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Master Equations for pulsed magnetic fields: Application to magnetic molecules

机译:脉冲磁场的主方程:应用于磁场   分子

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摘要

We extend spin-lattice relaxation theory to incorporate the use of pulsedmagnetic fields for probing the hysteresis effects and magnetization steps andplateaus exhibited, at low temperatures, by the dynamical magnetization ofmagnetic molecules. The main assumption made is that the lattice degrees offreedom equilibrate in times much shorter than both the experimental time scale(determined by the sweep rate) and the typical spin-lattice relaxation time. Wefirst consider the isotropic case (a magnetic molecule with a ground state ofspin $S$ well separated from the excited levels and also the general isotropicHeisenberg Hamiltonian where all energy levels are relevant) and then weinclude small off-diagonal terms in the spin Hamiltonian to take into accountthe Landau-Zener-St\"{u}ckelberg (LZS) effect. In the first case, and for an$S=1/2$ magnetic molecule we arrive at the generalized Bloch equation recentlyused for the magnetic molecule \{V$_6$\} in Phys. Rev. Lett. 94, 147204 (2005).An analogous equation is derived for the magnetization, at low temperatures, ofantiferromagnetic ring systems. The LZS effect is discussed for magneticmolecules with a low spin ground state, for which we arrive at a veryconvenient set of equations that take into account the combined effects of LZSand thermal transitions. In particular, these equations explain the deviationfrom exact magnetization reversal at $B\approx 0$ observed in \{V$_6$\}. Theyalso account for the small magnetization plateaus (``magnetic Foehn effect''),following the LZS steps, that have been observed in several magnetic molecules.Finally, we discuss the role of the Phonon Bottleneck effect at lowtemperatures and specifically we indicate how this can give rise to apronounced Foehn effect.
机译:我们扩展了自旋晶格弛豫理论,以结合脉冲磁场的使用来探测磁滞效应以及在低温下通过磁性分子的动态磁化表现出的磁化步骤和平稳期。做出的主要假设是,晶格自由度的平衡时间要比实验时间标度(由扫描速率确定)和典型的自旋晶格弛豫时间短得多。我们首先考虑各向同性的情况(一个自旋的$ S $基态的磁性分子与受激能级以及与所有能级有关的一般各向同性的海森堡哈密顿),然后在自旋哈密顿量中包括小的非对角项考虑到Landau-Zener-St \“ {u} ckelberg(LZS)效应。在第一种情况下,对于$ S = 1/2 $磁性分子,我们得出了最近用于磁性分子\ {V的广义Bloch方程$ _6 $ \},参见Phys。Rev. Lett。94,147204(2005)。推导了反铁磁环系统在低温下的磁化方程,讨论了低自旋基态的磁分子的LZS效应,为此,我们得出了一组非常方便的方程式,其中考虑了LZS和热跃迁的综合影响,尤其是这些方程式说明了在\ {V $ _6 $ \}中观察到的在$ B \约0 $处的精确磁化反转的偏差。他们也很直到在几个磁性分子中观察到的LZS阶跃之后,才发生小的磁化平稳期(``磁性Foehn效应'')。最后,我们讨论了声子瓶颈效应在低温下的作用,并具体说明了如何实现引起被宣扬的Foehn效应。

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