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首页> 外文期刊>Journal of the Physical Society of Japan >Occurrence of Fermi pockets without pseudogap hypothesis and clarification of the energy distribution curves of angle-resolved photoemission spectroscopy in underdoped cuprate superconductors
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Occurrence of Fermi pockets without pseudogap hypothesis and clarification of the energy distribution curves of angle-resolved photoemission spectroscopy in underdoped cuprate superconductors

机译:不存在假间隙假说的费米腔的发生以及澄清的低价铜酸盐超导体中角分辨光发射光谱的能量分布曲线的澄清

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摘要

Central issues in the electronic structure of underdoped cuprate superconductors are to clarify the shape of the Fermi surfaces and the origin of the pseudogap. On the basis of the model proposed by Kamimura and Suwa, which bears important features originating from the interplay of Jahn-Teller physics and Mott physics, the feature of Fermi surfaces in underdoped cuprates is the presence of Fermi pockets constructed from doped holes under the coexistence of a metallic state and a local antiferromagnetic order. Below Tc, the holes on Fermi pockets form Cooper pairs with d-wave symmetry in the nodal region. In the antinodal region, there are no Fermi surfaces. In this study we calculate the energy distribution curves (EDCs) of angle-resolved photoemission spectroscopy (ARPES) below Tc. It is shown that the feature of ARPES profiles of underdoped cuprates consists of a coherent peak in the nodal region and real transitions of photoexcited electrons from occupied states below the Fermi level to a free-electron state above the vacuum level in the antinodal region, where the latter transitions form a broad hump. From this feature, the origin of the two distinct gaps observed by ARPES is elucidated without introducing the concept of the pseudogap. Finally, a remark is made on the phase diagram of underdoped cuprates.
机译:掺杂不足的铜酸盐超导体的电子结构的中心问题是澄清费米表面的形状和伪间隙的起源。在Kamimura和Suwa提出的模型的基础上,其具有源自Jahn-Teller物理和Mott物理相互作用的重要特征,在掺杂不足的铜酸盐中,费米表面的特征是在共存下存在由掺杂孔构成的费米口袋。金属态和局部反铁磁序在Tc以下,费米腔上的孔在节点区域形成d波对称的库珀对。在反节点区域,没有费米表面。在这项研究中,我们计算了低于Tc的角度分辨光发射光谱(ARPES)的能量分布曲线(EDC)。结果表明,低掺杂铜酸盐的ARPES谱特征由节点区的相干峰和光激发电子从费米能级以下的占据态到真空区的真空能级以上的自由电子态的实际跃迁组成,其中后者的转变形成了一个巨大的驼峰。从这一特征出发,无需引入伪间隙的概念就可以阐明ARPES所观察到的两个不同间隙的起源。最后,在掺杂不足的铜酸盐的相图中作了说明。

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