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首页> 外文期刊>Journal of Superconductivity and Novel Magnetism >The Splitting of SDW State into Commensurable and Incommensurables Ones and the Peculiarities of the Behavior of Thermodynamic Quantities in a Magnetic Field Arbitrarily Oriented to Magnetization in Quasi Two-Dimensional Systems
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The Splitting of SDW State into Commensurable and Incommensurables Ones and the Peculiarities of the Behavior of Thermodynamic Quantities in a Magnetic Field Arbitrarily Oriented to Magnetization in Quasi Two-Dimensional Systems

机译:准二维系统中任意定向磁化的磁场中SDW状态分为可比较和不可比较的状态以及热力学量行为的特殊性

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The quasi-two-dimensional system in which magnetism is caused by spin density wave (SDW) with an anisotropic energy spectrum (with defined impurity concentration x) is examined. The wave vector Q is supposed to be different from 2k_F and the umklapp scattering (U-processes) is taken into account. The system is placed in a magnetic field arbitrarily oriented with respect to the vector M_Q. The basic equations for order parameters M_Q~z, M'_Q, M_z, M~σ are obtained and the system of these equations is transformed taking into account the U-processes. The particular cases (H‖M_Q) and (H⊥M_Q) and the case of small arbitrarily oriented magnetic fields H are examined in detail. The conditions of the system transition to commensurable and incommensurable SDW state are analyzed. The phase diagram (T, x) at H = 0 is traced. The influence of the magnetic field H on the temperature of magnetic transition is researched and the aspect of the phase diagram in magnetic field in the cases H~z H~σ = 0 is presented. The longitudinal magnetic susceptibility X‖ which demonstrates that at x < x_c the temperature behavior is similar to the case when the system has a gap, and at x > x_c to a gapless case. At x ~ x_c in the dependence X_(‖)(T) a local maximum appears. The influence of the energy spectrum anisotropy on the system's properties is researched. Also the angular anisotropy of the quantity χ‖ at different values of T and x is determined.
机译:研究了准二维系统,其中由具有各向异性能谱(定义为杂质浓度x)的自旋密度波(SDW)引起磁性。假设波矢量Q与2k_F不同,并且考虑了umklapp散射(U过程)。该系统被放置在相对于矢量M_Q任意定向的磁场中。获得了阶数参数M_Q〜z,M'_Q,M_z,M〜σ的基本方程,并考虑了U过程对这些方程的系统进行了变换。详细研究了(H‖M_Q)和(H⊥M_Q)的特殊情况以及任意定向的小磁场H的情况。分析了系统过渡到可比较和不可比较的SDW状态的条件。追踪H = 0时的相位图(T,x)。研究了磁场H对磁转变温度的影响,给出了H〜z H〜σ= 0时磁场中相图的变化。纵向磁化率X”表明,在x x_c时,温度行为与无间隙情况相似。在依赖关系X_(‖)(T)处的x〜x_c处,出现局部最大值。研究了能谱各向异性对系统性能的影响。还确定了在不同的T和x值下量χ′的角度各向异性。

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