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磁极化
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  magnetic polarization
     Clinical study on treatment of the risk factors of disease in old patients by the blood balance therapy with the magnetic polarization and the absorption of cooling and solidifying ion
     磁极化生物平衡离子吸附疗法治疗老年人心脑血管病危险因素的临床研究
短句来源
     Magnetic Polarization Currents of Submicroscopic Circuit in Parallel-coupled Double Quantum Dots Devices
     嵌入并联耦合量子点的介观环路的磁极化传输电流
短句来源
     The interaction proved between electric polarization and magnetic polarization of sources can strengthen electric field intensity when EM waves propagate in earth with chiral media.
     通过引入手征(注)(Chiral)媒质中电磁场的本构方程(亦称物性方程),证明了电磁波在地中传播时,源电极化和源磁极化之间存在耦合关系,这种耦合作用的结果总是程度不同地增强了电场强度,而对磁场强度的影响则较复杂。
短句来源
     Objective In this paper we discussed the clinical effect on treatment of the risk factors relating to the old aged patients with cardiovascular and cerebrovascular disease with the blood balance therapy with the magnetic polarization and the absorption of cooling and solidifying ion.
     目的 探讨磁极化生物平衡离子吸附降脂降粘疗法(也称之为洗血疗法)对老年心脑血管病危险因素的临床疗效。
短句来源
     We theoretically study the properties of the magnetic polarization currents (MPC) in parallel-coupled double-quantum-dot devices by means of the two-impurity Anderson Hamiltonian and Green functions.
     利用格林函数并借助于双杂质Anderson模型的哈密顿量,研究了嵌入平行耦合量子点的非平衡介观环路的磁极化电流性质.
短句来源
  magnetic quantum
     Clinical study on the effect of magnetic quantum blood balance treatment in treating hyperlipaemia and high viscosity of blood
     磁极化冷凝离子吸附血液平衡疗法降脂降粘效果的临床研究
短句来源
     [Objective]To study the clinical curative effect of magnetic quantum blood balance treatment in treating hyperlipaemia and high viscosity of blood.
     目的探讨磁极化冷凝离子吸附血液平衡疗法治疗心脑血管病危害因素的临床疗效。
短句来源
     [Conclusion]Magnetic quantum blood balance treatment is effective in treating hyperlipaemia and high viscosity of blood. It is an effective method to treat cardio - cerebrovascular disease.
     结论 磁极化冷凝离子吸附血液平衡疗法治疗高脂血症、高粘血症是有效的,是治疗预防心脑血管疾病的有效方法。
短句来源
  “磁极化”译为未确定词的双语例句
     For horizontally polarized waves, however, both the real and imaginary parts of the magnetic susceptibility, in a typical example, is about 10-4 and the imaginary part of electric susceptibility is about 10-3 and the real part of that is about 0.05.
     然而,对于水平极化波,其磁极化系数的实部和虚部,在一典型实例下,均约为10~(-4),而其电极化系数的虚部约为10~(-3),实部约为0.05。
短句来源
     Application and Reflection of Holistic Nursing to Blood Magnetizing Therapy
     整体护理在血液磁极化治疗中的应用
短句来源
     With the help of the theory of electromagnetic field and the torque equations of antiferromagnet, the relation between energy density and frequeney has been studied, and the strength functions of bulk polariton in the voigt configuration are presented.
     本文用电磁场理论和反铁磁体的转矩方程组研究了这两部分能量的能量密度与频率的关系,并给出在Voigt位形下体磁极化液元的强度函数。
短句来源
     Effective Mass of the Surface Magnetopolaron in Polar Crystals at a Finite Temperature
     有限温度下极性晶体中表面磁极化的有效质量
短句来源
     DIAGRAMMATIZED METHOD UNIFIED MODELAND ANALYZING OF THE PERMANENT MAGNET’S WORKING POINT IN THE POLARIZED MAGNETIC SYSTEM WITH SINGLE PERMANENT MAGNET
     单永磁极化磁系统的永磁工作点图解法统一模型与分析
短句来源
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  magnetic polarization
Over the years, there were several independent suggestions that the dominant source of pulsar magnetism is either the field-induced or the spontaneous magnetic polarization of the baryon material.
      
The magnetic polarization of ionic states, which spontaneously arises at the phase transition point, acts as an order parameter in displacive magnetic phase transitions.
      
For hydrogen-saturated hydrides with a high chromium concentration, the calculations predict magnetic polarization at chromium atoms with a magnetic moment of up to 2μB.
      
We prove the global uniqueness results in both cases of the transverse electric polarization and the transverse magnetic polarization within the class of rectangular periodic structures by a single choice of any wave number.
      
They are preferable for the emergence of the magnetic polarization (the Hundtendency).
      
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  magnetic quantum
The magnetoexciton effective mass in states with magnetic quantum number m=0 monotonically increases with H and D, while in states with m≠0 it is a nonmonotonic function of D/l.
      
We derive analytical expressions for third-order matrix elements in the spherical states |nlm? with fixed principal quantum number n and magnetic quantum number m.
      
The theory is based on expanding in powers of the field strength the eigenfunctions and eigenvalues of the matrix of diamagnetic interaction in the subspace of states with given principal and magnetic quantum numbers.
      
We consider states of the hydrogen atom with the principal quantum number n≤3 and zero magnetic quantum number in a constant homogeneous magnetic field ?.
      
It is shown that instead of selection rules for the magnetic quantum number, the interaction in this basis can be presented as the sum of direct transitions between corresponding pairs of polarization-dressed states of the upper and lower levels.
      
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When an electromagnetic wave propagates in an antiferromagnet, it will interact will the magnona of the antiferromagnet and form bulk magnetic polariton in the antiferromagnet. The energy associated with the polariton consists of two parts: One portion is the energy associated with the electromagnetic field and another portion is the energy accoeiated with the excited magnons. With the help of the theory of electromagnetic field and the torque equations of antiferromagnet, the relation between energy density...

When an electromagnetic wave propagates in an antiferromagnet, it will interact will the magnona of the antiferromagnet and form bulk magnetic polariton in the antiferromagnet. The energy associated with the polariton consists of two parts: One portion is the energy associated with the electromagnetic field and another portion is the energy accoeiated with the excited magnons. With the help of the theory of electromagnetic field and the torque equations of antiferromagnet, the relation between energy density and frequeney has been studied, and the strength functions of bulk polariton in the voigt configuration are presented.

当电磁波在反铁磁体中传播时,它将与反铁磁的磁振子相互作用而形成体磁极化激元。与体磁极化激元相联系的能量一部分存在于电磁场中,一部分存在于激发的磁振子中。本文用电磁场理论和反铁磁体的转矩方程组研究了这两部分能量的能量密度与频率的关系,并给出在Voigt位形下体磁极化液元的强度函数。

The general formula of the energy density associated with the bulk magnetic polaritons in uniaxial crystals is deduced from electromagnetic theory, the known results from the theory of lattical dynamics are included in this formula as Special examples. For an uniaxial ferromagnet the strength functions of the bulk magnetic polaritons are given both in Voigt configuration and Faraday configuration, and the experimental method is suggested to probe the magneticpolaritons.

本文从电磁场理论出发,导出了计算体磁极化激元的能量密度的一般公式,此式包括了已知的由点阵动力学导出的一些结果。对单轴铁磁体,计算了在Voigt位形和Faraday位形下的磁极化激元的强度函数,并由此建议了探测这种体磁极化激元的方法。

The effective constitutive parameters of forests at high frequency range is analyzed. It is found that because of the occurence of resonance at high frequency range in tree trunks, magnetic energy can be stored and the effective permeability of the tree trunks needs not be determined conventionally to be unity. For vertically polarized waves, the effective permeability is found to be not significantly different from unity. For horizontally polarized waves, however, both the real and imaginary parts of the magnetic...

The effective constitutive parameters of forests at high frequency range is analyzed. It is found that because of the occurence of resonance at high frequency range in tree trunks, magnetic energy can be stored and the effective permeability of the tree trunks needs not be determined conventionally to be unity. For vertically polarized waves, the effective permeability is found to be not significantly different from unity. For horizontally polarized waves, however, both the real and imaginary parts of the magnetic susceptibility, in a typical example, is about 10-4 and the imaginary part of electric susceptibility is about 10-3 and the real part of that is about 0.05.

本文分析了森林的高频有效导磁率和有效介电常数。由于在高频下,树干中要发生谐振并存储磁能,因而树干的有效导磁率不应像传统的那样定为1。对于垂直极化波而言,其有效导磁率与1相差不多;然而,对于水平极化波,其磁极化系数的实部和虚部,在一典型实例下,均约为10~(-4),而其电极化系数的虚部约为10~(-3),实部约为0.05。

 
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