绝热条件

  • 网络Adiabatic Condition
绝热条件绝热条件
  1. 基于EIT原子体系的量子存储及其绝热条件双模多光子纠缠态与多原子体系的消相干

    Quantum Memory and the Adiabatic Condition Based on Atoms Ensemble with Electromagnetically Induced Transparency ; The Decoherence of the Double-mode Multi-photon Entangled State and the Polyatomic System

  2. 结果发现,在无序存在和绝热条件下,BEC呈现出安德森定域化现象;局域态的中间区域宽度和尾部形状均受非线性空间调制影响。

    The results show that there exists Anderson localization in the presence of disorder and adiabatic condition , It was found that the nonlinear spatial modulation has influence on the central region and the tail of the localized state .

  3. 最小自由能法求解GAP在等压绝热条件下的燃烧产物

    Free-Energy Minimization Investigation on Combustion of GAP Under Constant Pressure and Adiabatic Condition

  4. 近似绝热条件下含酸DNT、TNT热分解过渡到热爆炸的实验研究

    An experimental study of acid-containing dnt , tnt in its transition from thermal decomposition to explosion under close-to-adiabatic conditions

  5. Kondo式估算结果与Jacobs式估算结果在中性条件下约为0.6,在非绝热条件下约为0.7;

    The result shown by Kondo 's formula vs that by Jacobs is about 0.6 under neutral condition , and about 0.7 under diabatic condition .

  6. 总之,螺旋光纤系统方案能自动满足Wang与Matsumoto的核磁共振方案中为实现非绝热条件几何相移所提出的全部条件与要求。

    In a word , the coiled fiber system can automatically satisfy the requirements and conditions , which were proposed by Wang and Matsumoto in order to create the nonadiabatic conditional geometric phase shift in their NMR scheme .

  7. 证明螺旋光纤系统内光子有效哈密顿量恰好是一个WangMatsumoto型哈密顿量,因此螺旋光纤系统能自动产生非绝热条件几何相移。

    It was demonstrated that the effective Hamiltonian that describes the propagation of photon fields inside the coiled fiber is just the Wang Matsumoto type of Hamiltonian . Thus , the coiled fiber system will automatically generate the nonadiabatic conditional geometric phase shift .

  8. 研究了近似绝热条件下含酸DNT、TNT模拟试样及生产现场采集试样从热分解过渡到热爆炸的热行为。

    The thermal action of acid-containing DNT , TNT in the transition from thermal decomposition to explosion was studied in close-to-adiabatic conditions . Two samples were studied , of which one was simulated in the laboratory , the other gathered from the production line .

  9. 螺旋光纤系统中非绝热条件几何相移

    The nonadiabatic conditional geometric phase shift in a coiled fiber system

  10. 量子微腔中暗态原子粒子数转移的绝热条件

    Adiabatic condition of a dark atom on population transfer in a cavity

  11. 然而,绝热条件在许多现实实验中都较难实现。

    But the adiabatic condition is not satisfied in many realistic cases .

  12. 随后对二能级系统的绝热条件提出了自己的见解。

    Subsequently adiabatic condition about two states system is obtained .

  13. 利用相法分析了简单的非绝热条件下的适定性系统的相轨道。

    Phase trajectores of well-posed systems are analysed under simple diabatic conditions .

  14. 超冷异核分子相干产生的绝热条件及量子控制研究

    Adiabatic Condition and Quantum Control for Creating Heteronuclear Molecule

  15. 邮件或货币的处理在近似绝热条件下完成。

    The treatment of either mail or currency is done under nearly adiabatic conditions .

  16. 我们给出了相对简明、方便的绝热条件,并且用这个绝热条件计算了一些例子。

    We also give concise and convenient adiabatic conditions and calculate some examples with this adiabatic conditions .

  17. 研究了输送管壁不同绝热条件、贮箱增压及气体引射对自然循环预冷过程的影响。

    The effects of different insulation , tank pressure and injection situations on the precooling process were investigated .

  18. 探讨了绝热条件下光子回波技术对量子信息存储和信息提取的动态过程。

    The dynamic process for the quantum information storage and that of the recall with the photon echo is discussed under adiabatic condition .

  19. 使用该设备,在绝热条件下记录电池内的温度、压力及自放热速率和时间的函数关系。

    ARC is used to record battery internal temperature , pressure and function relationship between self-discharge thermal rate and time under adiabatic condition .

  20. 在慢扫描(即绝热条件)和快扫描条件下,没有遂穿现象发生。

    In the adiabatic ( i.e. , slowly sweeping ) and sudden ( i.e. , fast sweeping ) limits , no tunneling is observed .

  21. 在绝热条件下,光场与系统作用过程中粒子的绝热状态随态和位相走势的不同而变化。

    During the interaction between field and system , the adiabatic states of particles are variant with the different circumstances of light field phase under the adiabatic condition .

  22. 考虑磁扩散率为温度的函数以及绝热条件,线性扰动磁流力学方程组的色散方程是频率的三次方程。

    The dispersion equation of linear disturbance magnetohydrodynamics equations ' is an algebraic equation of third power of frequency when the magnetic diffusivity is considered as a function of temperature .

  23. 通过对利用自然冷源单管制冰过程的传热分析,建立了管制冰的一维传热模型,在蓄冰池围护为绝热条件下,用积分法对一维模型进行了求解;

    Based on the analyzing and studying one pipe freezing ice process utilizing natural coldness resource ( NCR ), the one dimensional heat transfer model is developed and solved using integral method .

  24. 本文采用加速量热仪与电池充放电循环系统联用的技术,对锂离子电池在绝热条件下的循环产热特性进行了分析。

    In this paper , an Accelerating Rate Calorimeter combined with battery charging and discharging cycler was employed to study the heat release mechanism of a lithium ion battery during cycling under adiabatic condition .

  25. 利用分段线性函数,构建出燃烧器内的温度分布曲线、贫可燃极限和最大半周期。该解适用于绝热条件下往复式惰性多孔介质燃烧器。

    The temperature profiles in the burner , the lean flammable limit and maximum half cycle are predicted by a piecewise linear function , which is applied to inert porous medium combustors with reciprocating flow in the absence of heat loss to the surroundings .

  26. 从紧束缚Hamiltonian模型出发,在反绝热极限条件下,对费米子无自旋态MX链系统进行了研究。

    Based on the tight-binding Hamiltonian model , the anti-adiabatic limit of MX chain in spinless case is studied .

  27. 实验纪录了不同的管路结构及不同绝热结构条件下,管路出现的振动信号及管路温度分布,并将实验结果与Murphy曲线进行了对比。

    The vibration and temperature distribution ware recorded in different pipe structure and insulation conditions . The results of experiment were compared with the Murphy 's result .

  28. 用一维绝热边界条件热模型计算热饱和阈值。

    By employing one dimension non-conducting boundary condition , the thermal saturation threshold hasbeen calculated .

  29. 二能级系统的绝热近似条件

    Adiabatic Condition of Two States System

  30. 在绝热近似条件下,采用传递矩阵方法计算了电子和空穴的能谱。

    The energy spectrum of the electron and hole is calculated using the transfer matrix formalism in the adiabatic approximation .