Vol 52 (4) ◽  
pp. 635-641 ◽  
Author(s):  
Jer-Chyi Wang ◽  
Chih-Ting Lin ◽  
Pai-Chi Chou ◽  
Chao-Sung Lai

2015 ◽  
Vol 138 ◽  
pp. 86-90 ◽  
Author(s):  
Pi-Chun Juan ◽  
Jyh-Liang Wang ◽  
Tsang-Yen Hsieh ◽  
Cheng-Li Lin ◽  
Chia-Ming Yang ◽  
...  

2012 ◽  
Vol 52 (8) ◽  
pp. 1627-1631 ◽  
Author(s):  
Jer-Chyi Wang ◽  
Chih-Ting Lin ◽  
Chi-Hsien Huang ◽  
Chao-Sung Lai ◽  
Chin-Hsiang Liao

2019 ◽  
Vol 19 (1) ◽  
pp. 41-47
Author(s):  
Chia-Han Yang ◽  
Yue Kuo ◽  
Chen-Han Lin ◽  
Way Kuo

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