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arXiv 1502.05684cond-mat.mes-hallcond-mat.str-el
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具有奇数耦合自旋的反铁磁分子纳米磁体

Antiferromagnetic molecular nanomagnets with odd-numbered coupled spins

S. A. Owerre, J. Nsofini

摘要:

近年来,环状分子纳米磁体的研究引起了研究者的广泛关注。这些磁铁的大小是有限的,包含非常大的自旋。它们是有趣的,因为它们具有Néel矢量的宏观量子隧穿。对于具有有限个偶数耦合自旋的反铁磁分子纳米磁体,隧穿涉及由磁能垒分隔的两个经典局域Néel基态。问题是:在具有奇数个磁性离子的纳米磁体中是否可以观察到这种现象?答案并不直接明显,因为具有奇数耦合自旋的循环链是失败的,因为人们无法获得完美的Néel顺序。这些受抑自旋确实可以在实验中观察到,所以它们很有趣。在这封信中,我们从理论上研究了在沿磁体平面施加磁场的情况下,具有任意自旋$s$的奇自旋系统中的宏观量子隧穿。与偶自旋耦合系统相比,奇自旋循环系统的基态由于自旋阻挫而包含一个拓扑孤子。因此,经典基态是$2N$ -折叠简并的,因为孤子可以被放置在沿着环的任何地方,总$S_z=\pm s$。小的量子涨落使孤子离域,形成能带。我们用简并微扰理论在$2s$阶得到了这个能带。我们证明了孤子基态对于半奇数自旋是手征的,对于整数自旋是非手征的。从能带结构中我们推断,随着自旋值的增加,极化中子非弹性散射强度随哈密顿量参数的强弱而增大或减小。

英文摘要:

In recent years, studies on cyclic molecular nanomagnets have captivated the attention of researchers. These magnets are finite in size and contain very large spins. They are interesting because they possess macroscopic quantum tunneling of Néel vectors. For antiferromagnetic molecular nanomagnets with finite number of even-numbered coupled spins, tunneling involves two classical localized Néel ground states separated by a magnetic energy barrier. The question is: can such phenomena be observed in nano magnets with odd number of magnetic ions? The answer is not directly obvious because cyclic chains with odd-numbered coupled spins are frustrated as one cannot obtain a perfect Néel order. These frustrated spins can indeed be observed experimentally, so they are of interest. In this Letter, we theoretically investigate macroscopic quantum tunneling in these odd spin systems with arbitrary spins $s$, in the presence of a magnetic field applied along the plane of the magnet. In contrast to systems with an even-numbered coupled spins, the ground state of the cyclic odd-spin system contains a topological soliton due to spin frustration. Thus the classical ground state is $2N$-fold degenerate as the soliton can be placed anywhere along the ring with total $S_z=\pm s$. Small quantum fluctuations delocalize the soliton with a formation of an energy band. We obtain this energy band using degenerate perturbation theory at order $2s$. We show that the soliton ground state is chiral for half-odd integer spins and non-chiral for integer spins. From the structure of the energy band we infer that as the value of the spin increases the inelastic polarized neutron-scattering intensity may increase or decrease depending on the strengths of the parameters of the Hamiltonian.

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