0 (correspond'/> Spectral function of one hole in several one-dimensional spin arrangements
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Spectral function of one hole in several one-dimensional spin arrangements

机译:几个一维自旋排列中一个孔的光谱函数

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The spectral function of one hole in different magnetic states of the one-dimensional t-J model including three-site term and frustration J' is studied. In the strong-coupling limit J-->0 (corresponding to U-->infinity of the Hubbard model) a set of eigenoperators of the Liouvillian is found which allows us to derive an exact expression for the one-particle Green's function that is also applicable at finite temperature and in an arbitrary magnetic state. The spinon dispersion of the pure t-J model with the ground state of the Heisenberg model can be obtained by treating the corrections due to a small exchange term by means of the projection method. The spectral function for the special frustration J' = J/2 with the Majumdar-Ghosh wave function is discussed in detail. Besides the projection method, a variational ansatz with the set of eigenoperators of the t term is used. We find a symmetric spinon dispersion around the momentum k = pi/(2a) and a strong damping of the holon branch Below the continuum a bound state is obtained with finite spectral weight and a very small separation from the continuum. Furthermore, the spectral function of the ideal paramagnetic case at a temperature k(B)T much greater thanJ is discussed. [References: 26]
机译:研究了一维t-J模型在不同磁性状态下一个孔的谱函数,该模型包括三点项和无奈J'。在强耦合极限J-> 0(对应于Hubbard模型的U->无穷大)中,发现了Liouvillian的一组本征算子,这使我们可以得出一个单粒子格林函数的精确表达式,即也适用于有限温度和任意磁性状态。可以通过投影方法处理由于交换项较小而引起的修正,从而获得具有海森堡模型基态的纯t-J模型的旋子色散。详细讨论了带有Majumdar-Ghosh波函数的特殊挫折J'= J / 2的谱函数。除投影方法外,还使用带有t项本征算子集的变分ansatz。我们发现动量k = pi /(2a)周围有对称的旋子色散,并且霍隆分支具有很强的阻尼作用。在连续体下,获得的束缚态具有有限的光谱权重,并且与连续体的间距很小。此外,讨论了在比k大得多的温度k(B)T时理想顺磁情况的频谱函数。 [参考:26]

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