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Ferrimagnetism of the Heisenberg Models on the Quasi-One-Dimensional Kagome Strip Lattices

机译:准一维空间上海森堡模型的亚铁磁性   Kagome strip格子

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摘要

We study the ground-state properties of the S=1/2 Heisenberg models on thequasi-onedimensional kagome strip lattices by the exact diagonalization anddensity matrix renormalization group methods. The models with two differentstrip widths share the same lattice structure in their inner part with thespatially anisotropic two-dimensional kagome lattice. When there is no magneticfrustration, the well-known Lieb-Mattis ferrimagnetic state is realized in bothmodels. When the strength of magnetic frustration is increased, on the otherhand, the Lieb-Mattis-type ferrimagnetism is collapsed. We find that thereexists a non-Lieb-Mattis ferrimagnetic state between the Lieb-Mattisferrimagnetic state and the nonmagnetic ground state. The local magnetizationclearly shows an incommensurate modulation with long-distance periodicity inthe non-Lieb-Mattis ferrimagnetic state. The intermediate non-Lieb-Mattisferrimagnetic state occurs irrespective of strip width, which suggests that theintermediate phase of the two-dimensional kagome lattice is also thenon-Lieb-Mattis-type ferrimagnetism.
机译:通过精确的对角化和密度矩阵重归一化群方法,研究了准一维Kagome带状晶格上S = 1/2 Heisenberg模型的基态性质。具有两个不同条带宽度的模型在其内部与空间各向异性二维kagome晶格共享相同的晶格结构。当没有磁阻时,两个模型都实现了众所周知的利勃·马蒂斯亚铁磁态。另一方面,当增加磁阻强度时,利勃-马蒂斯型亚铁磁性崩溃。我们发现在Lieb-Mattisferrimagnetic状态和非磁性基态之间存在非Lieb-Mattis亚铁磁性状态。在非李布-马蒂斯亚铁磁态中,局部磁化清楚地显示出具有远距离周期性的不相称的调制。无论带状宽度如何,都发生中间非利勃-马蒂亚铁磁态,这表明二维高戈姆晶格的中间相也是非利勃-马蒂斯型亚铁磁。

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