• 基本释义

1.Fa(atomic ratio of Fe/(Fe+Mg)×100) value(with a range of 34.1 mol%~42.2 mol%) and percent mean deviation(PMD) value(6.1) of olivine reflected some degree of thermodynamics equilibration in olivine.
橄榄石颗粒Fa(Fe/(Fe+Mg)原子百分比)值范围在34.1 mol%~42.2 mol%,百分标准平均方差(PMD)值为6.1,表明这些颗粒达到了一定的热力学平衡。收藏指正
2.Using principle of eletronegativite equaligation to estimate atomic charge was putforward by Sanderson. Sinceit is difficult to find the value of electronegative in commontextbooks. We can get satisfactory result by using popular pauling eletrongativite tocalulate.
应用电负性均衡原理估算原子电荷,此概念是Sanderson提出来的,由于Sanderson电负性值一般教材难以找到,采用常用的鲍林电负性进行计算,能得到满意的结果.收藏指正
3.This paper introduces a new method which can obtain the extinction value linear to the concentration for the atomic absorption spectrometry (AAS) and atomic resonant fluorescent spectrometry (ARFS).
提出一种使原子吸收与原子共振荧光光谱分析均能得到与被测元素浓度成线性关系的消光值的方法.收藏指正
4.The results indicate that the value of squeezed component of the atomic dipole, squeezed frequency, amplitude and squeezed direction of the atomic information entropy ca be controlled by choosing the atomic initial state, the velocity of atomic motion, the field structure and the squeezing factor of field and the squeezing phase angle of the field, respectively.
结果表明,通过选择原子初态,原子运动速度、场模结构,场压缩因子和场压缩相位角可以分别控制原子信息熵压缩的偶极矩分量值、压缩频率、压缩幅度和压缩方向。收藏指正
5.Because of above reason, this method could not widely used . Based on the principle of Atomic Frequency Standard,This paper introduces a implemention of DDS which is based on CORDIC algorithm. this algorithm can retrieve the value of DDS by the basic process such as addition ,subtraction, shift.
简要介绍铷原子频标的基本原理的基础上,提出并且实现了一种基于CORDIC算法的DDS,本算法通过简单的加、减和移位等基本操作来实现DDS的功能,并给出实现DDS的实例。收藏指正
6.The band gap almost keeps constant, about 3.27 eV. The film deposited at -300 V exhibits atomic smooth surface, and Rrms is about 0.113 nm, which results in the highest refractive index, nλ=550 nm=2.51, which is more than or equal to the maximum value reported.
-300 V偏压时薄膜达到原子级表面平滑度,均方根粗糙度Rrms≈0.113 nm,因而薄膜折射率n也最高(nλ=550nm达到已有报道的最高值2.51).收藏指正
7.The results showed that both the ALCTE value of Al-32%Mg-6%Zn(atomic concentration) alloy heated from 28? ℃to 448? ℃and the one of Al-15%Cu-9%Mg-0.04%Be alloy heated from 25?
结果表明Al-32%Mg-6%Zn(原子数分数,下同)合金从28℃加热到448℃时,其ALCTE值为2.360×10-5℃-1,Al-15%Cu-9%Mg-0.04%Be合金从25℃加热到511℃时,其ALCTE值为1.881×10-5℃-1,分别是11种合金中最高和最低的.收藏指正
8.Using ab initio plane waves ultrasofi pseudopotential method based on generalized gradient approximation(GGA),the lattice constant is calculated of CaTiO_3,the total energy and the cohesive energy,the former of which is in good agreement with the experimental value,and then analyzed the effects of Ti atomic Z coordinate on the energy structure and Density of State of CaTiO_3.The electronic structure of CaTiO_3 was influenced intensely by the location of Ti atom.
基于广义剃度近似(GGA)的从头算平面波超软赝势方法,计算了CaTiO_3晶体的晶格常数、总能量以及结合能,得到了与实验相一致的结果。 分析了Ti原子Z坐标位置对CaTiO_3能带结构、态密度(DOS)等的影响。收藏指正
9.We study the time evolution law of the atomic response in an open Λ-type inversionless lasing system when the probe or driving field is off-resonance,and compare the law with that obtained when the probe and driving fields are resonant.We find that the detuning has considerable effects on the time evolution law:When the probe or driving fields is off-resonance,the dispersive responses for the probe and driving fields are no longer 0 and the two-photon coherence is no longer a pure real;The variation of the probe detuning can make the time evolution law of the population distributions and the gain (absorbtion) of the driving field changing obviously;With detuning increasing,the time evolution behavior of the gain (absorbtion),dispersion of the probe field and the two-photon coherence will gradually diviate from the evolution law of the standard damped oscillator;With the driving detuning increasing,the oscillating time of the dispersion of the driving field becomes longer,the amplitude and the stationary value increase.
研究了探测场或驱动场失谐情况下开放的Λ型无粒子数反转激光系统中原子响应的时间演化规律,并与探测场和驱动场都共振时的演化规律进行了比较.我们发现失谐对时间演化规律有显著的影响;当驱动场或探测场失谐时,原子对探测场和驱动场色散的响应不再为零,双光子相干不再是纯实量;探测场失谐的变化将使粒子布居和驱动场增益(吸收)的时间演化规律明显改变;随着失谐的增大,探测场增益(吸收)、色散和双光子相干随时间的演化行为逐渐偏离标准阻尼振子的演化规律;驱动场色散驱动场失谐量的增加而振荡时间变长,振幅和稳定值变大.收藏指正
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