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Bosonic Spectral Function and the Electron-Phonon Interaction in HTSC Cuprates

机译:HTSC铜酸盐中的波谱函数和电子-声子相互作用

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In this paper we discuss experimental evidence related to thestructure and origin of the bosonic spectral functionα2F(ω)in high-temperature superconducting (HTSC) cuprates atand near optimal doping. Global properties ofα2F(ω), such as number and positions of peaks, are extractedby combining optics, neutron scattering, ARPES and tunnellingmeasurements. These methods give evidence for strongelectron-phonon interaction (EPI) with1<λep≲3.5in cuprates near optimal doping. We clarify how theseresults are in favor of the modified Migdal-Eliashberg (ME) theoryfor HTSC cuprates near optimal doping. In Section 2 we discusstheoretical ingredients—such as strong EPI, strongcorrelations—which are necessary to explain the mechanism ofd-wave pairing in optimally doped cuprates. These comprise the MEtheory for EPI in strongly correlated systems which give rise tothe forward scattering peak. The latter is supported by thelong-range part of EPI due to the weakly screened Madelunginteraction in the ionic-metallic structure of layered HTSCcuprates. In this approach EPI is responsible for the strength ofpairing while the residual Coulomb interaction and spinfluctuations trigger the d-wave pairing.
机译:在本文中,我们讨论了与高温超导(HTSC)铜酸盐中及最佳掺杂附近的玻色子光谱函数α2F(ω)的结构和起源有关的实验证据。通过结合光学,中子散射,ARPES和隧穿测量来提取α2F(ω)的全局特性,例如峰的数量和位置。这些方法为在接近最佳掺杂的铜酸盐中1 <λep≲3.5的强电子-声子相互作用(EPI)提供了证据。我们阐明了这些结果如何支持改良的Migdal-Eliashberg(ME)理论,用于接近最佳掺杂的HTSC铜酸盐。在第2节中,我们讨论了理论成分(例如强EPI,强相关性),这对于解释最佳掺杂的铜酸盐中d波配对的机理是必要的。这些构成了在强相关系统中EPI的ME理论,从而产生了前向散射峰。后者由EPI的远距离部分支持,这是由于层状HTSC杯状离子的离子-金属结构中的弱筛选的马德隆相互作用。在这种方法中,EPI负责配对的强度,而剩余的库仑相互作用和自旋涨落则触发d波配对。

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