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51.
很多情况会引发网管中心或实验中心数据线、数据设备浪涌或瞬变电压的产生.这些浪涌电压有时可以达到几百甚至上千伏特,浪涌电流可这几百安培.如此高的电压电流,轻则引发系统逻辑错误,重则直接损坏硬件设备,或使系统崩溃.分析浪涌产生的机制和诱因,通过案例给出几种防止浪涌产生、以及降低浪涌破坏程度的方法. 相似文献
52.
The doping dependence of the velocity-field characteristic in InGaAs has been investigated by an analysis of measurements
with transferred-electron devices. The electron peak velocity has been determined directly as a function of electron concentration
and low-field mobility. The carrier-concentration dependence of the velocity-field characteristic has been deduced by comparing
experimental and theoretical transient device behaviour. The experimental results support a theoretical approach for the velocity-field
characteristic which has been proposed recently. 相似文献
53.
The presence of hole traps has been studied by deep level transient spectroscopy (DLTS) characterization of low carrier densityp-type GaAs grown by MBE on p+-GaAs substrates using Al and Co Schottky contacts. The results obtained indicate the presence of several hole traps with
energy levels of between 0.06 and 0.65 eV above the valence band in concentrations up to 2 × 1012/cm3. Some of these defects,e.g. Cu, are ascribed to system-, source-or substrate-related impurities, but the origin of several other defects is unknown. 相似文献
54.
Z-Q. Fang Q. H. Xie D. C. Look J. Ehret J. E. Van Nostrand 《Journal of Electronic Materials》1999,28(8):L13-L16
We have investigated electron emission from self-assembled In0.5Ga0.5As/GaAs quantum dots (QDs) grown by molecular-beam epitaxy (MBE). Through detailed deep level transient spectroscopy comparisons
between the QD sample and a reference sample, we determine that trap D, with an activation energy of 100 meV and an apparent
capture cross section of 5.4×10−18 cm2, is associated with an electron quantum level in the In0.5Ga0.5As/GaAs QDs. The other deep levels observed, M1, M3, M4, and M6, are common to GaAs grown by MBE. 相似文献
55.
介绍了脉搏血样饱和度检测的理论基础与重要的临床应用价值。提出了一种基于CMOS影像传感器的脉搏血氧饱和度监测系统,用CMOS传感器阵列取代了传统血氧仪中的光敏探测,实现了血氧饱和度及脉搏波的无接触测量。阐述了其在组织发育、伤口诊断、病变的提前预测等场合的潜在应用价值。实验结果表明,由于摄像头不能够有效屏蔽外界光源噪声的干扰,所设计样机较传统的血氧仪测得的饱和度值偏低,误差偏大,从而进一步提出减小误差提高精度的方案构想。 相似文献
56.
57.
58.
Z. -Q. Fang D. C. Look A. Krtschil A. Krost F. A. Khan I. Adesida 《Journal of Electronic Materials》2006,35(4):613-617
Extended defects on the top surface of a 250-μm-thick free-standing GaN sample, grown by hydride vapor phase epitaxy (HVPE),
were studied by deep level transient spectroscopy (DLTS) and scanning surface potential microscopy (SSPM). For comparison,
similar studies were carried out on as-grown HVPE-GaN samples. In addition to the commonly observed traps in as-grown HVPE-GaN,
the DLTS measurements on free-standing GaN reveal a very high concentration of deep traps (∼1.0 eV) within about 300 nm of
the surface. These traps show nonexponential capture kinetics, reminiscent of those associated with large defects, that can
accumulate multiple charges. The SSPM measurements clearly reveal the presence of charged microcracks on the top surface of
the sample. It appears that the “giant traps” may be associated with these microcracks, but we cannot rule out the involvement
of other extended defects associated with the near-surface damage caused by the polishing/etching procedure. 相似文献
59.
Recharge to the aquifer leads to the growth of a groundwater mound. Therefore, for the proper management of an aquifer system, an accurate prediction of the spatio-temporal variation of the water table is very essential. In this paper, a problem of groundwater mound formation in response to a transient recharge from a rectangular area is investigated. An approximate analytical solution has been developed to predict the transient evolution of the water table. Application of the solution and its sensitivity to the variation of the recharge rate have been illustrated with the help of a numerical example.Notations
a =
Kh/e [L2/T]
-
A =
aquifer's extent in the x-direction [L]
-
B =
aquifer's extent in the y-direction [L]
-
e =
effective porosity
-
h =
variable water table height [L]
-
h
0=
initial water table height [L]
-
h =
weighted mean of the depth of saturation [L]
-
K =
hydraulic conductivity [L]
-
m, n =
integers
-
P =
constant rate of recharge [L/T]
-
P
1+P0=
initial rate of transient recharge [L/T]
-
P
1=
final rate of transient recharge [L/T]
-
s =
h
2–h
0
2
[L2]
-
t =
time of observation [T]
-
x,y =
space coordinates
-
x
2–x1=
length of recharge area in x-direction [L]
-
y
2–y1=
width of recharge area in y-direction [L]
-
z =
decay constant [T-1] 相似文献
60.
高水头抽水蓄能电站中,常采用一洞多机系统,所以机组之间水力联系紧密,本文建立了对水力干扰进行过渡过程计算所必须的既能进行大波动计算又可进入小波动的数学模型,并编制了计算程序,通过计算研究了部分机组停机过程中,其余机组在水力干扰下的过渡过程及稳定问题。 相似文献