1) generalized magnetic-field component
广义磁场分量
1.
Effects of generalized nonlinear unequal-power higher-power sum-squeezing of superposition state light-field composed of the two different multimode functional coherent states-unequal higher power sum-squeezing of generalized magnetic-field component;
两多模泛函相干态叠加态的高次和压缩——广义磁场分量的不等幂次高次和压缩效应
2.
The properties of the equal-power Y-squeezing of the state ｜Ψ~((4))〉_q generalized magnetic-field component of four state superposition multimode superposition state light field ｜Ψ~((4))〉_q are studied in detail by utilizing multimode squeezed state theory.
根据量子力学中的态叠加原理,应用多模压缩态理论,研究了态|Ψ(4)〉q广义磁场分量的等幂次压缩特性,构造了四态叠加多模叠加态光场|Ψ(4)〉q。
2) generalized magnetic field component
广义磁场分量
1.
The properties of the Equal-power amplitude squeezing of the generalized magnetic field component in the five state superposition multimode superposition state light field ｜Ψ~((5))〉_q is studied in detail by utilizing the multimode squeezed state theory.
构造了五态叠加多模叠加态光场｜Ψ(5)〉q,利用多模压缩态理论研究了态｜Ψ(5)〉q的广义磁场分量的等幂次N次振幅压缩特性。
2.
The properties of the equalorder Nth order Hsqueezing of the generalized magnetic field component in state Ψ(4)e,Ⅲ>q are studied in detail by using multimode squeezed state theory.
结果表明,当腔模总数q与压缩次数N的乘积qN=4m(m=1,2,3,…)时,态Ψ(4)e,Ⅲ〉q的广义磁场分量可恒处于等幂次N H最小测不准态;当qN=4m′+2(m′=0,1,2,3,…)时,若态间的初始相位差(θ1-θ2)、各模初始相位和∑qR2j分别满足一定取值φj及各模平均光子数之和∑qj=1j=1条件,态Ψ(4)e,Ⅲ〉q的广义磁场分量可呈现周期性等幂次N次方H压缩效应。
3) generalized magnetic-field
广义磁场
1.
By using multimode squeezing state theory,this paper makes a detailed study of the unequal-power higher-power amplitude-squeezing of generalized magnetic-field of 4MFSS light field in medium and it is found that 1) under certain conditions,the generalized magnetic-field of 4MFSS light field shows periodical generalized .
利用多模压缩态理论,对介质中4MFSS光场广义磁场分量的不等幂次高次振幅压缩效应进行了详细的研究。
4) generalized electric-field component
广义电场分量
1.
The general theory of generalized nonlinear equal-power higher-power difference-squeezing of multimode radiation light-field is utilized to study the properties of equal-power N-power difference-squeezing of generalized electric-field component of the arbitrary two-states superposition multimode functional superposition state light-field.
利用多模辐射场广义非线性等幂次高次差压缩的一般理论,研究了任意两态叠加多模泛函叠加态光场|ψ(f2)〉q的广义电场分量的非线性等幂次N次方差压缩特性。
5) generalized electric field component
广义电场分量
1.
Equal-power H-squeezing of generalized electric field component in multimode coherent state light field of functional with superposition of three macroscopically distinct quantum states;
多模泛函叠加态光场的广义电场分量等幂次H压缩特性
2.
Higher-Power sum squeezing of generalized electric field component in the first kind of multimode superposition state light field with superpositions of macroscopically distinct three quantum states;
构造了由多模相干态|{Zj}〉q、多模真空态|{0j}〉q和多模相干态的相反态|{-Zj}〉q线性叠加组成的第Ⅰ类三态叠加多模叠加态光场|ψ(3)1〉q,利用多模压缩态理论,研究了态|ψ(3)1〉q中广义电场分量的等幂次高次和压缩特性。
6) magnetic field component
磁场分量
补充资料：对称分量
由不对称三相相量分解而得的对称三相相量。一组不对称三相相量凔、妋、凗，当三者之和不为零(即凔+妋+凗≠0)时,可以分解成三组对称三相相量，它们分别是:零序分量,记为凔0,妋0,凗0;正序分量,记为凔1,妋1,凗1；负序分量,记为凔2,妋2,凗2。由于三相电力系统中有三相交流电机、三相输电线等三相电路元件，它们的电路参数在对称的运行条件下较便于确定，因而将非对称三相相量分解为三组对称分量便可分别考虑在每一相序的电压、电流作用下三相电路的工作情况，然后根据叠加定理得到三相电路的工作情况。
零序分量如图1所示，其特征是3个相量大小相等且同相。妋0＝凔0凗0＝凔0正序分量如图2所示，其特征是3个相量大小相等但不同相。三者按妋1滞后凔1，凗1滞后妋1,凔1又滞后凗1的顺序互差120°，即
妋1＝a2凔1凗1＝a凔1
式中
负序分量如图3所示，其特征类似正序分量，也是3个相量大小相等但不同相。不过，此时3个相量是按凗2滞后凔2，妋2滞后凗2，凔2又滞后妋2的顺序互差120°,即妋2＝a凔2凗2＝a2凔2三组对称分量与原不对称三相相量的关系如下：不对称三相相最可以是三相电压相量，也可以是三相电流相量。在三相不对称电路中，有的不对称电压相量和不对称电流相量只有两组对称分量。例如，不对称线电压相量,因必须满足KVL，即妭AB+妭BC+凗CA=0，故只含有正序对称分量和负序对称分量。
零序分量如图1所示，其特征是3个相量大小相等且同相。妋0＝凔0凗0＝凔0正序分量如图2所示，其特征是3个相量大小相等但不同相。三者按妋1滞后凔1，凗1滞后妋1,凔1又滞后凗1的顺序互差120°，即
妋1＝a2凔1凗1＝a凔1
式中
负序分量如图3所示，其特征类似正序分量，也是3个相量大小相等但不同相。不过，此时3个相量是按凗2滞后凔2，妋2滞后凗2，凔2又滞后妋2的顺序互差120°,即妋2＝a凔2凗2＝a2凔2三组对称分量与原不对称三相相量的关系如下：不对称三相相最可以是三相电压相量，也可以是三相电流相量。在三相不对称电路中，有的不对称电压相量和不对称电流相量只有两组对称分量。例如，不对称线电压相量,因必须满足KVL，即妭AB+妭BC+凗CA=0，故只含有正序对称分量和负序对称分量。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条