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单层 La2CuO4 中的自旋激发。

Spin excitations in a single La2CuO4 layer.

机构信息

Department of Condensed Matter Physics and Materials Science, Brookhaven National Laboratory, Upton, New York 11973, USA.

出版信息

Nat Mater. 2012 Oct;11(10):850-4. doi: 10.1038/nmat3409. Epub 2012 Sep 2.

Abstract

Cuprates and other high-temperature superconductors consist of two-dimensional layers that are crucial to their properties. The dynamics of the quantum spins in these layers lie at the heart of the mystery of the cuprates. In bulk cuprates such as La(2)CuO(4), the presence of a weak coupling between the two-dimensional layers stabilizes a three-dimensional magnetic order up to high temperatures. In a truly two-dimensional system however, thermal spin fluctuations melt long-range order at any finite temperature. Here, we measure the spin response of isolated layers of La(2)CuO(4) that are only one-unit-cell-thick. We show that coherent magnetic excitations, magnons, known from the bulk order, persist even in a single layer of La(2)CuO(4), with no evidence for more complex correlations such as resonating valence bond correlations. These magnons are, therefore, well described by spin-wave theory (SWT). On the other hand, we also observe a high-energy magnetic continuum in the isotropic magnetic response that is not well described by two-magnon SWT, or indeed any existing theories.

摘要

铜酸盐和其他高温超导体由二维层组成,这些二维层对其性质至关重要。这些层中量子自旋的动力学是铜酸盐之谜的核心。在块状铜酸盐(如 La(2)CuO(4))中,二维层之间的弱耦合存在会在高温下稳定三维磁有序。然而,在真正的二维系统中,热自旋涨落会在任何有限温度下融化长程有序。在这里,我们测量了只有一个单胞厚的孤立 La(2)CuO(4)层的自旋响应。我们表明,与体有序相关的相干磁激发,磁振子,即使在单层 La(2)CuO(4)中也会持续存在,没有证据表明存在更复杂的关联,如共振价带关联。因此,这些磁振子可以很好地用自旋波理论(SWT)来描述。另一方面,我们也在各向同性磁响应中观察到高能磁连续体,其不能很好地用双磁振子 SWT 或任何现有理论来描述。

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