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1)  compressional wave field
压缩波场
2)  radiation squeezing
光场压缩
1.
The radiation squeezing effect in the interaction process between the single mode squeezed vacuum field and a moving two-level atom is studied by means of solving the Schrdinger equation and numerical calculations.
文章采用求解Schrdinger方程和数值计算方法,研究了单模压缩真空场与运动二能级原子相互作用过程中的光场压缩效应。
2.
In this article,by means of solving Schrdinger equation and numerical calculations,the radiation squeezing effects in the system of the binomial states field interacting with a moving two-level atom has been discussed.
本文采用求解Schr dinger方程和数值计算方法,研究了二项式光场与运动二能级原子相互作用过程中的光场压缩效应。
3.
By means of solving Schrdinger’s equation and numerical calculations, the radiation squeezing effects in the system of the binomial states field interacting with a moving Ξ-type three-level atom are discussed.
采用求解Schrdinger方程和数值计算的方法,研究二项式光场与Ξ型三能级原子相互作用过程中的光场压缩效应。
3)  light squeezing
光场压缩
1.
By means of solving Schrdinger equation and numerical calculations,the light squeezing effects in the system of the two-mode odd-even entangled coherent optical field interacting with a V-type threelevel atom discussed.
采用求解薛定谔方程和数值计算方法,研究了V型三能级原子与双模奇偶纠缠相干光场相互作用过程中的光场压缩效应,讨论了压缩效应与双模奇偶纠缠相干光场的纠缠程度、系统失谐量、双模光场的平均光子数和原子基态概率幅的依赖关系。
2.
The squeezing properties of light field interacting with the A-type three level atom via intensity-dependent coupling are studied and the influences of detuning between the atomic transition frequency and the light frequency in single-photon process and the initial squeezing of light on the light squeezing are discussed emphatically.
研究了光场与A-型三能级原子依赖强度耦合系统光场的压缩特性,讨论了单光子跃迁失谐量和初始光场压缩因子对光场压缩的影响。
3.
By solution of Schrodinger equation and numerical calculations, the light squeezing effects in the system of the two-mode entangled coherent state optical field interacting with a V-type three-level atom was discussed.
研究了双模纠缠相干光场与V型三能级原子相互作用过程中光场压缩效应,结果表明:此压缩效应与双模纠缠光场的纠缠程度、失谐量、平均光子数和原子初态相关联。
4)  optical field squeezing
光场压缩
1.
Influence of the coupling constant ga of dipole-dipole interaction between atoms and the coupling strength x of the Kerr medium with the optical field on the double atoms dipole squeezing and optical field squeezing are discussed by numerical calculations.
通过数值计算,讨论了原子偶极间相互作用耦合常数和Kerr介质与单模腔场相互作甩的耦合强度对体系中的双原子偶极压缩和光场压缩的影响。
5)  field squeezing
场压缩
6)  field entropy squeezing
场熵压缩
1.
With the numerical method,the influence of two-atom s entanglement and field intensity on the field entropy squeezing properties is discussed.
研究了相干态光场与纠缠双原子相互作用系统中场熵的压缩性质,借助于数值计算,讨论了双原子纠缠度及光场强度对场熵压缩的影响。
2.
The entropy squeezing properties in the two photon Jaynes-Cummings model in a Kerr medium are studied by means of quantum information entropy,and the nonlinear interaction of the Kerr medium with the model field and the initial state of atoms on the field entropy squeezing are discussed.
运用量子信息熵理论研究了K err介质中双光子J-C模型中场熵压缩性质,讨论了K err介质与原子初态对场熵压缩特性的影响。
3.
The field entropy squeezing properties in the nonlinear interaction between squeezing vacuum state field and atom are studied by means of quantum information entropy theory.
讨论了初始压缩真空场的压缩度以及克尔非线性作用的强度对场熵压缩特性的影响。
补充资料:压缩波
      在气体动力学中,波是扰动区和未扰动区的分界面。若穿过此界面,扰动使气体的压强升高,则此波称为压缩波;反之称为膨胀波。一维非定常流动中的压缩波的形成可用图1说明。 图1a上方表示一个原来装有压强和密度分别为p0和ρ0的静止气体的管道。当活塞以无限小的速度dv向右运动时,活塞右侧相邻的一层气体被压缩,压强和密度分别升高一个微量dp和dρ,并被迫以与活塞同样的速度向右运动。接着,已运动的气体又推动右边相邻的气体。如此一层一层往右传播,即活塞的运动在静止气体中产生扰动并以一定的速度在未扰动气体中传播。这种微弱扰动的传播速度等于声速。过一定时间后,扰动传播到A-A′位置,AA′面便是扰动和未扰动区域的分界面。这个分界面就是压缩波。图1a下方表示在某一对应的瞬间气体压强p沿管长x的分布。反之,若活塞以速度dv向左运动,产生的扰动使活塞右侧气体压强和密度减小,相应的波称为膨胀波。压缩波和膨胀波有一个根本区别:对于一系列前后相继的压缩波(图1b),后面的波的传播速度比前面的波快,最终可能叠在一起形成一道突跃的压缩波,即激波;膨胀波则相反,不会形成突跃的膨胀波。一维非定常波主要用来分析各种管道中的非定常流动。在二维和三维定常超声速气流中,扰动和未扰动区的分界面就是马赫波(见马赫锥)。超声速气流经过一系列马赫波膨胀加速,也称为膨胀波,若增压减速,则称为压缩波。定常超声速气流绕凸壁表面和凹壁表面的流动就是膨胀波和压缩波的典型例子(图2)。当气流绕凸壁表面时(图2a),气流的马赫数逐渐增大,马赫角逐渐减小,依次的波逐渐向下游倾斜,形成向下游张开的一个扇形连续膨胀区(见普朗特-迈耶尔流动)。绕凹壁则情况相反(图2b),诸波依次有汇交的趋势。在诸压缩波汇交时,一系列微弱压缩波叠在一起,形成激波。在定常超声速气流中,气体速度、压强等的变化都是以压缩波、膨胀波或激波的形式出现的。
  

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