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equal-power
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     The Properties of Generalized Nonlinear Equal-Power N-th Power H-Squeezing of Generalized Electric Field Component in The State|ψ_3~((3))〉_q
     态|ψ_3~((3))〉_q广义电场分量的等幂次N次方H压缩
短句来源
     Effects of Generalized Nonlinear Equal-power Higher-power Sum Squeezing of Generalized Magnetic Field Component in the State |Ψ_3~((3))>_q
     态|ψ_3~((3))〉_q中广义磁场分量的等幂次高次和压缩
短句来源
     3. The properties of generalized nonlinear equal-power N-th power Y-squeezing and equal-power N-th power H-squeezing of the state are further studied too .
     3.研究了态|ψ~((4))〉_q的广义非线性等幂次N次方Y压缩和等幂次N次方H压缩特性。
短句来源
     Effects of equal-power n-th power y-squeezing of generalied electric field component in the state|ψ_3~((3))>q
     态|ψ_3~((3))>q中广义电场分量的等幂次N次方Y压缩特性
短句来源
     2. The properties of generalized nonlinear equal-power N-th power Y-squeezing , equal-power N-th power H-squeezing, unequal-power -th power Y-squeezing and unequal-power Nj-th power H-squeezing of the stateare studied.
     2.研究了态|ψ_5~((3))〉_q的广义非线性等幂次N次方Y压缩、等幂次N次方H压缩、不等幂次N_j次方Y压缩以及不等幂次N_j次方H压缩特性。
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  “equal-power”译为未确定词的双语例句
     THE EFFECTS OF EQUAL-POWER 4m-TH POWER Y-SQUEEZING OF GENERALIZED MAGNETIC FIELD COMPONENT IN THE STATE |ψ_5~((3))〉_q
     多模叠加态光场|ψ_5~((3))〉_q中广义磁场4m次方Y压缩
短句来源
     The Effects of Equal-Power 2p-Th Power Y-Squrrzing of Generalize Magnetic Field Component in the State |Ψ_6~(3)>q
     多模叠加态光场|Ψ_6~(3)>q中广义磁场2p次方Y压缩
短句来源
     3 The study of the effects of Equal-Power N-th Power Y-Squeezing on the Quantum Noise of Effective Field-Operator of Generalized Vector Potential in a New Kind of 4MFSS (Ⅰ) Light-Field.
     3研究了新型4MFSS(Ⅰ)光场的广义矢势有效场算符量子噪声的等幂N次Y压缩效应。
短句来源
     GENERALIZED NONLINEAR EQUAL-POWER N-TH POWER Y-SQUEEZING OF GENERALIZED ELECTRIC FIELD COMPONENT IN THE STATE |Ψ~ (3) >_q
     态|Ψ~((3))〉_q中广义电场分量的偶数次N次方Y压缩
短句来源
     2 The study of the effects of Generalized Nonlinear Equal-Power Even-Number-Power Higher-Power Amplitude Squeezing of Generalized Electric-Field Component in 4MFSS(Ⅰ) Light-Field.
     2研究了4MFSS(Ⅰ)光场广义电场分量的等幂偶次高次振幅压缩效应。
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The paper analyses the macrofractography morphology of metal fatigue and bri-ttleness. It Shows that the space of the beach marks on fatigue sarface, the change of bended direction and the slant of the beach marks , the shape of the beach marks at the circumambdient stress concentration and fatigue steps at the different conditions can be described by using a simple equation. The shapes of the brittle rapid radiactive curves are calculated,analysed, compared and discussed with two different models (the vertical...

The paper analyses the macrofractography morphology of metal fatigue and bri-ttleness. It Shows that the space of the beach marks on fatigue sarface, the change of bended direction and the slant of the beach marks , the shape of the beach marks at the circumambdient stress concentration and fatigue steps at the different conditions can be described by using a simple equation. The shapes of the brittle rapid radiactive curves are calculated,analysed, compared and discussed with two different models (the vertical lines of the including curves of the twinkling leading edges of cracks and the traces cruves of the intersection of the growth of nuclei) and with two different growing methods of the nuclei (equal speed and equal power).

本文对金属疲劳和脆性宏观断口形态进行了数学分析。分析表明,宏观疲劳弧线的间隔、弯曲方向的改变、偏转、周应力集中时对轴的疲劳弧线的形状及各种情况下的疲劳沟线(台阶),均可用一简单的数学方程式来描述;本文用两种不同的模型(瞬时裂纹前沿线的包络线的垂线和依次生核的裂纹扩展交点的轨迹线)及两种不同的裂纹核心的扩展方式(等功的和等速的)形成的宏观脆性放射线条——即人字纹——进行了数学分析、比较和讨论。

The expression of light pressures produced by laser pulse trains are obtained by solving the density matrix equation. The effect of the pressures on atomic velocity distribution are calculated and its action is compared with that of the CW laser light. The result shows that retardation and cooling would be more effective by using a laser pulse train with appropriate modulation than a CW laser of equal power or even 50% higher.

本文通过解双能级系统的密度矩阵方程,求出了序列脉冲激光的光压力,计算了光压对原子速度分布的影响,并与连续激光的作用进行了对比。结果表明:采用序列脉冲激光并适当选择调制函数参数,可比相同功率甚至功率增大1/2情况下的连续激光更为有效地使原子束减速和冷却。

This study describes the acute and chronic responses of brain tissue to injury by nonfocused argon (Ar) laser beam with equal power density.Cortices of 26 rabbits were exposed to laser pulses for 6 s and examined 0.5 hour, 24 hours, half a month and 1 month after injury respectively.Histologically, all brain tissues were sharply demarcated by hemispheroidal defects with a vaporized center surrounded by a zone of coagulation, necrosis and edema.The depth of this vaporized center is 2 mm, and the width is 3mm.The...

This study describes the acute and chronic responses of brain tissue to injury by nonfocused argon (Ar) laser beam with equal power density.Cortices of 26 rabbits were exposed to laser pulses for 6 s and examined 0.5 hour, 24 hours, half a month and 1 month after injury respectively.Histologically, all brain tissues were sharply demarcated by hemispheroidal defects with a vaporized center surrounded by a zone of coagulation, necrosis and edema.The depth of this vaporized center is 2 mm, and the width is 3mm.The width of the zone of coagulation, necrosis and edema was less than 1 mm.The thermal damage caused by the argon Laser beam was minimal in the surrounding tissue.One Month after injury, a core of coagulation and necrsis surrounded by mild fibrillary gliosis was observed.

本研究讨论了相等能量密度的、非聚焦的氩激光作用于兔脑组织后所产生的急、慢性反应。分别在26只兔脑皮层上作定点连续照射6s,在照射后的30min,24h、15天和30天后的兔脑标本,组织学上现发有明显界缘的气化中心,其平均深度为2mm,宽度为3mm,其外依次为凝固、坏死和水肿带,宽度不超过1mm。周围脑组织的热反应也是很小的。30天后见有胶质细胞增生修复创伤。

 
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