1) Cross tail magnetic field B y component
越尾磁场By分量
2) magnetic field component
磁场分量
3) electromagnetic field component
电磁场分量
1.
In this paper,the expressions of the electromagnetic field components in a plasma waveguide immersed in a strong longitudinal magnetic field are derived in detail from the Maxwell s equations.
文章从麦克斯韦方程组出发,利用纵向场分量法,详细地推导了强引导磁场下等离子体波导中电磁场分量的表达式。
4) Longitudinal components of electromagnetic fields
纵向电磁场分量
5) integral magnetic field measurement
积分磁场测量
1.
This article presents the basic principle of dipole integral magnetic field measurement .
介绍了兰州重离子加速器冷却储存环(HIRFL CSR)积分磁场测量系统以及积分测量的基本原理和数据处理方法,对测量结果的分析表明整个系统运行可靠稳定,可用于CSR磁铁的积分测量。
6) 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。
补充资料:黑越越
1.形容黑暗。
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