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首页> 外文期刊>Journal of Experimental and Theoretical Physics >Commensurate and incommensurate states of a spin density wave in a quasi-two-dimensional system with an anisotropic energy spectrum in an external magnetic field of arbitrary direction relative to magnetization
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Commensurate and incommensurate states of a spin density wave in a quasi-two-dimensional system with an anisotropic energy spectrum in an external magnetic field of arbitrary direction relative to magnetization

机译:准二维系统中自旋密度波的相称和不相称状态,其各向异性能谱在相对于磁化方向为任意方向的外部磁场中

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A theory of thermodynamic properties of a spin density wave (SDW) in a quasi-two-dimensional system (with a preset impurity concentration x) is constructed. We choose an anisotropic dispersion relation for the electron energy and assume that external magnetic field H has an arbitrary direction relative to magnetic moment M _Q. The system of equations defining order parameters M _Q ~z, M _Q ~σ, M _z, and M ~σ is constructed and transformed with allowance for the Umklapp processes. Special cases when H a?- M Q and H a?¥ M _Q (H _Z H ~σ = 0) are considered in detail as well as cases of weak fields H of arbitrary direction. The condition for the transition of the system to the commensurate and incommensurate states of the SDW is analyzed. The concentration dependence of magnetic transition temperature T M is calculated, and the components of the order parameter for the incommensurate phase are determined. The phase diagram (T,~x) is constructed. The effect of the magnetic field on magnetic transition temperature T _M is analyzed for H _Z H ~σ = 0, and longitudinal magnetic susceptibility χa?- is calculated; this quantity demonstrates the temperature dependence corresponding to a system with a gap for x < x c and to a gapless state for x > x c. In the immediate vicinity of the critical impurity concentration (x ~ x _c), the temperature dependence of the magnetic susceptibility acquires a local maximum. The effect of anisotropy of the electron energy spectrum on the investigated physical quantities is also analyzed.
机译:构造了准二维系统(预设杂质浓度x)中自旋密度波(SDW)的热力学性质的理论。我们为电子能量选择各向异性色散关系,并假设外部磁场H相对于磁矩M _Q具有任意方向。构造并定义了阶次参数M_Q〜z,M_Q〜σ,M_z和M〜σ的方程组,并在考虑到Umklapp过程的情况下进行了转换。详细考虑了H a?-M Q和H a?¥ M _Q(H _Z H〜σ= 0)的特殊情况,以及任意方向的弱场H的情况。分析了系统向SDW的相称和相称状态过渡的条件。计算出磁性转变温度T M的浓度依赖性,并确定不相称相的有序参数的分量。构造了相位图(T,〜x)。在H _Z H〜σ= 0的情况下,分析了磁场对磁转变温度T _M的影响,并计算了纵向磁化率χa?-。该量证明了温度依赖性,该温度依赖性对应于一个对于x x c而言具有无间隙状态的系统。在临界杂质浓度(x〜x _c)的附近,磁化率的温度依赖性获得局部最大值。还分析了电子能谱各向异性对研究的物理量的影响。

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