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1)  critical magnetic field strength
临界定向磁场强度
2)  critical magnetic induction
临界磁感应强度
3)  critical electric field
临界电场强度
1.
A higher couple coefficient and lower operating voltage can be obtained by taking thinner bottom oxide and thicker top oxide which can obtain higher critical electric field and thinner efficient oxide.
结果表明 ,采用较薄的底氧和较厚的顶氧 ,既能保证较高的临界电场强度 ,又能获得较薄的等效氧化层厚度 ,提高耦合率 ,降低编程电压 。
4)  limiting field
临界场强
1.
51Td are simulated, and the electron swarm parameters such as effective ionization coefficient α , drift velocity Vd, and limiting field .
51Td(1Td=10~(-17)Vcm~2)的场强范围内,仿真了SF_6和CO_2混合气体中的电子崩发展,求出了有效电离系数,漂移速度和临界场强。
5)  critical magnetic field
临界磁场
1.
The binding energies of low excited states and the critical magnetic fields at which D- states changed from unbound states to bound states are presented too.
用超球坐标数值计算近似方法解二维D-中心在磁场中的薛定锷方程,得到了基态能,计算了低激发态的束缚能同时得到了低激发态由非束缚态变为束缚态的临界磁场值。
2.
On the basis of GL theory,this paper gives the Gibbs function of DSC system and the relation between the critical magnetic field of DSC system in case of microwave irradiation and both the coherence length and the thickness of dielectric under considering the Josephson current.
在GL理论基础上,考虑Josephson电流,给出DSC系统在微波辐照下的Gibbs函数,并得出临界磁场与绝缘层的厚度、相干长度的关
3.
The unstable magnetization changes discontinuously when across a critical value,corresponding to a critical magnetic field.
这个不稳定的磁化强度对应于一个临界磁场,低温时外场变化经过临界磁场时磁化强度发生突变。
6)  critical strength
临界强度
1.
This paper analyzes mechanism of concrete early frost damage,discusses its expression and its permissible critical strength,and introduces application of the critical strength combined with practical engineering.
分析了混凝土早期受冻损害的机理,论述了混凝土早期受冻损害的表现,探讨了允许混凝土早期受冻的临界强度,并结合工程实例,介绍了允许混凝土早期受冻的临界强度的应用。
2.
As a result, the critical strength can not be decided by it.
研究表明:初始冻结强度在宏观规模析冰的一次冻结法中为非敏感参数,无法确定负温砼抗冻临界强度。
补充资料:临界磁场(criticalmagneticfield)
临界磁场(criticalmagneticfield)

在外磁场H中将正常态第一类超导体冷却到临界温度Tc(H)时,样品即开始转入超导态(见“迈斯纳效应”)。对可逆迈斯纳效应,意味着在T<Tc温度下也对应着开始破坏超导电性的磁场Hc(T),称临界磁场,这里又称热力学临界磁场。它的经验公式可写为:

`H_c(T)=H_c(0)[1-(\frac{T}{T_c})^2]`

这里Hc(0)是T=0K时的临界磁场。这类相变属一级相变。对第二类超导体,则尚有第一,第二和第三临界磁场。

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