1) 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。
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 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。
4) generalized electrical-field
广义电场
1.
The unequal-power Nj-th power Y-squeezing of generalized electrical-field of 4MFSS light field in the medium;
介质中4MFSS光场广义电场的不等幂次N_j次方Y压缩
2.
The sum-squeezing of generalized electrical-field of multimode functional superposition state light field in medium;
介质中多模泛函叠加态光场广义电场的高次和压缩
3.
Unequal-order H-squeezing of generalized electrical-field of multimode functional superposition state light field in medium;
介质中多模泛函叠加态光场广义电场的不等幂次H压缩
5) generalized gaussian field
广义高斯场
1.
In this paper, we discuss the linear large deviation principle of generalized gaussian field.
本文考虑广义高斯场的线性大偏差。
6) generalized free field
广义自由场
补充资料：Соболев广义导数
Соболев广义导数
Sobolev generalized derivative
【补注】在西方文献中，O众泪玲B广义导数称为弱导数(，祀ak deri珑币ve)或分布导数(dis川h川0刊目山幻W币记).。6o二。广义导数【S诵川eVg留司加团山滋.d视;Co-60二皿0606川e一。朋”Po“3即及”a“」 局部可积函数的局部可积‘广义导数(见广义函数(罗ne阁讼沮丘mctlon)). 确切地说，假设Q是n维空间R”的开集，F和.厂都是Q上局部可积函数，那么f是F在Q上羊于x，的。分叨e”广冬停导攀记为 斋(·，一f‘·，，·〔“，，一’，‘’，”，是指对O上所有具紧支集的无限次可微函数价，等式 fF(二)李竺d二=一ff(二、耐，、d二 J OX，夕- 日-一]O成立.C改沁朋B广义导数在O上仅对几乎处处的戈有定义. 一个等价的定义如下.假设Q上局部可积函数F能在某个陀维零测度集上改变它的值成为这样一个函数，使后者对几乎所有(依”一1维测度)的点(x，，·，x，一;，毛十，，“‘，x。)关于x，是一元局部绝对连续的于是F对几乎所有的x〔。，存在关于xj的通常偏导数.如果后者局部可积，则称它为O石如cB广义导数. 第三种等价的定义是:给定两个函数F与f，若在。上存在连续可微函数列遥凡}，使对其闭包含于Q的任意区域田都有 J!r*(x)一F(x)‘dx一0， rl刁F‘(x飞_、} )}二成一一了“’}“x一“，“一的，则f就是F在Q上的O力期eB广义导数. F在Q上的高阶广义导数(若存在) a 2 F a3F 口x。ax，’ax.口x，刁x。’可由归纳法定义.它们与微分的次序无关;例如在Q上几乎处处有 J ZF_刁ZF 日x.刁x，日x，己x，’
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