期刊文献+

铜氧化物超导体两能隙问题的电子拉曼散射理论研究 被引量:1

Theoretical research on two gaps in cuprate superconductors: an electronic Raman scattering study
原文传递
导出
摘要 电子拉曼实验表明在空穴型掺杂的铜氧化物超导体中存在两能隙行为,即在欠掺杂区,随着掺杂浓度的降低,一个能隙逐渐增大而且在超导转变温度以上仍然存在,而另一个能隙逐渐减小且在DDW态依然存在.解释两能隙行为非常重要因为它与赝能隙的机理密切相关.本文计算了超导序和d-density-wave(DDW)序竞争机理下相图上不同区域的电子拉曼谱,发现欠掺杂区能隙表现出两能隙行为,与实验一致.特别地,本文发现B1g峰对应能量由超导和DDW序共同决定,且随着掺杂浓度的降低而增大,在DDW态依然存在.而B2g峰只对超导序敏感,所以在正常态消失(即使存在DDW序).B1g和B2g两个通道拉曼峰与掺杂浓度和温度的依赖关系也与最近的实验相符.这些结果对赝能隙的竞争序机理是一个有力的支持. Electronic Raman experiments have shown the presence of two types of gaps in hole-doped cuprate superconductors: one is the gap that increases with underdoping and survives in the pseudogap normal state and the other is the gap that traces the superconducting dome and disappears above the transition temperature. This two-gap behavior is important in that it is related to the mechanism of the pseudogap. By calculating the electronic Raman spectra we show that this behavior is consistent with the picture in which the d-wave superconducting (SC) order and d-density-wave (DDW) order compete in the phase diagram. In particular,the energy of the B1g peak is determined by both the SC and the DDW orders, increases with underdoping and survives in the DDW normal state. On the other hand,the B2g peak is shown to be sensitive to the SC order alone,and thus vanishes in the normal state (even if in the presence of the DDW order). The doping dependence and the temperature dependence of the peak energies in the two channels accord nicely with recent experimental results,which strongly supports the competing-order point of view for the superconducting and pseudogap phases.
出处 《物理学报》 SCIE EI CAS CSCD 北大核心 2011年第3期640-646,共7页 Acta Physica Sinica
基金 国家自然科学基金(批准号:10974086 60806015) 南京固体微结构国家实验室开放基金(批准号:M22010) 安徽省教育厅自然科学基金(批准号:KJ2010B184)资助的课题~~
关键词 两能隙 电子拉曼散射 竞争序 two gaps electronic Raman scattering competing order
  • 相关文献

参考文献1

二级参考文献3

同被引文献12

  • 1BEDNORZ J G, MOLLER K A. Possible high T superconductivity in the Ba-La-Cu-O system [J]. Z Phys B, 1986, 64(2): 189-193.
  • 2XIAO Gang, CIEPLAK M Z, XIAO J Q, et al. Magnetic pair-breaking effects: moment formation and critical doping level in superconducting Lal.ssSr0.1sCu-,AO4 systems (A=Fe, Co, Ni, Zn, Ga, A1) [J]. Phys Rev B, 1990, 42(13)= 8752-8755.
  • 3XU Jingtao, TAN Shun, PI Li, et al. Coexistence and competition between superconductivity and magnetism in La2 SrCu.9M.60(M=Mnand Ru) [J]. J Appl Phys, 2008, 104(6): 063914:1 10.
  • 4WANG Caixia, HUANG Qibing, CHEN Xiaobing. The suppression of superconductivity by the localization of oxygen holes in the double-doped La.ss 1.5, Sr0.15+l.,Cul Mn.O4 system [J]. Phys C, 2011, 471(17): 528- 532.
  • 5WANG Caixia, SUN Yuping, QU Zhe, et al. Suppression of superconductivity by the localization of hole carri- ers inTi-doped Lal. ssSr0.sCuO4 [J]. Phys RevB, 2006, 73(14): 144518: 1-9.
  • 6WILES D B, YOUNG R A. A new computer program for Rietveld analysis of X-ray powder diffraction patterns f-J]. J ApplCryst, 1981, 14(2): 149-151.
  • 7WANG Caixia, CHEN Xiaobin, ZHU Aiping. Thermopower and transport mechanism of the La2-. Sr Cu0.94 T i0.06 04 system [J]. Solid StateCommun, 2012, 152(12): 1067-1071.
  • 8XU Jingtao, QU Zhe, TAN Shun, et al. Different carrier compensation effect in La2- SrCuo. 94 Zno.o6 04 and La2- Sr.Cu0.94Nio. 0604 samples [J]. J Appl Phys, 2009, 105(8) : 083913 : 1-5.
  • 9BRUN T, GRIMSDITCH M, GRAY K E, et al. Phonon dispersion curves for Lal.ssSro. lsCuO4 [J]. Phys Rev B, 1987, 35(16): 8837-8839.
  • 10OHANA I, DRESSELHAUS M S, LIU Y C, et al. Raman study of pure and doped (Li, Sr) single crystals of La2CuO4 [J]. PhysRevB, 1989, 39(4): 2293-2298.

引证文献1

二级引证文献1

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部