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Magnetic phase transitions and monopole excitations in spin ice under uniaxial pressure: A Monte Carlo simulation

机译:单轴压力下自旋冰中的磁相变和单极激发:蒙特卡洛模拟

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摘要

In this work, we explore the spin ice model under uniaxial pressure using the Monte Carlo simulation method. For the known spin ices, the interaction correction (δ) introduced by the uniaxial pressure varies in quite a wide range from positive to negative. When δ is positive, the ground state characterized by the ferromagnetic spin chains is quite unstable, and in real materials it serves as intermediate state connecting the ice state and the long range ordered dipolar spin ice ground state. In the case of negative δ, the system relaxes from highly degenerate ice state to ordered ferromagnetic state via a first order phase transition. Furthermore, the domain walls in such ferromagnetic state are the hotbed of the excitations of magnetic monopoles, thus indicating that the uniaxial pressure can greatly increase the monopole density.
机译:在这项工作中,我们使用蒙特卡洛模拟方法探索单轴压力下的自旋冰模型。对于已知的旋转冰,由单轴压力引入的相互作用校正(δ)在从正到负的很大范围内变化。当δ为正时,以铁磁自旋链为特征的基态非常不稳定,在实际材料中,它充当连接冰态和长程有序偶极自旋冰基态的中间态。在负δ的情况下,系统会通过一阶相变从高度退化的冰态松弛到有序的铁磁态。此外,处于这种铁磁状态的畴壁是磁性单极子激发的温床,因此表明单轴压力可以极大地增加单极子密度。

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